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BEGIN:VEVENT
SUMMARY:Kit Gallagher (QMUL)
DTSTART:20200228T050000Z
DTEND:20200228T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/1
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/1/">Viable Gauge Choices in Cosmologies with Non-Linear Structures</a>\
 nby Kit Gallagher (QMUL) as part of Cosmology Talks\n\n\nAbstract\n<a href
 ="https://www.youtube.com/watch?v=ZqY54LXC4AQ">Link to Video</a> \n\nRefer
 ence for cosmological perturbation theory: <a href="https://arxiv.org/abs/
 0809.4944">arxiv.org/abs/0809.4944</a>\n\nReference for Post Newtonian The
 ory: <a href="https://www.cambridge.org/core/books/gravity/1F0CF38A59B1E51
 A63C7C3138268BE5D">Gravity\, by Eric Poisson\, Cambridge University Press<
 /a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>\n\n0:00:00 <a href="
 https://youtu.be/ZqY54LXC4AQ">Shaun's introduction</a>\n\n0:01:05 <a href=
 "https://youtu.be/ZqY54LXC4AQ?t=65">Kit's opening comments on the paper</a
 >: compared the differences in the gauge problems in two different approac
 hes to approximating solutions to the Einstein field equations\; cosmologi
 cal perturbation theory (applicable on large scales)\; post-Newtonian grav
 ity (applicable on small scales)\; what the gauge problem is\; paper/book 
 references\;\n\n0:09:12 <a href="https://youtu.be/ZqY54LXC4AQ?t=552">Q&A: 
 Next steps</a>: Issue on large scales - next gen galaxy surveys will requi
 re more realistic theoretical modeling than has been done in the past\; di
 scussion of different approaches\; important precautions\n\n0:15:51 <a hre
 f="https://youtu.be/ZqY54LXC4AQ?t=951">Why the paper's approach was not us
 ed before</a>: using post-Newtonian ideas in cosmology is kind of a new th
 ing to do\n\n0:16:29 <a href="https://youtu.be/ZqY54LXC4AQ?t=989">Two take
 aways from the talk</a>\n\n0:17:37 <a href="https://youtu.be/ZqY54LXC4AQ?t
 =1057">1st slide: Cosmological Perturbation Theory</a>\n\n0:18:56 <a href=
 "https://youtu.be/ZqY54LXC4AQ?t=1136">Conceptual problems</a>: discussion 
 leading to explanation of the gauge problem in cosmological perturbation t
 heory\n\n0:27:11 <a href="https://youtu.be/ZqY54LXC4AQ?t=1631">Post-Newton
 ian gravity</a>: capable of dealing with large density contrasts\, provide
 d...\n\n0:28:16 <a href="https://youtu.be/ZqY54LXC4AQ?t=1696">: the condit
 ions under which a post-Newtonian expansion can be done\; 3 conditions</a>
 \n\n0:31:40 <a href="https://youtu.be/ZqY54LXC4AQ?t=1900">Small velocities
  and weak field lead to...</a>: mathematical consequences\; small time der
 ivatives: equations change structure from wave equations to Poisson equati
 ons\n\n0:40:55 <a href="https://youtu.be/ZqY54LXC4AQ?t=2455">The explicit 
 structure of all the gauge transformations</a>\n\n0:49:17 <a href="https:/
 /youtu.be/ZqY54LXC4AQ?t=2957">Section IV A in paper: Spatially Flat Gauge 
 choice</a>\n\n0:52:13 <a href="https://youtu.be/ZqY54LXC4AQ?t=3133">Sectio
 n IV B in paper: Synchronous Gauge choice</a>\n\n0:52:42 <a href="https://
 youtu.be/ZqY54LXC4AQ?t=3162">Section IV F in paper: N-body Gauge choice</a
 >\n\n0:53:13 <a href="https://youtu.be/ZqY54LXC4AQ?t=3193">Section IV G in
  paper: Longitudinal Gauge choice</a>: important one to look at\n\n0:57:40
  <a href="https://youtu.be/ZqY54LXC4AQ?t=3460">Q&A on the N-body gauge</a>
 \n\n1:00:00 <a href="https://youtu.be/ZqY54LXC4AQ?t=3600">Section V of pap
 er: Newtonian Motion Gauge</a>\n\n1:04:40 <a href="https://youtu.be/ZqY54L
 XC4AQ?t=3880">Discussion on equation 89 in paper</a>\n\n1:07:50 <a href="h
 ttps://youtu.be/ZqY54LXC4AQ?t=4070">Applicability</a>\n\n1:10:32 <a href="
 https://youtu.be/ZqY54LXC4AQ?t=4232">Summary</a>\n\n1:16:17 <a href="https
 ://youtu.be/ZqY54LXC4AQ?t=4577">Q&A: what are two simple things you'd want
  viewers to take away from this talk?</a>\n\n1:17:45 <a href="https://yout
 u.be/ZqY54LXC4AQ?t=4665">Q&A: outside of your own research\, what do you t
 hink is the most interesting thing in cosmology at the moment?</a>\n\nRefe
 rence for cosmological perturbation theory: https://arxiv.org/abs/0809.494
 4\n\nReference for Post Newtonian Theory: https://www.cambridge.org/core/b
 ooks/gravity/1F0CF38A59B1E51A63C7C3138268BE5D\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/1/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Seshadri Nadathur (ICG Institute of Cosmology and Gravitation\, Un
 iversity of Portsmouth)
DTSTART:20200319T050000Z
DTEND:20200319T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/2
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/2/">Voids are powerful\, free and have tantalising insights on H0</a>\n
 by Seshadri Nadathur (ICG Institute of Cosmology and Gravitation\, Univers
 ity of Portsmouth) as part of Cosmology Talks\n\n\nAbstract\nSesh tells us
  how the void-galaxy cross correlation provides information about cosmolog
 y via redshift space distortions and (importantly) the Alcock Paczynski ef
 fect. The information is independent of Baryon Acoustic Oscillations (BAO)
  and improves error bars by up to a factor of four. The combination of voi
 ds and BAO have very interesting insights into the Hubble discrepancy and 
 the late-time acceleration of the Universe.\n\nLink to video of talk: <a h
 ref="https://www.youtube.com/watch?v=UivvhqEuVuo">youtube.com/watch?v=Uivv
 hqEuVuo</a>\n\nThe most relevant papers for this talk: <a href="https://ar
 xiv.org/abs/2001.11044">arxiv.org/abs/2001.11044</a> and <a href="https://
 arxiv.org/abs/1904.01030">arxiv.org/abs/1904.01030</a>\n\n<hr>\n\n<b>Index
  to Key Parts of the Talk:</b>\n\n00:00 <a href="https://youtu.be/UivvhqEu
 Vuo?t=1">Shaun's introduction</a>\n\n00:38 <a href="https://youtu.be/Uivvh
 qEuVuo?t=38">Sesh's opening comments on the paper</a>: BAO and RSD have be
 en studied for decades and applied to basically every spectroscopic galaxy
  survey but the void-galaxy cross-correlation measurement is something tha
 t's pretty new\n\n01:40 <a href="https://youtu.be/UivvhqEuVuo?t=100">Q&A: 
 what are two simple things you'd want viewers to remember about this talk?
 </a>: what a void-galaxy cross-correlation is and why it tells us anything
  about cosmology\; the distribution of galaxies around the center of low d
 ensity void regions is anisotropic\, not symmetric\; details of that aniso
 tropy\; usefulness as another method to measure the current expansion rate
  of the universe\, H0\n\n04:18 <a href="https://youtu.be/UivvhqEuVuo?t=258
 ">Q&A: what was the motivation for this work?</a>: interest in what can be
  done with voids\; by using the void-galaxy cross-correlation\, improvemen
 t can be made in the measurement precision of important quantities like th
 e expansion rate and growth structure of the universe\; can improve the pr
 ecision of such quantities by about a factor of two (equivalent to an incr
 ease in the survey volume without requiring any new data or observation ti
 me)\n\n08:13 <a href="https://youtu.be/UivvhqEuVuo?t=493">First slide: Voi
 d-galaxy basics</a>: the distribution of galaxies around void locations\; 
 anisotropic in redshift space\; not looking at void size but at distortion
  away from sphericity\, plot showing distortion due to galaxy velocities a
 round voids (key segment 11:32 to 13:59)\; second and more interesting and
  important effect (13:59 to 17:00)\n\n17:05 <a href="https://youtu.be/Uivv
 hqEuVuo?t=1025">Correlations in redshift space</a>: 2 sources of anisotrop
 y - RSD (peculiar velocities\, growth rate) and Alcock-Paczynski effect\; 
 why the void-galaxy correlation is a better measurement method than the st
 andard auto-correlation technique\n\n19:57 <a href="https://youtu.be/Uivvh
 qEuVuo?t=1197">Breaking the RSD/AP degeneracy</a>: the quadrupole moment o
 f the void-galaxy correlation function\; Fig. 3 in paper \n\n25:33 <a href
 ="https://youtu.be/UivvhqEuVuo?t=1533">Measuring ξvg in surveys\, 1st sli
 de</a>: various complications that have to be considered but left for a di
 fferent talk\n\n25:54 <a href="https://youtu.be/UivvhqEuVuo?t=1554">Measur
 ing ξvg in surveys\, 2nd slide</a>: simulations testing\; Fig. 7 and 8 (t
 riangle plot showing posterior constraints on parameters of the joint RSD-
 AP model for the void-galaxy cross-correlation) in paper\; the important p
 arameters in Fig. 8 are the AP parameter and the growth rate\, they are no
 t strongly degenerate with each other\; were able to get a 1% measurement 
 of the AP parameter\n\n28:27 <a href="https://youtu.be/UivvhqEuVuo?t=1707"
 >Cosmological implications I</a>: Factor 2x improvement in precision (comp
 ared to BAO + FS\, full shape of the galaxy power spectrum)\; covariance m
 atrix\; about a factor of 4 improvement in Fap\; information that is not a
 vailable from usual 2-pt or 3-pt statistics\n\n32:35 <a href="https://yout
 u.be/UivvhqEuVuo?t=1955">Comparing voids to bispectrum</a>: higher order s
 tatistics than just the galaxy power spectrum  gives more information\; le
 ft panel shows same BOSS data but going from power spectrum to bispectrum\
 ; right panel shows going from power spectrum to power spectrum + voids\; 
 the gain from adding voids far exceeds that from the bispectrum\n\n35:32 <
 a href="https://youtu.be/UivvhqEuVuo?t=2132">Cosmological implications II<
 /a>: direct evidence of acceleration independent of CMB and SN Ia (picked 
 up again at 43:15)\n\n34:47 <a href="https://youtu.be/UivvhqEuVuo?t=2147">
 Cosmological implications III</a>: results from using combinations of BAO\
 , voids\, and Ly-a to determine H0 \n\n43:15 <a href="https://youtu.be/Uiv
 vhqEuVuo?t=2595">Back to Cosmological implications II</a>: > 10σ evidence
  of late-time acceleration (>> SN Ia)\; also direct evidence for DE\n\n47:
 39 <a href="https://youtu.be/UivvhqEuVuo?t=2859">the DE EoS can be constra
 ined better with voids included and is consistent with a cosmological cons
 tant</a>:  Fig. 15 and discussion in paper\n\n48:07 <a href="https://youtu
 .be/UivvhqEuVuo?t=2887">Recap of the take-away messages</a>: very powerful
  method for analyzing data from galaxy surveys\, and it's essentially for 
 free as don't need any new observations and it tightens cosmological const
 raints\; some tantalizing answers on H0 discrepancy\; the strongest late-t
 ime evidence for DE comes from BAO+voids and not supernovae\n\n50:07 <a hr
 ef="https://youtu.be/UivvhqEuVuo?t=3007">Q&A: outside of your own research
 \, what do you think is the most interesting thing in cosmology at the mom
 ent?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/2/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Graham White (TRIUMF)
DTSTART:20200326T050000Z
DTEND:20200326T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/3
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/3/">Light dark matter is an ideal mix of particle and cosmology</a>\nby
  Graham White (TRIUMF) as part of Cosmology Talks\n\n\nAbstract\nGraham te
 lls us how Big Bang Nucleosynthesis (BBN) and the Cosmic Microwave Backgro
 und can be used to constrain the potential existence of particles beyond t
 he Standard Model. \n\nThe focus is on light dark matter (masses less than
  1GeV)\, which escapes direct detection bounds by being too light to kick 
 nucleons hard enough and is most interesting to cosmology because it has p
 recisely the masses relevant in the early universe processes we can "obser
 ve"\, e.g. BBN.\n\nGraham volunteered to give this talk on less than 36 ho
 urs notice\, so huge thanks to him for pulling something together so quick
 ly!!\n\nTalk video: <a href="https://www.youtube.com/watch?v=85sXsaj02yE">
 youtube.com/watch?v=85sXsaj02yE</a>\n\nGraham's paper: <a href="https://ar
 xiv.org/abs/2003.02273">Cosmological Bounds on sub-GeV Dark Vector Bosons 
 from Electromagnetic Energy Injection</a>\n\n<hr>\n\n<b>Index to Key Parts
  of the Talk:</b>\n\n00:00 <a href="https://youtu.be/85sXsaj02yE?t=01">Sha
 un's introduction</a>\n\n00:43 <a href="https://youtu.be/85sXsaj02yE?t=43"
 >Graham's opening comments</a> \n\n01:20 <a href="https://youtu.be/85sXsaj
 02yE?t=80">Q&A: what are two simple things you'd want viewers to remember 
 about this talk?</a>\n\n02:49 <a href="https://youtu.be/85sXsaj02yE?t=169"
 >Q&A: What is the motivation for this work?</a>: focus is on the mass rang
 e between 1 MeV and 1 GeV\, a particularly interesting region for cosmolog
 ical constraints   \n\n08:36 <a href="https://youtu.be/85sXsaj02yE?t=516">
 1st slide: Where to look for hidden sectors</a>\n\n09:44 <a href="https://
 youtu.be/85sXsaj02yE?t=584">Why bother with cosmology?</a>: tie-in with co
 nstraints previously identified\n\n10:51 <a href="https://youtu.be/85sXsaj
 02yE?t=651">Big Bang nucleosynthesis</a>: 3 slides\n\n14:08 <a href="https
 ://youtu.be/85sXsaj02yE?t=848">Electromagnetic Cascade</a>: several proces
 ses outlined\; one very important thing that has been a little neglected i
 s final-state radiation\n\n15:22 <a href="https://youtu.be/85sXsaj02yE?t=9
 22">Photon spectrum</a>: 2 slides\; conventional wisdom is to use the univ
 ersal spectrum method\, but it breaks down in this sub-GeV case for severa
 l reasons\, see top of pg3 of paper\n\n16:09 <a href="https://youtu.be/85s
 Xsaj02yE?t=969">the universal spectrum method results in orders of magnitu
 de differences from the exact calculations at this scale</a>: it was previ
 ously known this can occur near or below the GeV scale\n\n17:30 <a href="h
 ttps://youtu.be/85sXsaj02yE?t=1050">Light element abundances</a>: 3 observ
 ables trying to constrain</a>\n\n18:53 <a href="https://youtu.be/85sXsaj02
 yE?t=1133">Boltzmann equations</a>\n\n19:46 <a href="https://youtu.be/85sX
 saj02yE?t=1186">Nucleon-destruction</a>\n\n20:42 <a href="https://youtu.be
 /85sXsaj02yE?t=1242">Benchmarks for photon injection</a>\n\n23:38 <a href=
 "https://youtu.be/85sXsaj02yE?t=1418">Benchmarks for electron injection</a
 >\n\n24:28 <a href="https://youtu.be/85sXsaj02yE?t=1468">Monochromatic inj
 ection</a>: Figure 7 in paper\n\n26:08 <a href="https://youtu.be/85sXsaj02
 yE?t=1568">Other model independent constraints</a>: 2 slides\; Fig. 2 in p
 aper\n\n28:01 <a href="https://youtu.be/85sXsaj02yE?t=1681">Model dependen
 t constraints</a>: 4 slides\; Figs. 1 and 3 in paper\n\n31:51 <a href="htt
 ps://youtu.be/85sXsaj02yE?t=1911">Discussion on the Lithium problem</a>\n\
 n34:10 <a href="https://youtu.be/85sXsaj02yE?t=2048">CMB ionization constr
 aints</a>: 3 slides\n\n38:05 <a href="https://youtu.be/85sXsaj02yE?t=2285"
 >CMB spectral distortion constraints</a>: 2 slides\n\n38:57 <a href="https
 ://youtu.be/85sXsaj02yE?t=2337">COBE and PIXIE Limits</a>: Fig. 5 in paper
 \n\n39:23 <a href="https://youtu.be/85sXsaj02yE?t=2363">Freeze in abundanc
 es</a>: 2 slides\; section 5.1 of paper\n\n42:04 <a href="https://youtu.be
 /85sXsaj02yE?t=2524">Parameter constraints</a>: Fig. 6 in paper\n\n45:25 <
 a href="https://youtu.be/85sXsaj02yE?t=2725">Conclusions</a>\n\n46:00 <a h
 ref="https://youtu.be/85sXsaj02yE?t=2760">Q&A: Next steps</a>\n\n49:15 <a 
 href="https://youtu.be/85sXsaj02yE?t=2955">Q&A: Recap of take-away message
 s</a>\n\n49:55 <a href="https://youtu.be/85sXsaj02yE?t=2996">Q&A: outside 
 of your own research\, what do you think is the most interesting thing in 
 cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/3/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Julien Lesgourgues (Institut für Theoretische Teilchenphysik und 
 Kosmologie\, RWTH Aachen University)
DTSTART:20200402T050000Z
DTEND:20200402T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/4
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/4/">Cosmology won't measure individual neutrino mass states</a>\nby Jul
 ien Lesgourgues (Institut für Theoretische Teilchenphysik und Kosmologie\
 , RWTH Aachen University) as part of Cosmology Talks\n\n\nAbstract\nJulien
  tells us about the cosmological effects of different neutrino mass states
  (i.e. the same sum of masses\, but different masses for each individual n
 eutrino - e.g. "normal" vs "inverted"). \n\nThere are effects\, but they'r
 e all very small and not even the best future experiments will distinguish
  them.\n\nNon-standard model neutrinos would still have interesting effect
 s\, but it seems that cosmology's insight on the SM ones will be limited t
 o the sum of the masses.\n\n<a href="https://www.youtube.com/watch?v=V68Gv
 zBrAWU">Video of talk</a>\n\nPaper: <a href="https://arxiv.org/abs/2003.03
 354">[2003.03354] What will it take to measure individual neutrino mass st
 ates using cosmology?</a>\, by Maria Archidiacono\, Steen Hannestad\, Juli
 en Lesgourgues\n\nSupplemental info: <a href="https://www.sunnyvagnozzi.co
 m/blog/top-arxiv-week-11-2020">Review of paper by Sunny Vagnozzi</a>\n\n<h
 r>\n\n<b>Index to Key Parts of the Talk:</b>\n\n[00:01] <a href="https://y
 outu.be/V68GvzBrAWU?t=1">Shaun's intro to the topic and Julien's work</a>\
 n\n[00:32] <a href="https://youtu.be/V68GvzBrAWU?t=32">Julien's opening co
 mments summarizing the paper's findings</a> \n\n[01:46] <a href="https://y
 outu.be/V68GvzBrAWU?t=106">Q&A: what are two simple things you'd want view
 ers to remember about this talk?</a>: two take-home messages\, one for par
 ticle physicists and one for cosmologists\n\n[04:01] <a href="https://yout
 u.be/V68GvzBrAWU?t=241">Q&A: what is the motivation for this work?</a>: th
 ere were many papers addressing the same question but situation not crysta
 l clear\, this work used Bayesian evidence which was not used before and a
 lso discusses in detail the physical effects of different mass splittings 
 on the cosmological observables\n\n[05:21] <a href="https://youtu.be/V68Gv
 zBrAWU?t=321">Title page from the paper and collaborators\; definitions of
  acronyms and proxies that will be referred to</a>: normal (NH)\, inverted
  (IH)\, and degenerate (DH) hierarchy\; Proxy 1 (1 massive + 2 massless)\,
  Proxy 2 (2 massive + 1 massless)\n\n[08:09] <a href="https://youtu.be/V68
 GvzBrAWU?t=489">Plot of total neutrino mass vs lightest\, commentary on Fi
 g. 1 of paper</a>\n\n[11:23] <a href="https://youtu.be/V68GvzBrAWU?t=683">
 Total background density evolution for IH and NH compared to the equivalen
 t DH model\, Fig. 2b from paper</a>\n\n[15:11] <a href="https://youtu.be/V
 68GvzBrAWU?t=911">CDM density perturbation evolution for IH or NH compared
  to the equivalent DH model\, Fig. 4a</a>\n\n[17:06] <a href="https://yout
 u.be/V68GvzBrAWU?t=1026">The power spectrum of the different models\; Fig.
  5 from paper</a> \n\n[20:54] <a href="https://youtu.be/V68GvzBrAWU?t=1254
 ">Observable galaxy power spectrum\, Fig. 7a</a>: probably the most intere
 sting plot\, reformulated in terms not of the theoretical matter power spe
 ctrum but of the real observable power spectrum that Euclid will measure\;
  all done analytically or semi-analytically with CLASS code and starting f
 rom linear observables\n\n[25:45] <a href="https://youtu.be/V68GvzBrAWU?t=
 1545">Observable weak lensing\, Fig. 7b</a>\n\n[26:13] <a href="https://yo
 utu.be/V68GvzBrAWU?t=1573">Ratio of the lensed angular power spectra of te
 mperature\, E-mode polarization\, and B-mode polarization for the same mod
 els\, Fig. 6b</a>\n\n[28:54] <a href="https://youtu.be/V68GvzBrAWU?t=1734"
 >Mass reconstruction forecast using DH instead of fiducial NH/IH + Bayesia
 n evidence ratio of "correct" / DH\; Fig. 8</a>\n\n[32:04] <a href="https:
 //youtu.be/V68GvzBrAWU?t=1924">Julien's recap comments on the paper's find
 ings</a>\n\n[36:28] <a href="https://youtu.be/V68GvzBrAWU?t=2188">Q&A: Nex
 t steps</a>\n\n[39:05] <a href="https://youtu.be/V68GvzBrAWU?t=2345">Q&A: 
 outside of your own research\, what do you think is the most interesting t
 hing in cosmology at the moment?</a>\n\n[41:35] <a href="https://youtu.be/
 V68GvzBrAWU?t=2495">Q&A on spatial curvature</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/4/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Deanna C. Hooper (University of Brussels)
DTSTART:20200409T060000Z
DTEND:20200409T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/5
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/5/">CMB spectral distortions are a prime untapped resource</a>\nby Dean
 na C. Hooper (University of Brussels) as part of Cosmology Talks\n\n\nAbst
 ract\nDeanna tells us about what we could learn from future measurements o
 f the spectral distortions in the CMB\, as well as how spectral distortion
 s complement current and future measurements of CMB anisotropies. She also
  discusses CLASS (v3.0)\, the code you can (very soon) use to calculate pr
 edictions for both.\n\nThere is a guaranteed spectral distortion signal to
  detect within ΛCDM and the possibility to constrain many possible deviat
 ions\, including primordial black holes and decaying dark matter. In fact\
 , we can detect the signal even if the PBHs and/or decaying dark matter on
 ly make up one part in a million of the total dark matter!\n\nWhy have we 
 waited so long (and are still waiting) for an updated measurement after CO
 BE-FIRAS\, which is now more than 25 years old?! I don't know\, but hopefu
 lly it won't be another 25.\n\n<a href="https://www.youtube.com/watch?v=pR
 8MrqlCz0k">Video of Talk</a>\n\nPaper: <a href="https://arxiv.org/abs/1910
 .04619">[1910.04619] The synergy between CMB spectral distortions and anis
 otropies</a>\, by Matteo Lucca\, Nils Schöneberg\, Deanna C. Hooper\, Jul
 ien Lesgourgues\, Jens Chluba\n\n<a href="https://lesgourg.github.io/class
 _public/class.html">CLASS\, the Cosmic Linear Anisotropy Solving System</a
 >\n\nSupplemental Info: \n\n<a href="https://twitter.com/DCHooper91/status
 /1183084231267885057">Deanna's 20-tweet thread on this paper</a>\n\nDeanna
  also does live streams about cosmology/the universe on Periscope. These a
 re aimed at a general audience: <a href="https://www.pscp.tv/DCHooper91/1L
 yxBNjVbzjxN">https://www.pscp.tv/DCHooper91/1LyxBNjVbzjxN</a>\n\n<hr>\n\n<
 b>Index to Key Parts of the Talk:</b>\n\n[00:02] <a href="https://youtu.be
 /pR8MrqlCz0k?t=2">Shaun's intro to the topic and Deanna's work</a>\n\n[00:
 45] <a href="https://youtu.be/pR8MrqlCz0k?t=45">Deanna's opening comments 
 on this work</a>: spectral distortions (SDs)\, deviations from a perfect b
 lack body spectrum\, have very much not been exploited to full potential\;
  a whole new region of parameter space can be explored\; first step was to
  implement the full calculation of SDs in the standard Boltzmann code CLAS
 S\; can now produce both the anisotropy and SD predictions for the same mo
 del\n\n[01:52] <a href="https://youtu.be/pR8MrqlCz0k?t=112">Q&A: what are 
 two simple things you'd want viewers to remember about this talk?</a>: (1)
  SDs are the future of CMB\, even with future CMB missions\; SDs will allo
 w several orders of magnitude improvements in some regions of parameter sp
 ace\, and (2) we now have a very powerful tool in CLASS v3 which computes 
 SDs in parallel with anisotropies.\n\n[02:33] <a href="https://youtu.be/pR
 8MrqlCz0k?t=153">Q&A: what is the motivation for this work?</a>: there is 
 only one observation of the spectrum of CMB photons from COBE-FIRAS 25-yea
 rs ago\, with deviations of 10^-5\; but even with ΛCDM\, SDs are clearly 
 predicted on the order of 10^-8\; if an SD mission does not measure anisot
 ropies at 10^-8\, it means ΛCDM is wrong\; other models also predicting S
 Ds\; an SD mission could distinguish between models\; observation is reall
 y lagging behind the theory\; SDs are extremely well understood\, studied 
 for 30-40 years\; improvements in code\, mainly by Jens Chluba\; SD missio
 ns have been proposed but not yet funded\n\n[05:42] <a href="https://youtu
 .be/pR8MrqlCz0k?t=342">Q&A (an aside): Why is it taking so long for a new 
 mission to probe SDs?</a>: problem of foreground removal\; perhaps overloo
 ked as only a small part of the community is pushing for this\; gaining mo
 re and more attention now\; being able to test the predictions of ΛCDM is
  something we should be doing\; NASA roadmap includes SDs but nothing offi
 cially approved yet\; feasible to have measurements within 15-20 years\n\n
 [07:20] <a href="https://youtu.be/pR8MrqlCz0k?t=440">Returning to motivati
 ons</a>: paper is long but intended as a review of the whole formalism whi
 ch streamlines earlier literature and details of the new CLASS code\n\n[08
 :52] <a href="https://youtu.be/pR8MrqlCz0k?t=532">Slide of paper title pag
 e and collaborators</a>\n\n[09:07] <a href="https://youtu.be/pR8MrqlCz0k?t
 =547">Main Technicalities of Spectral Distortions</a>: 4 contributions to 
 the total distortion to the photon intensity spectrum\; other comments on 
 frequency bins\, amplitude of the SDs\, heating function\, branching ratio
 s\n\n[17:10] <a href="https://youtu.be/pR8MrqlCz0k?t=1030">Branching ratio
 s slide</a>: CLASS calculations plot of the 4 distortion types\n\n[21:42] 
 <a href="https://youtu.be/pR8MrqlCz0k?t=1302">SDs to the total photon inte
 nsity caused by ΛCDM processes and basic extensions</a>: testable predict
 ion of ΛCDM if we had the satellite to do it\n\n[24:20] <a href="https://
 youtu.be/pR8MrqlCz0k?t=1460">SDs to the total photon intensity caused by D
 M decay and annihilation</a>: Decaying DM can be constrained by SDs\; Fig.
  1 left panel and Fig. 2 right panel in paper\n\n[25:40] <a href="https://
 youtu.be/pR8MrqlCz0k?t=1540">Heating rate produced by DM decay and annihil
 ation</a>: Fig. 4 left panel in paper\n\n[26:20] <a href="https://youtu.be
 /pR8MrqlCz0k?t=1580">SDs to the total photon intensity caused by PBH evapo
 ration</a>: Figure 5 right panel in paper.\n\n[27:10] <a href="https://you
 tu.be/pR8MrqlCz0k?t=1630">Making mock data to see what we'd be able to do 
 with future missions</a>\n\n[28:26] <a href="https://youtu.be/pR8MrqlCz0k?
 t=1706">Constraints from different current and future missions for ΛCDM +
  n_run</a>: 5 different cases involving combinations of Planck\, FIRAS\, P
 IXIE\, LiteBIRD\, CMB-S4\, PRISM\; Fig. 7 in paper\n\n[33:10] <a href="htt
 ps://youtu.be/pR8MrqlCz0k?t=1990">Constraints on decaying DM fraction as a
  function of the particle lifetime</a>: Deanna's favorite plot from the pa
 per\, Fig. 8\; the part of the plot where spectral distortions are needed\
 ; different regions of parameter space\, one can be constrained by anisotr
 opies and the other with SDs\n\n[35:55] <a href="https://youtu.be/pR8MrqlC
 z0k?t=2155">Constraints on PBHs as a function of their mass</a>: they foun
 d a new way to study PBH evaporation\; Fig. 9 in paper\n\n[39:05] <a href=
 "https://youtu.be/pR8MrqlCz0k?t=2345">Q&A about using CLASS v3</a>\n\n[40:
 19] <a href="https://youtu.be/pR8MrqlCz0k?t=2419">Next Steps</a>: 2 papers
  in the pipeline using this framework\; 3rd paper on foreground removal\n\
 n[42:56] <a href="https://youtu.be/pR8MrqlCz0k?t=2576">Reiterating 2 takea
 way points from talk</a>\n\n[43:40] <a href="https://youtu.be/pR8MrqlCz0k?
 t=2620">Q&A: outside of your own research\, what do you think is the most 
 interesting thing in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/5/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Omar Darwish (DAMP\, University of Cambridge)
DTSTART:20200416T060000Z
DTEND:20200416T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/6
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/6/">Lensing maps are great\, but they're even better with the tSZ effec
 t removed!</a>\nby Omar Darwish (DAMP\, University of Cambridge) as part o
 f Cosmology Talks\n\n\nAbstract\nOmar tells us about the excellent quality
  lensing map he's produced with the Atacama Cosmology Telescope collaborat
 ion. You honestly won't believe how well this lensing map correlates with 
 the cosmic infrared background (sorry about the clickbait). \n\nThis map w
 ill be incredibly useful to cross-correlate with any dataset of tracers in
 side the relatively large window of ACT observations. It will be public ve
 ry soon\, so once it is you should definitely be using it!\n\nOmar also ex
 plains how he and the collaboration\, for the first time\, removed the ann
 oying thermal Sunyaev–Zeldovich contamination that ordinarily produces a
  ~10% bias in sigma8 (and thus any other cosmological parameter correlated
  with sigma8).\n\n<a href="https://www.youtube.com/watch?v=BnFxAFrxbtI">Vi
 deo of Talk</a>\n\nPaper: <a href="https://arxiv.org/abs/2004.01139">[2004
 .01139] The Atacama Cosmology Telescope: A CMB lensing mass map over 2100 
 square degrees of sky and its cross-correlation with BOSS-CMASS galaxies</
 a>\n\n<a href="https://www.sunnyvagnozzi.com/blog/top-arxiv-week-14-2020">
 Review of paper by Sunny Vagnozzi</a>\n\n<hr>\n\n<b>Index to Key Parts of 
 the Talk:</b>\n\n[00:02] <a href="https://youtu.be/BnFxAFrxbtI?t=2">Shaun'
 s introduction</a>\n\n[00:23] <a href="https://youtu.be/BnFxAFrxbtI?t=23">
 Omar's opening comments on this work</a>\n\n[02:24] <a href="https://youtu
 .be/BnFxAFrxbtI?t=144">Q&A: what are two simple things you'd want viewers 
 to remember about this talk?</a>\n\n[05:32] <a href="https://youtu.be/BnFx
 AFrxbtI?t=332">Q&A: what is the motivation for this work?</a>\n\n[07:52] <
 a href="https://youtu.be/BnFxAFrxbtI?t=472">Title slide of talk and collab
 orators</a>: ACTPol lensing maps and foreground-cleaned galaxy correlation
 s\; with Mathew Madhavacheril\, Blake Sherwin\, and the ACT Collaboration\
 n\n[08:45] <a href="https://youtu.be/BnFxAFrxbtI?t=525">CMB Lensing Intro<
 /a>: lensing deflection field\; lensing convergence field κ \n\n[12:02] <
 a href="https://youtu.be/BnFxAFrxbtI?t=722">CMB Lensing Reconstruction Bas
 ics</a>\n\n[14:27] <a href="https://youtu.be/BnFxAFrxbtI?t=867">ACT Experi
 ment</a>: effective area BOSS-North + Deep56 ~ 2100 sq deg\; overlap with 
 multiple surveys (BOSS\, DES\,...)\n\n[16:11] <a href="https://youtu.be/Bn
 FxAFrxbtI?t=971">CMB Lensing from ACT</a>: Deep56 ACTPol Lensing <a href="
 https://youtu.be/BnFxAFrxbtI?t=991">[16:31]</a>\; Deep56 ACTPol Lensing vs
  Planck CIB <a href="https://youtu.be/BnFxAFrxbtI?t=1181">[19:41]</a> (plo
 t shown here is top part of Fig. 2 in paper)\; BOSS-N ACTPol Lensing vs Pl
 anck CIB <a href="https://youtu.be/BnFxAFrxbtI?t=1252">[20:52]</a> (bottom
  part of Fig. 2 in paper)\n\n[21:32] <a href="https://youtu.be/BnFxAFrxbtI
 ?t=1292">ACT CMB Lensing Maps</a>\n\n[25:38] <a href="https://youtu.be/BnF
 xAFrxbtI?t=1538">Many CMB Lensing x Galaxy papers</a>\n\n[27:16] <a href="
 https://youtu.be/BnFxAFrxbtI?t=1636">One particular systematic effect for 
 low-z galaxy lensing cross correlations</a>: this effect will become impor
 tant for AdvACT and Simons Observatory\n\n[30:44] <a href="https://youtu.b
 e/BnFxAFrxbtI?t=1844">Systematics: tSZ contamination</a>: important for TT
  dominated lensing maps\; negative bias ~10 - 20%\n\n[32:06] <a href="http
 s://youtu.be/BnFxAFrxbtI?t=1926">Removing tSZ contamination</a>: three sli
 des\n\n[36:07] <a href="https://youtu.be/BnFxAFrxbtI?t=2167">tSZ cleaned C
 MB lensing maps from ILC ACT+Planck</a>\n\n[38:20] <a href="https://youtu.
 be/BnFxAFrxbtI?t=2300">Symmetrising gradient cleaning for foreground remov
 al</a>\n\n[44:36] <a href="https://youtu.be/BnFxAFrxbtI?t=2676">Minimum va
 riance forecasted lensing noise</a>\n\n[45:24] <a href="https://youtu.be/B
 nFxAFrxbtI?t=2724">Contaminated vs non-contaminated measurement</a>\n\n[46
 :07] <a href="https://youtu.be/BnFxAFrxbtI?t=2767">Simple amplitude fit</a
 >\; refers to Fig. 5\, pg10\, of paper\n\n[46:45] <a href="https://youtu.b
 e/BnFxAFrxbtI?t=2805">Next Steps</a>\n\n[48:37] <a href="https://youtu.be/
 BnFxAFrxbtI?t=2917">Conclusions</a>\n\n[49:40] <a href="https://youtu.be/B
 nFxAFrxbtI?t=2980">Q&A: outside of your own research\, what do you think i
 s the most interesting thing in cosmology at the moment?</a>\n\nSupplement
 al info: <a href="https://twitter.com/just_shaun/status/125092144293953126
 4">A tweet thread by Shaun about this talk</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/6/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Jurek Bauer (Georg August University of Göttingen)
DTSTART:20200424T060000Z
DTEND:20200424T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/7
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/7/">Fuzzy dark matter arising from GUT scale physics should be ruled in
 /out by SKA</a>\nby Jurek Bauer (Georg August University of Göttingen) as
  part of Cosmology Talks\n\n\nAbstract\nJurek tells us about the prospects
  for constraining axion (aka ultralight aka fuzzy) dark matter with future
  21cm intensity mapping survey such as SKA and HIRAX.\n\nAxion models aris
 ing from specific energy scales predict that an axion with a given mass wi
 ll only provide a certain fraction of the total dark matter. It seems plau
 sible that with SKA we will be able to detect ultralight dark matter even 
 if it arises from a GUT scale axion model. An observational noise model fo
 r SKA was included to make this claim\, but as of yet no theoretical uncer
 tainty is included in the calculation.\n\n<a href="https://www.youtube.com
 /watch?v=bMlrDOWw978">Video of talk</a>\n\nPaper: <a href="https://arxiv.o
 rg/abs/2003.09655">[2003.09655] Intensity Mapping as a Probe of Axion Dark
  Matter</a>\, by Jurek B. Bauer\, David J. E. Marsh\, Renée Hložek\, Ham
 sa Padmanabhan\, Alex Laguë\n\n<hr>\n\n<b>Index to Key Parts of the Talk:
 </b>\n\n[00:02] <a href="https://youtu.be/bMlrDOWw978?t=2">Shaun's intro t
 o the topic and Jurek's work</a>\n\n[00:57] <a href="https://youtu.be/bMlr
 DOWw978?t=57">Jurek's brief summary of the paper</a>: we investigated the 
 impact of ultralight axions on 21cm intensity mapping (IM) in the post-rei
 onization universe\; vastly increases the accessible modes\; use a data-dr
 iven framework for the HI power spectrum provided by the HI halo model of 
 Padmanabhan+ 2017 (a separate Cosmology Talk is available on this at <a hr
 ef="https://youtu.be/K8bS_52_XMk">youtu.be/K8bS_52_XMk</a>)\; etc. \n\n[02
 :27] <a href="https://youtu.be/bMlrDOWw978?t=147">Q&A: what are two simple
  things you'd want viewers to remember about this talk?</a>: (1) their HI 
 halo model allowed extending the axion phenomenology to a completely new l
 evel\; it highlights the importance of the bias\, and (2) exciting prospec
 ts with near future surveys (SKA1MID\, HIRAX\, CMB-SO)\, which in combinat
 ion can test the theoretical predictions\n\n[03:54] <a href="https://youtu
 .be/bMlrDOWw978?t=234">Q&A: what is the motivation for this work?</a>: ult
 ralight axions (ULAs) are a well-motivated DM candidate\, and (2) work by 
 Carucci+ 2017 (more at <a href="https://youtu.be/bMlrDOWw978?t=1742">[29:0
 2]</a>)\n\n[08:39] <a href="https://youtu.be/bMlrDOWw978?t=519">First slid
 e: What is 21cm Intensity Mapping?</a>: includes commments on Fig. 13\, pg
 12\, of the paper\n\n[10:40] <a href="https://youtu.be/bMlrDOWw978?t=640">
 Axion Physics</a>: large de Broglie wavelength introduces scale-dependent 
 pressure\; ULAs suppress the matter power spectrum on small scales\, depen
 ding on their mass\; axionCAMB used for computation. See section 2.1 and F
 ig. 1 of the paper.\n\n[12:57] <a href="https://youtu.be/bMlrDOWw978?t=777
 ">Modeling the 21cm signal</a>\; halo mass function (HMF)\; halo bias\; ne
 utral hydrogen - halo mass relation\; neutral hydrogen density profile\; r
 edshift space distortions are ignored in the present study\, a conservativ
 e assumption (see pg4 of paper)\n\n[16:47] <a href="https://youtu.be/bMlrD
 OWw978?t=1047">HI Halo Model</a>: comments based on Fig. 2\, pg4\, of pape
 r\n\n[17:52] <a href="https://youtu.be/bMlrDOWw978?t=1072">Modeling the 21
 cm signal</a>: Use spherical harmonics tomography: slice survey volume int
 o redshift bins and do spherical harmonic decomposition for the surface\, 
 similar to CMB\n\n[19:30] <a href="https://youtu.be/bMlrDOWw978?t=1170">Ac
 commodating Axions</a>: comments on Fig. 3 on pg6 of the paper\n\n[22:39] 
 <a href="https://youtu.be/bMlrDOWw978?t=1359">HMF and HI bias</a>: comment
 s on Figs. 4 and 5\, pg6\, of the paper\n\n[26:20] <a href="https://youtu.
 be/bMlrDOWw978?t=1580">The HI Power Spectrum for the ULAs</a>: comments on
  Fig. 6\, pg 7\, of the paper\n\n[29:02] <a href="https://youtu.be/bMlrDOW
 w978?t=1742">Comparison to HI Power Spectrum simulation by Carucci+ 2017</
 a>: similar trend but an offset\; comments on Fig. 7\, add'l details on pg
 8 of paper\n\n[32:26] <a href="https://youtu.be/bMlrDOWw978?t=1946">Degene
 racy Structure</a>: 4 parameters are highly degenerate\; ways to break deg
 eneracies\; Fig. 10 comments\, add'l details on pg11 of paper\n\n[34:44] <
 a href="https://youtu.be/bMlrDOWw978?t=2084">Error on Axion Fraction - Ove
 rview</a>: comments on Fig. 9\, pg10\, of the paper\n\n[38:40] <a href="ht
 tps://youtu.be/bMlrDOWw978?t=2320">Combining IM with CMB-SO</a>: comments 
 on Fig. 12\, pg12\, of the paper\n\n[39:28] <a href="https://youtu.be/bMlr
 DOWw978?t=2368">SKA1MID and HIRAX surveys</a>: exclusion limits\; comments
  on Fig. 14\, pg13\, of the paper\n\n[44:08] <a href="https://youtu.be/bMl
 rDOWw978?t=2648">Q&A: What's next?</a>\n\n[44:58] <a href="https://youtu.b
 e/bMlrDOWw978?t=2698">Two takeaway comments</a>\n\n[45:41] <a href="https:
 //youtu.be/bMlrDOWw978?t=2741">Q&A: outside of your own research\, what do
  you think is the most interesting thing in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/7/
END:VEVENT
BEGIN:VEVENT
SUMMARY:W. L. Kimmy Wu (KICP at the University of Chicago)
DTSTART:20200501T060000Z
DTEND:20200501T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/8
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/8/">Planck lensing and line of sight BAO in mild tension. A vital clue 
 in the Hubble mystery?</a>\nby W. L. Kimmy Wu (KICP at the University of C
 hicago) as part of Cosmology Talks\n\n\nAbstract\nKimmy tells us about a s
 ubtle but very interesting tension between Planck lensing data and line of
  sight Baryon Acoustic Oscillation (BAO) data.\n\nShe and her coauthors di
 scovered this via an intriguing mismatch between Planck and South Pole Tel
 escope (SPT) lensing results. The Planck and SPT power spectrum amplitudes
  matched\, but when combined with BAO and Big Bang Nucleosynthesis the inf
 erred Hubble parameters were slightly different.\n\nLike great data-detect
 ives they tracked the source of this discrepancy down to the mismatch betw
 een Planck lensing and line of sight BAO. Why the line of sight BAO might 
 be causing this is unclear. On the Planck lensing side\, it has something 
 to do with the shape of the lensing power spectrum\, e.g. the location of 
 the peak - because SPT only measures the power spectrum's tail and so is o
 nly sensitive to the amplitude.\n\nThe result is definitely interesting\, 
 and unknown by the community until now (as far as I'm aware). Whether it i
 s a red herring or a vital clue in the hunt to solve the Hubble mystery re
 mains to be seen. But it should provide fuel for both model builders and h
 unters of systematic errors trying to solve this mystery.\n\n<a href="http
 s://www.youtube.com/watch?v=JEFQqnxP2jk">Video of talk</a>\n\nPaper: <a hr
 ef="https://arxiv.org/abs/2004.10207">[2004.10207] Hubble constant tension
  between CMB lensing and BAO measurements</a>\, by W.L. Kimmy Wu\, Pavel M
 otloch\, Wayne Hu\, Marco Raveri\n\n<hr>\n\n<b>Index to Key Parts of the T
 alk:</b>\n\n[00:02] <a href="https://youtu.be/JEFQqnxP2jk?t=2">Shaun's int
 ro to the topic and Kimmy's work</a>\n\n[01:10] <a href="https://youtu.be/
 JEFQqnxP2jk?t=70">Kimmy's brief summary of the paper</a>: A tension metric
 \, the update difference in mean parameters\, is applied to trace the orig
 in of the observed differences in H0 between Planck and SPT lensing measur
 ements when both are combined with BAO measurements with a baryon density 
 prior\n\n[01:52] <a href="https://youtu.be/JEFQqnxP2jk?t=112">Q&A: what ar
 e two simple things you'd want viewers to remember about this talk?</a>: (
 1) a surprise result\, the driver of the tension between the two data sets
  is a mild tension between the Planck lensing data set and BAO measurement
 s (in particular\, the line-of-sight BAO measurements appear to be an outl
 ier)\, and (2) a very good use case for this update difference in mean ten
 sion metric\, it allows the data to tell what are the interesting paramete
 r directions to look at\n\n[04:42] <a href="https://youtu.be/JEFQqnxP2jk?t
 =282">Q&A: what is the motivation for this work?</a>: A little history on 
 how they stumbled across this curiosity\; first slide: Ωm\, H0 constraint
 s with galaxy BAO + BBN prior\; SPTpol lensing and Planck lensing are cons
 istent\, but there is something about adding BAO and BBN that draws out va
 rious features of the lensing spectrum that causes a difference in the H0 
 inference  \n\n[11:04] <a href="https://youtu.be/JEFQqnxP2jk?t=664">Brief 
 overview of CMB lensing measurements</a>\n\n[12:51] <a href="https://youtu
 .be/JEFQqnxP2jk?t=771">Planck and SPTpol lensing measurements</a>\n\n[14:1
 8] <a href="https://youtu.be/JEFQqnxP2jk?t=858">The BAO measurements</a> \
 n\n[15:37] <a href="https://youtu.be/JEFQqnxP2jk?t=937">Perpendicular and 
 Parallel BAO</a>\n\n[17:00] <a href="https://youtu.be/JEFQqnxP2jk?t=1020">
 Tension metric: update difference in mean parameters\, Qudm</a>: a modifie
 d version of the simpler metric\, difference in mean parameters\, which wo
 rks well if both data sets are Gaussian\; Qudm is useful where A's posteri
 or is Gaussian but B's is not\, but where A + B are sufficiently approxima
 tely Gaussian\; usefulness of KL decomposition (more details in the paper 
 in section II: Quantifying Tensions)\n\n[22:51] <a href="https://youtu.be/
 JEFQqnxP2jk?t=1371">Choosing the Parameter basis</a>\n\n[26:35] <a href="h
 ttps://youtu.be/JEFQqnxP2jk?t=1595">Qudm: BAO + BBN + SPTpol lens update w
 ith Planck lens</a>: How much fractional constraining power each KL mode c
 ontributes to a parameter\n\n[30:17] <a href="https://youtu.be/JEFQqnxP2jk
 ?t=1817">Qudm: BAO + BBN update with Planck lens</a>\n\n[32:59] <a href="h
 ttps://youtu.be/JEFQqnxP2jk?t=1979">Parallel and perpendicular BAO measure
 ments are consistent</a>\n\n[35:37] <a href="https://youtu.be/JEFQqnxP2jk?
 t=2137">Parallel BAO contributes most to the mild tension between Planck l
 ensing and BAO+BBN</a>\n\n[39:50] <a href="https://youtu.be/JEFQqnxP2jk?t=
 2390">High best-fit Ωm to parallel BAO => high H0</a>\n\n[40:53] <a href=
 "https://youtu.be/JEFQqnxP2jk?t=2453">Redshift slope in parallel BAO measu
 rements drives high Ωm</a>\n\n[42:20] <a href="https://youtu.be/JEFQqnxP2
 jk?t=2540">High Ωm strongly ruled out</a>\n\n[44:23] <a href="https://you
 tu.be/JEFQqnxP2jk?t=2663">Q&A: Where to next?</a>\n\n[47:30] <a href="http
 s://youtu.be/JEFQqnxP2jk?t=2850">Q&A: What might be causing the Hubble ten
 sion?</a>\n\n[50:18] <a href="https://youtu.be/JEFQqnxP2jk?t=3018">Q&A: ou
 tside of your own research\, what do you think is the most interesting thi
 ng in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/8/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Adam Riess (Johns Hopkins University)
DTSTART:20200506T060000Z
DTEND:20200506T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/9
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/9/">Cepheid crowding is not the cause of the Hubble tension</a>\nby Ada
 m Riess (Johns Hopkins University) as part of Cosmology Talks\n\n\nAbstrac
 t\nAdam tells us about what he and collaborators considered to be the lead
 ing candidate for a systematic error in the SHOES measurement of the expan
 sion rate of the Universe. This is "Cepheid crowding"\, the possibility th
 at background sources change our interpretation of Cepheid brightness\, ru
 ining one step in the SHOES distance ladder.\n\nThey devise a nice way to 
 test whether the crowding is correctly accounted for and find that it is. 
 So crowding cannot be the "explanation" of an error in the distance ladder
  measurement of H0.\n\nHe also stresses that both the early and late unive
 rse measurements of H0 are now backed up by multiple different measurement
 s. Therefore\, if the resolution isn't fundamental physics\, then no singl
 e systematic can entirely solve the tension.\n\nWe also discuss a few topi
 cs around the H0 tension\, including what resolution of the tension he wou
 ld pick as most likely if forced to gamble (answer: a deviation from vanil
 la ΛCDM in the early universe)\n\n<a href="https://www.youtube.com/watch?
 v=2LN6dJi0ogI">Video of talk</a>\n\nPaper: <a href="https://arxiv.org/abs/
 2005.02445">[2005.02445] The Accuracy of the Hubble Constant Measurement V
 erified through Cepheid Amplitudes</a>\, by Adam G. Riess\, Wenlong Yuan\,
  Stefano Casertano\, Lucas M. Macri\, Dan Scolnic\n\n<hr>\n\n<b>Index to K
 ey Parts of the Talk:</b>\n\n[00:02] <a href="https://youtu.be/2LN6dJi0ogI
 ?t=2">Shaun's intro to the topic and Adam's work</a>\n\n[00:57] <a href="h
 ttps://youtu.be/2LN6dJi0ogI?t=57">Q&A: Adam's brief summary of the paper</
 a>: Cepheid crowding can be ruled out at greater than 5σ as an issue caus
 ing the Hubble tension\n\n[02:58] <a href="https://youtu.be/2LN6dJi0ogI?t=
 178">Q&A: what are two simple things you'd want viewers to remember about 
 this talk?</a>  \n\n[04:21] <a href="https://youtu.be/2LN6dJi0ogI?t=261">Q
 &A: what is the motivation for this work? Of all the potential systematics
  to check\, why is crowding the one that you chose?</a>\n\n[06:09] <a href
 ="https://youtu.be/2LN6dJi0ogI?t=369">First slide: the paper and the SH0ES
  colleagues involved</a>\n\n[06:49] <a href="https://youtu.be/2LN6dJi0ogI?
 t=409">Background on the Hubble tension problem</a>\n\n[08:38] <a href="ht
 tps://youtu.be/2LN6dJi0ogI?t=518">The distance ladder method for measuring
  the Hubble constant</a>: late universe method\n\n[09:31] <a href="https:/
 /youtu.be/2LN6dJi0ogI?t=571">Representative early universe methods to dete
 rmine the Hubble constant</a>: early vs late universe  determinations diff
 er by 5-6σ (*see Adam's later comment at [37:23] on his rule of thumb to 
 clarify what differentiates early vs late universe methods)\n\n[10:54] <a 
 href="https://youtu.be/2LN6dJi0ogI?t=654">Why do we use Cepheid variable s
 tars?</a>: includes brief comments on other calibration methods besides Ce
 pheids\n\n[12:38] <a href="https://youtu.be/2LN6dJi0ogI?t=758">Importance 
 of Cepheids since there aren't enough supernovae to build the distance lad
 der just from SNe</a>\n\n[13:14] <a href="https://youtu.be/2LN6dJi0ogI?t=7
 94">Cepheids and Crowding - the non-trivial challenge</a>: idealized situa
 tion vs reality for accurate photometric measurements\; cannot resolve the
  non-uniform background under Cepheids but that must be accounted for to m
 easure accurate photometry\; image showing what crowding is\; how to figur
 e out how much crowding there is\; measuring the offset or bias that resul
 ts on average from the other field stars that are crowding into the resolu
 tion element\; extra wrinkles\; possibly the most significant challenge fo
 r Cepheid measurements beyond 20 Mpc is crowding and blending from redder 
 stars particularly in near-infrared observations (Wendy Freedman quote)\n\
 n[15:44] <a href="https://youtu.be/2LN6dJi0ogI?t=944">Amplitudes Provide <
 i>Direct</i> Measure of Cepheid Crowding</a>: crowded flux is bigger fract
 ional contribution when Cepheid at minimum\, which compresses the light cu
 rve amplitude\; mathematical relationship\n\n[18:09] <a href="https://yout
 u.be/2LN6dJi0ogI?t=1089">Three Examples of Different Crowding Levels: NGC 
 1559</a>: illustrates the amplitude compression effect from crowding\n\n[1
 9:45] <a href="https://youtu.be/2LN6dJi0ogI?t=1185">Step 1: Calibrate Ampl
 itude-period Relation with Milky Way Cepheids</a>: Cepheid amplitudes depe
 nd on period\; expected amplitude as a function of period and crowding\n\n
 [21:01] <a href="https://youtu.be/2LN6dJi0ogI?t=1261">Step 2: 224 NIR ampl
 itudes Measured in 4 hosts\, compare to Milky Way (benchmark)</a>: empiric
 ally measured amplitudes match prediction (with no free parameters) from c
 rowding assessed in the conventional way from local (Milky Way) regions\, 
 confirming their accuracy for estimating the background at the (extragalac
 tic) Cepheid locations\n\n[23:21] <a href="https://youtu.be/2LN6dJi0ogI?t=
 1401">Step 3: Constrain "unrecognized" crowding\, compare to Hubble tensio
 n</a>: "unrecognized" crowding needed to explain Hubble tension ruled out 
 at >5σ\n\n[25:10] <a href="https://youtu.be/2LN6dJi0ogI?t=1510">So what c
 ould explain the Hubble tension?</a>\n\n[32:56] <a href="https://youtu.be/
 2LN6dJi0ogI?t=1976">Future Prospects: Improvements coming in the next coup
 le years</a>\n\n[34:50] <a href="https://youtu.be/2LN6dJi0ogI?t=2090">Q&A:
  If you had to guess right now\, what is the most probable explanation on 
 either the theory or observational side?</a>\n\n[37:23] <a href="https://y
 outu.be/2LN6dJi0ogI?t=2243">*Adam's rule of thumb to clarify what differen
 tiates late universe vs early universe methods</a>\n\n[39:13] <a href="htt
 ps://youtu.be/2LN6dJi0ogI?t=2353">Q&A: could a breakdown in the FRW metric
  at late times be an explanation?</a>\n\n[41:10] <a href="https://youtu.be
 /2LN6dJi0ogI?t=2470">Q&A: outside of your own research\, what do you think
  is the most interesting thing in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/9/
END:VEVENT
BEGIN:VEVENT
SUMMARY:J. Colin Hill (Columbia University)
DTSTART:20200515T060000Z
DTEND:20200515T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/10
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/10/">Early dark energy doesn't make cosmology concordant again</a>\nby 
 J. Colin Hill (Columbia University) as part of Cosmology Talks\n\n\nAbstra
 ct\nColin tells us about how even though early dark energy can alleviate t
 he Hubble tension\, it does so at the expense of increasing other tension.
  Early dark energy can raise the predicted expansion rate inferred from th
 e cosmic microwave background (CMB)\, by changing the sound horizon at the
  last scattering surface. However\, the early dark energy also suppresses 
 the growth of perturbations that are within the horizon while it is active
 . This mean that\, to fit the CMB\, the matter density must increase (and 
 the spectral index becomes more blue tilted). The consequence is that the 
 matter power spectrum should get bigger.\n\nIn their paper\, Colin and his
  coauthors show that this affects the weak lensing measurements by DES\, K
 iDS and HSC\, and therefore including those experiments in a full data ana
 lysis makes things discordant again. The Hubble parameter is pulled back d
 own\, restoring most of the tension between local and CMB measurements of 
 H0\, and the tension in S_8 gets magnified by the increased mismatch in th
 e predicted and measured matter power spectrum.\n\nIt is also worth noting
  that\, if you exclude the local measurements of H0\, there is no preferen
 ce for early dark energy in the data.\n\nThere is hope\, perhaps. If the s
 ound horizon could be changed without altering the growth of perturbations
  that might still be a valid resolution\, but it is unlikely to be caused 
 by early dark energy (alone).\n\n<a href="">Video of talk</a>\n\nPaper: <a
  href="https://arxiv.org/abs/2003.07355">[2003.07355] Early Dark Energy Do
 es Not Restore Cosmological Concordance</a>\, by J. Colin Hill\, Evan McDo
 nough\, Michael W. Toomey\, Stephon Alexander\n\n<a href="https://www.sunn
 yvagnozzi.com/blog/top-arxiv-week-12-2020">Review of paper by Sunny Vagnoz
 zi</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>\n\n[00:02] <a hre
 f="https://youtu.be/5JRHFGuPAV8?t=2">Shaun's intro to the topic and Colin'
 s work</a>\n\n[01:15] <a href="https://youtu.be/5JRHFGuPAV8?t=68">Colin's 
 summary of the 2003.07355 paper</a>\n\n[04:52] <a href="https://youtu.be/5
 JRHFGuPAV8?t=292">The broader context to Colin's motivation for this work<
 /a>\n\n[08:16] <a href="https://youtu.be/5JRHFGuPAV8?t=496">First slide: T
 he Hubble Constant</a>\n\n[08:54] <a href="https://youtu.be/5JRHFGuPAV8?t=
 534">Early Dark Energy</a>: earlier EDE papers\; summary plot\; the chain 
 of reasoning leading to the EDE models with a reference to Knox and Millea
  for a nice review\, <a href="https://arxiv.org/abs/1908.03663">1908.03663
 </a>\; EDE models decrease the physical size of the sound horizon imprinte
 d in the CMB - they have added flexibility due to a set of 3 additional ne
 w parameters that are relevant in the calculation of the physical size of 
 the sound horizon\n\n[12:27] <a href="https://youtu.be/5JRHFGuPAV8?t=747">
 How the EDE model has been implemented from a more physical perspective</a
 >: a new (pseudo)-scalar field important prior to recombination\, whose en
 ergy density contribution decays away rapidly just before the redshift of 
 last scattering\; the mass of the scalar field needs to be ~ 10 ^-27 eV\n\
 n[17:36] <a href="https://youtu.be/5JRHFGuPAV8?t=1056">The actual paramete
 rs used to describe this model</a>: 3 physical parameters - mass of the fi
 eld\, a decay constant\, and its initial position on the potential\; these
  are converted into phenomenological parameters which are more closely rel
 ated to what the data can actually constrain\; plot showing fractional con
 tribution of EDE to cosmic energy budget as function of z\n\n[20:05] <a hr
 ef="https://youtu.be/5JRHFGuPAV8?t=1205">EDE maintains a good fit to CMB p
 ower spectrum data with higher H0</a>: plot shows a sub-percent difference
  in the TT power spectrum between ΛCDM (H0=68.21) and EDE model (H0=72.19
 )\n\n[21:40] <a href="https://youtu.be/5JRHFGuPAV8?t=1300">What about larg
 e-scale structure?</a>: motivation for the project - no one had made a plo
 t of the matter power spectrum P(k)\; modified version of the Boltzmann co
 de\, CLASS_EDE\, is public on github\n\n[22:26] <a href="https://youtu.be/
 5JRHFGuPAV8?t=1346">Plot of the matter power spectrum comparing ΛCDM and 
 EDE models</a>: the plot of their ratio highlights the significant differe
 nces\n\n[24:19] <a href="https://youtu.be/5JRHFGuPAV8?t=1459">Parameter Sh
 ifts are the driver for these differences</a>: caused by parameter shifts 
 in the so-called normal cosmological parameters in the EDE scenario compar
 ed to ΛCDM\; also a noticeable shift in the scalar spectral index\n\n[27:
 38] <a href="https://youtu.be/5JRHFGuPAV8?t=1658">Interesting physical eff
 ects due to the EDE itself</a>\n\n[30:28] <a href="https://youtu.be/5JRHFG
 uPAV8?t=1826">Updated EDE Analysis Including Large-Scale Structure Data Se
 ts</a>: includes 2 data sets not included in previous work: DES "3x2pt" fu
 ll likelihood and S8 constraints from HSC and KiDS\; Cobaya code used for 
 the MCMC sampling\n\n[33:08] <a href="https://youtu.be/5JRHFGuPAV8?t=1988"
 >Inclusion of LSS Data</a>\n\n[35:07] <a href="https://youtu.be/5JRHFGuPAV
 8?t=2107">Inclusion of DES/HSC/KiDS</a>: inclusion of LSS data leads to no
 n-detection of EDE component\n\n[36:28] <a href="https://youtu.be/5JRHFGuP
 AV8?t=2184">Analysis without SH0ES</a>: comparing all data sets without SH
 OES\; looking at the posteriors in the EDE parameter space\; broadening of
  error bars when analyzing EDE model\, but no major shifts seen\; H0 tensi
 on persists\; strong upper limit on existence of EDE component\; SH0ES is 
 in 3.5σ tension with other data sets (even in EDE model)\; bottom line: y
 ou can't shift the parameters in the way that's needed for the CMB without
  messing up the large-scale structure data\n\n[38:42] <a href="https://you
 tu.be/5JRHFGuPAV8?t=2322">Summary</a>: SHOES is the only data set driving 
 preference for EDE (moderate evidence\, ~ 2σ)\n\n[40:43] <a href="https:/
 /youtu.be/5JRHFGuPAV8?t=2443">Physical Priors</a>: uniform priors on f_EDE
  and log(z_c) are very non-uniform on physical scalar field parameters f a
 nd m\n\n[41:34] <a href="https://youtu.be/5JRHFGuPAV8?t=2494">Final Summar
 y</a>: \n<ul><li>No evidence for EDE component seen in CMB-only or CMB+LSS
  data</li>\n<li>SHOES constraint is in tension\, even in this model</li>\n
 <li>Basic problem: higher H0 requires higher f_EDE\, which increases σ8 a
 nd hence worsens fit to LSS data</li>\n<li>In short: EDE model does not re
 store concordance</li>\n<li>Use of physical priors (on scalar field parame
 ters) further weakens evidence for EDE</li>\n<li>Follow-up work in progres
 s: (1) validate the BAO and RSD results here using the effective field the
 ory of LSS\; (2) demonstrate that the "all data except SHOES" analysis ind
 eed would detect EDE if it were present in the universe</li>\n<li>Theorist
 s: back to the drawing board</li>\n</ul>\n\n[42:45] <a href="https://youtu
 .be/5JRHFGuPAV8?t=2563">Q&A: Where to next?</a>: upcoming release of ACT c
 osmological parameter measurements in the next couple months\; the observa
 bles that dominate the constraining power are different between ACT (TE) a
 nd Planck (TT).\n\n[44:19] <a href="https://youtu.be/5JRHFGuPAV8?t=2659">Q
 &A discussion on the sound horizon issue)</a>: to be consistent with LSS\,
  the sound horizon would need to be changed (lowered) in a way that does n
 ot then act to suppress the growth of pertubations\n\n[45:49] <a href="htt
 ps://youtu.be/5JRHFGuPAV8?t=2749">Q&A: what do you think is the most proba
 ble explanation of H0 tension?</a>\n\n[48:13] <a href="https://youtu.be/5J
 RHFGuPAV8?t=2893">Q&A: Outside of your own research\, what do you think is
  the most interesting thing in cosmology at the moment?</a>\n\nOther Paper
  References:<br> \n<a href="https://arxiv.org/abs/1811.04083">[1811.04083]
  Early Dark Energy Can Resolve The Hubble Tension</a>\, by V. Poulin\, T. 
 Smith\, T. Karwal\, M. Kamionkowski<br>\n<a href="https://arxiv.org/abs/19
 08.06995">[1908.06995] Oscillating scalar fields and the Hubble tension: a
  resolution with novel signatures</a>\, by T. Smith\, V. Poulin\, M. Amin<
 br>\n<a href="https://arxiv.org/abs/1905.12618">[1905.12618] Acoustic Dark
  Energy: Potential Conversion of the Hubble Tension</a>\, by M. Lin\, G. B
 enevento\, W. Hu\, M. Raveri<br>\n<a href="https://arxiv.org/abs/1904.0101
 6">[1904.01016] Rock 'n' Roll Solutions to the Hubble Tension</a>\, by P. 
 Agrawal\, F. Cyr-Racine\, D. Pinner\, L. Randall\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/10/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Hamsa Padmanabhan (CITA\, University of Toronto)
DTSTART:20200529T060000Z
DTEND:20200529T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/11
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/11/">The overlap between HI halo modelling and cosmology</a>\nby Hamsa 
 Padmanabhan (CITA\, University of Toronto) as part of Cosmology Talks\n\n\
 nAbstract\nHamsa tells us about how baryonic gases arrange themselves insi
 de galaxies\, specifically in the context of the HI halo model (with some 
 deviation to discuss other gases like molecular hydrogen and carbon monoxi
 de).\n\nThis is a great talk in its own right\, full of really useful info
 rmation for cosmologists who want to know how intensity mapping\, etc\, wi
 ll be used for cosmology - but\, it also acts as a good companion talk to 
 Jurek Bauer's talk on constraining axion dark matter using intensity mappi
 ng (<a href="https://www.youtube.com/watch?v=bMlrDOWw978">https://www.yout
 ube.com/watch?v=bMlrDOWw978</a>). Hamsa was a coauthor on Jurek's paper an
 d the expert in that collaboration on the HI/intensity mapping part.\n\nTh
 is video builds up to eventually being about this paper\, <a href="https:/
 /arxiv.org/abs/2002.01489">https://arxiv.org/abs/2002.01489</a>\, however 
 in getting there it covers the whole background of modelling HI and other 
 baryonic gases within galaxies in an information packed\, but accessible w
 ay.\n\n<a href="https://www.youtube.com/watch?v=K8bS_52_XMk">Video of talk
 </a>\n\nPaper: <a href="https://arxiv.org/abs/2002.01489">[2002.01489] New
  empirical constraints on the cosmological evolution of gas and stars in g
 alaxies</a>\, by Hamsa Padmanabhan\, Abraham Loeb\n\n<hr>\n\n<b>Index to K
 ey Parts of the Talk:</b>\n\n[00:01] <a href="https://youtu.be/K8bS_52_XMk
 ?t=1">Shaun's introduction to Hamsa's work</a>\n\n[01:12] <a href="https:/
 /youtu.be/K8bS_52_XMk?t=72">Hamsa's brief summary of the paper and her wor
 k</a>\n\n[03:27] <a href="https://youtu.be/K8bS_52_XMk?t=207">Q&A: what ar
 e two simple things you'd want viewers to remember about this talk?</a>\n\
 n[06:22] <a href="https://youtu.be/K8bS_52_XMk?t=382">Q&A: What problems w
 ere unsolved that motivated this work?</a>\n\n[09:21] <a href="https://you
 tu.be/K8bS_52_XMk?t=561">Details on the paper</a>: "everything here is mor
 e or less centered around this innovative technique known as intensity map
 ping...it's been gaining a lot of attention over the past few years and in
  fact over the last decade"\n\n[10:02] <a href="https://youtu.be/K8bS_52_X
 Mk?t=602">What intensity mapping is</a>: "much faster and much cheaper" th
 an other methods\; "it can be done for different lines\, for different tra
 cers of large scale structure (e.g.\, 21cm\, CO\, C<sup>+</sup>)"\n\n[11:2
 2] <a href="https://youtu.be/K8bS_52_XMk?t=682">Impact of astrophysics and
  the "astrophysical systematic" that needs to be quantified</a>: "how much
  does the uncertainty in the astrophysics (foreground) propagate into the 
 power spectrum of 21cm intensity fluctuations?"\n\n[15:27] <a href="https:
 //youtu.be/K8bS_52_XMk?t=927">Efficiently modeling the astrophysics</a>: "
 the most natural way to do this seems to be by using a halo model framewor
 k" for associating baryonic gas with dark matter halos\n\n[17:44] <a href=
 "https://youtu.be/K8bS_52_XMk?t=1064">The HI halo model and its free param
 eters</a>\n\n[25:02] <a href="https://youtu.be/K8bS_52_XMk?t=1502">Availab
 le HI data</a>\n\n[27:54] <a href="https://youtu.be/K8bS_52_XMk?t=1674">Co
 nstraints</a>\n\n[28:54] <a href="https://youtu.be/K8bS_52_XMk?t=1734">Bes
 t fit halo model</a>\n\n[31:04] <a href="https://youtu.be/K8bS_52_XMk?t=18
 64">Insights</a>\n\n[36:46] <a href="https://youtu.be/K8bS_52_XMk?t=2206">
 Cosmology and astrophysics constraints: precision and accuracy</a>\n\n[37:
 50] <a href="https://youtu.be/K8bS_52_XMk?t=2270">CO contraints: z ~ 0.3</
 a>\n\n[38:14] <a href="https://youtu.be/K8bS_52_XMk?t=2294">A halo model f
 or carbon monoxide</a>\n\n[40:54] <a href="https://youtu.be/K8bS_52_XMk?t=
 2454">Reverse engineering</a>: "Abundance matching\; combine HI constraint
 s with empirical evolution of stellar-halo relations"\n\n[42:36] <a href="
 https://youtu.be/K8bS_52_XMk?t=2556">Stellar mass buildup</a>: Commentary 
 on Figures 2 and 4 in the paper\n\n[46:20] <a href="https://youtu.be/K8bS_
 52_XMk?t=2781">Summary</a><br><br>\n \n[49:48] <a href="https://youtu.be/K
 8bS_52_XMk?t=2988">Future work</a> \n\n[51:36] <a href=https://youtu.be/K8
 bS_52_XMk?t=3096">Q&A: Outside of your own research\, what are your though
 ts on what's most interesting in cosmology currently?\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/11/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Clare Burrage (University of Nottingham)
DTSTART:20200605T060000Z
DTEND:20200605T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/12
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/12/">Atomic lab experiments rule out almost all of chameleon dark energ
 y model-space</a>\nby Clare Burrage (University of Nottingham) as part of 
 Cosmology Talks\n\n\nAbstract\nClare tells us about how chameleon dark ene
 rgy models can be very tightly constrained by simple atomic lab experiment
 s (well\, simple compared to particle accelerators and space telescopes). 
 \n\nChameleon models were popular for dark energy because their non-linear
  potentials generically create screening mechanisms\, which stop them gene
 rating a "fifth force" even though they couple to matter. This means we wo
 uldn't normally see their effects on Earth. However\, in a suitably precis
 e atomic experiment the screening can be minimised and their effect measur
 ed.\n\nIn less than five years\, Clare and her collaborators went from the
  idea to the completed experiment\, which rules out almost all of the viab
 le parameter space where a chameleon model can explain dark energy. Only a
  tiny sliver of allowed space is left\, albeit at fundamental parameter va
 lues that would be natural ones - so maybe the chameleon is hiding right t
 here waiting?\n\n<a href="https://www.youtube.com/watch?v=xzm5rkhyj7E">Vid
 eo of talk</a>\n\nMost relevant paper: <a href="https://arxiv.org/abs/1812
 .08244">[1812.08244] Experiment to detect dark energy forces using atom in
 terferometry</a>\, by Dylan Sabulsky\, Indranil Dutta\, E. A. Hinds\, Benj
 amin Elder\, Clare Burrage\, Edmund J. Copeland\n\n<hr>\n\n<b>Index to Key
  Parts of the Talk:</b>\n\n[00:02] <a href="https://youtu.be/xzm5rkhyj7E?t
 =2">Shaun's intro to the topic and Clare's work</a>\n\n[01:15] <a href="ht
 tps://youtu.be/xzm5rkhyj7E?t=75">Clare's introductory brief comments</a>\n
 \n[01:45] <a href="https://youtu.be/xzm5rkhyj7E?t=105">Q&A: what are a cou
 ple things you'd want viewers to remember about this talk?</a>\n\n[02:27] 
 <a href="https://youtu.be/xzm5rkhyj7E?t=147">Q&A: what is the background m
 otivation to your recent work and to this topic in general?</a>\n\n[04:17]
  <a href="https://youtu.be/xzm5rkhyj7E?t=257">Q&A: In the near past\, what
  were the specific problems about this?</a>\n\n[06:25] <a href="https://yo
 utu.be/xzm5rkhyj7E?t=385">First slide: A Very Old Idea</a> The types of ex
 periments we're going to talk about is the idea of testing the equivalence
  principle...What we're going to see is that these theories of dark energy
 \, or modified gravity\, or scalar fields kind of related to dark energy\,
  give you a reason to expect that under certain circumstances\, light obje
 cts or small objects would fall faster than large ones...that they feel an
  additional force essentially...and the interesting physics is why that on
 ly happens under certain circumstances\n\n[07:42] <a href="https://youtu.b
 e/xzm5rkhyj7E?t=462">The standard picture: If the New Physics is Linear</a
 >\n\n[10:55] <a href="https://youtu.be/xzm5rkhyj7E?t=655">If the New Physi
 cs is Non-Linear: Screening Mechanisms</a>\n\n[12:43] <a href="https://you
 tu.be/xzm5rkhyj7E?t=763">The Chameleon</a> A scalar field with canonical k
 inetic terms\, non-linear potential\, and direct coupling to matter.  (<a 
 href="https://arxiv.org/abs/astro-ph/0309300">astro-ph/0309300</a>)\n\n[15
 :58] <a href="https://youtu.be/xzm5rkhyj7E?t=958">Varying Mass</a> Dynamic
 s governed by an effective potential. Non-linearities in the potential mea
 ns that the mass of the field depends on the local energy density.\n\n[17:
 04] <a href="https://youtu.be/xzm5rkhyj7E?t=1024">Chameleon Screening</a> 
  (<a href="https://arxiv.org/abs/1412.6373">1412.6373</a>)\n\n[23:21] <a h
 ref="https://youtu.be/xzm5rkhyj7E?t=1401">Why Atoms?</a> (<a href="https:/
 /arxiv.org/abs/1408.1409">1408.1409</a>)\n\n[25:51] <a href="https://youtu
 .be/xzm5rkhyj7E?t=1549">Atom Interferometry</a>\n\n[30:17] <a href="https:
 //youtu.be/xzm5rkhyj7E?t=1817">Atom Interferometry for Chameleons</a>  (<a
  href="https://arxiv.org/abs/1812.08244">1812.08244</a>\, Experiment to de
 tect dark energy forces using atom interferometry)\n\n[32:04] <a href="htt
 ps://youtu.be/xzm5rkhyj7E?t=1924">Imperial Experiment</a>\n\n[40:23] <a hr
 ef="https://youtu.be/xzm5rkhyj7E?t=2423">Combined Chameleon Constraints</a
 > (<a href="https://arxiv.org/abs/1609.01192">1609.01192</a> and <a href="
 https://arxiv.org/abs/1709.09071">1709.09071</a>)\n\n[41:08] <a href="http
 s://youtu.be/xzm5rkhyj7E?t=2468">Summary</a>\n\n[46:43] <a href="https://y
 outu.be/xzm5rkhyj7E?t=2803">Clare's work in large collaboration atomic exp
 eriment proposals</a>\n\n[48:15] <a href="https://youtu.be/xzm5rkhyj7E?t=2
 895">Q&A: Where to next?</a>\n\n[49:47] <a href="https://youtu.be/xzm5rkhy
 j7E?t=2987">Q&A: Outside of your own research\, what do you think is the m
 ost interesting thing in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/12/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Amanda Weltman (University of Cape Town)
DTSTART:20200611T060000Z
DTEND:20200611T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/13
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/13/">Fast radio bursts and cosmology</a>\nby Amanda Weltman (University
  of Cape Town) as part of Cosmology Talks\n\n\nAbstract\nAmanda Weltman te
 lls us about fast radio bursts (FRBs)\, which have been in the news recent
 ly in the context of the "missing baryons". She tells us about that measur
 ement (and her own theoretical work preceding it)\, but also about FRBs in
  general and how they'll be useful for cosmology.\n\nFRBs are what it soun
 ds like they are\, short bursts of radio frequency radiation detected from
  outside the solar system. We still don't know 100% what their origin is\,
  but it is possible at least some of them come from magnetars (neutron sta
 rs with very large magnetic fields).\n\nA very useful property of FRBs is 
 that they have a non-zero dispersion relation in the intergalactic medium\
 , because they interact with the ionised electrons in that space. This mak
 es it possible to measure the electron density of the inter-galactic mediu
 m\, and/or to measure how far the FRBs are away from us. In each case this
  is based on how much the frequencies within each FRB have dispersed by th
 e time we detect them.\n\nIf you're a cosmologist looking for a primer on 
 FRBs and how they'll be relevant for your research\, this is the video you
 're looking for.\n\n<a href="https://www.youtube.com/watch?v=cqK18-O3ptA">
 Video of talk</a>\n\n<a href="https://frbtheorycat.org/index.php/Main_Page
 ">FRB theory wiki</a>\n\nRelevant papers:<br>\n<a href="https://arxiv.org/
 abs/1909.02821">[1909.02821] Probing Diffuse Gas with Fast Radio Bursts</a
 ><br> \n<a href="https://arxiv.org/abs/1905.07132">[1905.07132] Fast Radio
  Burst Cosmology & HIRAX</a><br> \n<a href="https://arxiv.org/abs/1810.058
 36">[1810.05836] A Living Theory Catalogue for FRBs</a><br>\n\n<hr>\n\n<b>
 Index to Key Parts of the Talk:</b>\n\n[00:02] <a href="https://youtu.be/c
 qK18-O3ptA?t=2">Shaun's intro to the topic and Amanda's work</a>: includes
  her comments as an expert on chameleon theory: e.g.\, the experiments don
 e to rule out parts of the chameleon phase space\; the original theory is 
 still alive\; observations have ruled out a lot of alternative dark energy
  theories.\n\n[02:01] <a href="https://youtu.be/cqK18-O3ptA?t=121">First s
 lide summarizing what fast radio bursts are and why they're useful for cos
 mology</a>\n\n[04:43] <a href="https://youtu.be/cqK18-O3ptA?t=283">Q&A: wh
 at are two simple things you'd want viewers to take away from this talk?</
 a>\n\n[06:10] <a href="https://youtu.be/cqK18-O3ptA?t=370">What we know ab
 out FRBs</a>\n\n[08:38] <a href="https://youtu.be/cqK18-O3ptA?t=518">Dispe
 rsion Measure (DM)</a>\n\n[10:46] <a href="https://youtu.be/cqK18-O3ptA?t=
 646">FRB Implications for Cosmology</a>: implications at different scales:
  early universe\, late universe\, intermediate scales\; there are more imp
 lications than what could be listed here\n\n[15:37] <a href="https://youtu
 .be/cqK18-O3ptA?t=937">Can you get better constraints on curvature using F
 RBs?</a>\n\n[17:24] <a href="https://youtu.be/cqK18-O3ptA?t=1004">Dispersi
 on Measure of the IGM as a function of z</a>\n\n[18:40] <a href="https://y
 outu.be/cqK18-O3ptA?t=1120">Contributions to DM</a>\n\n[21:33] <a href="ht
 tps://youtu.be/cqK18-O3ptA?t=1293">DM(z) can shed light on the "missing ba
 ryon problem"</a>: paper reference - A census of baryons in the Universe f
 rom localized fast radio bursts\, <a href="https://arxiv.org/abs/2005.1316
 1">2005.13161</a> \n\n[23:26] <a href="https://youtu.be/cqK18-O3ptA?t=1406
 ">Tribute to Jean-Pierre Macquart\, first author of 2005.13161\, who recen
 tly passed</a>\n\n[24:04] <a href="https://youtu.be/cqK18-O3ptA?t=1444">Co
 mments on the 2005.13161 paper</a>: "all the baryons in the IGM that we co
 uldn't find\, so to speak\, are found by these FRBs\, an absolutely stunni
 ng result... when we wrote this paper (<a href="https://arxiv.org/abs/1909
 .02821">1909.02821</a>) last year showing that this could be theoretically
  done\, it hadn't occurred to me how quickly it <i>would</i> be done. The 
 rapid evolution in this field is fantastic." Includes an illustrative\, sh
 ort video.\n\n[26:15] <a href="https://youtu.be/cqK18-O3ptA?t=1575">Four l
 ocalised FRBs and what is known about them</a>: new paper by <a href="http
 s://https://iopscience.iop.org/article/10.3847/2041-8213/ab672e">Bhandari 
 et al.</a>\; much of the discussion is about the fact they all are at the 
 edge of their host galaxies\n\n[31:20] <a href="https://youtu.be/cqK18-O3p
 tA?t=1880"><b>H</b>ydrogen <b>I</b>ntensity and <b>Real</b> time <b>A</b>n
 alysis e<b>X</b>periment (HIRAX)</a>: similar to CHIME\, "it's a BAO inten
 sity mapping experiment that has FRBs as one of its science cases"\n\n[33:
 15] <a href="https://youtu.be/cqK18-O3ptA?t=1993">"South Africa has made a
  really strong case for radio astronomy"</a>\n\n[34:16] <a href="https://y
 outu.be/cqK18-O3ptA?t=2052">Prototype Array and Outriggers</a>\n\n[34:46] 
 <a href="https://youtu.be/cqK18-O3ptA?t=2086">Localising FRBs</a>\n\n[35:1
 6] <a href="https://youtu.be/cqK18-O3ptA?t=2116">Lessons from FRBs</a>\n\n
 [35:41] <a href="https://youtu.be/cqK18-O3ptA?t=2141">Q&A: Where to next? 
 (from the viewpoint of a theoretical cosmologist)</a>\n\n[36:15] <a href="
 https://youtu.be/cqK18-O3ptA?t=2205">The FRB Catalogue\, and the FRB Theor
 y Wiki</a>: references - (a) <a href="http://frbcat.org">frbcat.org</a> an
 d (b) <a href="https://frbtheorycat.org">frbtheorycat.org</a> (paper - FRB
 CAT: The Fast Radio Burst Catalogue\, <a href="https://arxiv.org/abs/1601.
 03547">1601.03547</a>)\n\n[38:04] <a href="https://youtu.be/cqK18-O3ptA?t=
 2284">Q&A: What are some things not yet mentioned where the community shou
 ld work out what things to look into right away?</a>\n\n[43:43] <a href="h
 ttps://youtu.be/cqK18-O3ptA?t=2623">The importance of priors</a>\n\n[47:36
 ] <a href="https://youtu.be/wawsmQ2SZvA?t=2856">Outside of your own resear
 ch\, what do you think is the most interesting thing in cosmology at the m
 oment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/13/
END:VEVENT
BEGIN:VEVENT
SUMMARY:José Luis Bernal (Johns Hopins University)
DTSTART:20200619T060000Z
DTEND:20200619T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/14
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/14/">How to tell if your cosmological approximations are accurate</a>\n
 by José Luis Bernal (Johns Hopins University) as part of Cosmology Talks\
 n\n\nAbstract\nJose tells us about how we can make sure our predictions fr
 om cosmology models can be both precise *and* accurate.\n\n<a href="https:
 //www.youtube.com/watch?v=wawsmQ2SZvA">Video of talk</a>\n\nPaper1: <a hre
 f="https://arxiv.org/abs/2005.10384">[2005.10384] Beware of commonly used 
 approximations I: errors in forecasts</a>\, by Nicola Bellomo\, José Luis
  Bernal\, Giulio Scelfo\, Alvise Raccanelli\, Licia Verde\n\nPaper2: <a hr
 ef="https://arxiv.org/abs/2005.09666">[2005.09666] Beware of commonly used
  approximations II: estimating systematic biases in the best-fit parameter
 s</a>\, byJosé Luis Bernal\, Nicola Bellomo\, Alvise Raccanelli\, Licia V
 erde\n\n<a href="https://github.com/nbellomo/Multi_Class">Modified CLASS c
 ode</a>\n\n<a href="https://www.youtube.com/watch?v=WiTcAUXIUO4">Jose's ta
 lk from the <i>Cosmology from Home</i> conference</a>\n\n<hr>\n\n<b>Index 
 to Key Parts of the Talk:</b>\n\n[00:02] <a href="https://youtu.be/wawsmQ2
 SZvA?t=2">Shaun's intro to the topic and José's work</a>\n\n[01:14] <a hr
 ef="https://youtu.be/wawsmQ2SZvA?t=75">José's opening comments on his wor
 k and the topic papers</a>\n\n[02:20] <a href="https://youtu.be/wawsmQ2SZv
 A?t=140">Q&A: what are two simple things you'd want viewers to remember ab
 out this talk?</a>\n\n[03:24] <a href="https://youtu.be/wawsmQ2SZvA?t=204"
 >Background details on the motivations for this work</a>\n\n[06:15] <a hre
 f="https://youtu.be/wawsmQ2SZvA?t=375">Shaun draws parallels to an earlier
  Kit Gallagher talk</a>\n\n[06:50] <a href="https://youtu.be/wawsmQ2SZvA?t
 =410">Start of José's slides and intro comments on the two papers</a>\n\n
 [07:32] <a href="https://youtu.be/wawsmQ2SZvA?t=452">From the Precision Er
 a to the Accuracy Era</a>: very different concepts\; comments on observati
 onal and theoretical systematics\, statistical uncertainties\; importance 
 of blind analysis\; two outcomes of systematic errors: bias (shift in the 
 posterior)\, misestimation (change in the shape of the posterior)\; recomm
 endation to use methodology of 1803.04470 (Bernal & Peacock) if you want t
 o be conservative\n\n[13:20] <a href="https://youtu.be/wawsmQ2SZvA?t=800">
 Estimating bias in parameters</a>\n\n[17:20] <a href="https://youtu.be/waw
 smQ2SZvA?t=1040">Case example: Galaxy Clustering</a>\n\n[21:34] <a href="h
 ttps://youtu.be/wawsmQ2SZvA?t=1294">Quick summary on nongaussianity\, then
  continuing on galaxy clustering</a>\n\n[24:07] <a href="https://youtu.be/
 wawsmQ2SZvA?t=1447">Case example 1: Cosmic magnification</a>\n\n[30:54] <a
  href="https://youtu.be/wawsmQ2SZvA?t=1854">Exploring 2D biases</a>\n\n[33
 :51] <a href="https://youtu.be/wawsmQ2SZvA?t=2031">Case example 2: Limber 
 Approximation</a>\n\n[36:54] <a href="https://youtu.be/wawsmQ2SZvA?t=2214"
 >Multi-tracer Analysis</a>: can be calculated thanks to the Multi_CLASS co
 de</a>\n\n[42:04] <a href="https://youtu.be/wawsmQ2SZvA?t=2524">Conclusion
 s</a>\n\n[43:50] <a href="https://youtu.be/wawsmQ2SZvA?t=2630">Where to ne
 xt?</a>\n\n[44:42] <a href="https://youtu.be/wawsmQ2SZvA?t=2682">Shaun's h
 ope for an eventual 'central repository' of summarized information or 'cos
 mology wiki'</a>\n\n[47:36] <a href="https://youtu.be/wawsmQ2SZvA?t=2856">
 Outside of your own research\, what do you think is the most interesting t
 hing in cosmology at the moment</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/14/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Natalia Porqueres (Imperial College London)
DTSTART:20200703T060000Z
DTEND:20200703T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/15
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/15/">You can get 3D info from quasar Lyman-α absorption lines using fo
 rward modelling</a>\nby Natalia Porqueres (Imperial College London) as par
 t of Cosmology Talks\n\n\nAbstract\nNatalia speaks about forward modelling
  in the context of Lyman-α absorption lines of quasar spectra. Forward mo
 delling essentially takes the initial conditions from your early universe 
 model and evolves them forward to give the full observational prediction o
 f all measurable things\, for those specific initial conditions.\n\nThis i
 s different to\, e.g.\, having a "summary statistic" of this full set of i
 nitial conditions and/or observations that you extract to constrain your m
 odel. An example of a summary statistic might be a bispectrum in the late 
 universe. The bispectrum captures some of the information lost from the po
 wer spectrum due to non-linearity\, but not all. Whereas\, in principle\, 
 if the forward modelling is done precisely enough no information is lost.\
 n\nOf course "done precisely enough" is the crucial phrase and forward mod
 elling needs to balance precision with speed. The more common summary stat
 istics methods are usually much\, much faster than forward modelling.\n\nS
 o\, Natalia presents a new method for evolving non-linearities faster\, on
 e that in particular does a much better job at capturing under-densities t
 han the typical particle-mesh codes. She also shows that this forward mode
 lling technique is able to extract\, statistically\, information about the
  3D regions between absorption lines because it uses the full set of (corr
 elated) initial conditions as its set of model parameters.\n\nTalk video: 
 <a href="https://youtu.be/eBQv5gRs2y8">youtu.be/eBQv5gRs2y8</a>\n\nPaper: 
 <a href="https://arxiv.org/abs/2005.12928">[2005.12928] A hierarchical fie
 ld-level inference approach to reconstruction from sparse Lyman-α forest 
 data</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>\n\n[00:00] <a h
 ref="https://youtu.be/eBQv5gRs2y8">Shaun's intro to this forward modelling
  topic and Natalia's work</a>\n\n[01:19] <a href="https://youtu.be/eBQv5gR
 s2y8?t=79">Natalia's summary of the 2005.12928 paper</a>: inferring the da
 rk matter distribution from the Lyman-α forest\; improved method introduc
 es a field-based approach to describe the DM dynamics\, more accurate in d
 escription of the voids and under-densities\n\n[02:33] <a href="https://yo
 utu.be/eBQv5gRs2y8?t=153">Q&A: what are two simple things you'd want viewe
 rs to remember about this talk?</a>: it's possible to infer 3D information
  from the Lyman-α forest\, and a field-based approach to describe the DM 
 dynamics has some advantages over the more standard particle-based approac
 h \n\n[03:54] <a href="https://youtu.be/eBQv5gRs2y8?t=234">Q&A: the motiva
 tion for this work</a>\n\n[06:55] <a href="https://youtu.be/eBQv5gRs2y8?t=
 415">(1) collaborators\, and (2) this work was carried out within the Aqui
 la Consortium</a>\n\n[07:13] <a href="https://youtu.be/eBQv5gRs2y8?t=433">
 First slide: Forward modelling approach</a>: visual description of the tec
 hnique\; initial conditons => dynamical model => data model => compare to 
 real data\n\n[09:55] <a href="https://youtu.be/eBQv5gRs2y8?t=595">From dat
 a to cosmology</a>\n\n[11:20] <a href="https://youtu.be/eBQv5gRs2y8?t=680"
 >Data model</a>: fluctuating Gunn-Peterson approximation\n\n[14:23] <a hre
 f="https://youtu.be/eBQv5gRs2y8?t=863">The BORG framework</a>: Gaussian pr
 ior => dynamical model => data model \n\n[16:15] <a href="https://youtu.be
 /eBQv5gRs2y8?t=975">Propagator Perturbation Theory (PPT): an alternative t
 o particles</a>: recently developed semiclassical analogue to Lagrangian p
 erturbation theory (LPT)\n\n[20:53] <a href="https://youtu.be/eBQv5gRs2y8?
 t=1253">Comparison LPT and PPT</a>\n\n[22:20] <a href="https://youtu.be/eB
 Qv5gRs2y8?t=1340">Statistical modular framework</a>\n\n[23:23] <a href="ht
 tps://youtu.be/eBQv5gRs2y8?t=1403">Hierarchical annealing with PPT</a>\n\n
 [24:41] <a href="https://youtu.be/eBQv5gRs2y8?t=1481">Testing the method w
 ith mock data</a>\n\n[26:42] <a href="https://youtu.be/eBQv5gRs2y8?t=1602"
 >Interpolation between lines-of-sight</a>\n\n[27:34] <a href="https://yout
 u.be/eBQv5gRs2y8?t=1654">Posterior matter power spectrum</a>\n\n[28:13] <a
  href="https://youtu.be/eBQv5gRs2y8?t=1693">Cluster mass profile</a>\n\n[2
 8:48] <a href="https://youtu.be/eBQv5gRs2y8?t=1728">Void profiles</a>: app
 lication - constraint on total neutrino mass\n\n[29:15] <a href="https://y
 outu.be/eBQv5gRs2y8?t=1755">Constraining cosmological parameters</a>\n\n[3
 1:14] <a href="https://youtu.be/eBQv5gRs2y8?t=1874">Velocity field at z > 
 2</a>\n\n[31:47] <a href="https://youtu.be/eBQv5gRs2y8?t=1907">Matter flow
 </a>\n\n[32:12] <a href="https://youtu.be/eBQv5gRs2y8?t=1932">Summary</a>\
 n\n[33:33] <a href="https://youtu.be/eBQv5gRs2y8?t=2013">Q&A: next steps</
 a>\n\n[35:06] <a href="https://youtu.be/eBQv5gRs2y8?t=2106">Q&A: outside o
 f your own research\, what do you think is the most interesting thing in c
 osmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/15/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Benjamin Giblin (University of Edinburgh)
DTSTART:20200711T060000Z
DTEND:20200711T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/16
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/16/">What is KiDS-1000? And why we can trust its results!</a>\nby Benja
 min Giblin (University of Edinburgh) as part of Cosmology Talks\n\n\nAbstr
 act\nBen Giblin tells us about the in-process KiDS-1000 results release. A
 t the time this video is released the collaboration have satisfied themsel
 ves that their data is robust and passes all relevant consistency checks\,
  but haven't yet released any cosmological results. \n\nIn fact\, their co
 smological results are still blinded\, but the consistency remains for all
  possible unblinded results. So whatever the results are\, they're consist
 ent.\n\nI'm not an observer\, but I found Ben's discussion of things like 
 "point spread functions" and "shear ratio null tests" to be very clear and
  understandable - in fact much\, much clearer than what I'm used to from t
 alks like this 😅.\n\nPaper: <a href="https://arxiv.org/abs/2007.01845">
 [2007.01845] KiDS-1000 catalogue: weak gravitational lensing shear measure
 ments</a>\n\nPaper on redshift measurements using self organised maps: <a 
 href="https://arxiv.org/abs/1909.09632">arxiv.org/abs/1909.09632</a>\n\n<h
 r>\n\n<b>Index to Key Parts of the Talk:</b>\n\n[00:01] <a href="https://y
 outu.be/r_hMWpl6xd0?t=1">Shaun's intro to the topic and Ben's work</a>\n\n
 [00:54] <a href="https://youtu.be/r_hMWpl6xd0?t=54">Ben's opening comments
  on this work</a>: series of tests\; modeling of the point spread function
 \; redshift distributions\; some new findings\n\n[03:01] <a href="https://
 youtu.be/r_hMWpl6xd0?t=181">Q&A: what are two simple things you'd want vie
 wers to remember about this talk?</a>: (1) the new data release has gone t
 hrough a lot of rigorous testing and found to be robust\, and (2) don't ju
 st copy the equations in other papers without proving them to yourself\n\n
 [03:29] <a href="https://youtu.be/r_hMWpl6xd0?t=209">Q&A: what is the moti
 vation for this work?</a>: measure cosmological parameters from the weak l
 ensing signal: cosmic shear\, galaxy-galaxy lensing\, and galaxy clusterin
 g\; the benefits of weak lensing as a low redshift probe in comparison to 
 Planck as a very high redshift probe\n\n[06:13] <a href="https://youtu.be/
 r_hMWpl6xd0?t=373">The details of KiDS-1000 and Ben's recent paper</a>: Ki
 DS-North and KiDS-South\; improvements on this data since the previous dat
 a release: photometric redshift calibration\; paper references below are t
 o the first paper that has come out as of the date of this talk: <a href="
 https://arxiv.org/abs/2007.01845">[2007.01845] KiDS-1000 catalogue: weak g
 ravitational lensing shear measurements</a>\n\n[08:14] <a href="https://yo
 utu.be/r_hMWpl6xd0?t=494">Table comparing 3 surveys: KiDS\, DES\, and HSC<
 /a>\n\n[08:46] <a href="https://youtu.be/r_hMWpl6xd0?t=526">Weak lensing c
 osmology: the state of play</a>: KiDS measures a lower S8 than the other 2
  surveys\; tension between KiDS and Planck ~2.5σ\; comments on other pape
 rs\;  this tension with Planck disappears if KiDS uses COSMOS2015\, which 
 is used by DES and HSC to calibrate their redshifts\; ongoing debate\n\n[1
 3:42] <a href="https://youtu.be/r_hMWpl6xd0?t=822">KiDS-1000: How to make 
 sure our shear and redshift estimates are accurate</a>: Null tests of the 
 PSF modelling\; Null-tests of the joint shear and redshift data\n\n[14:16]
  <a href="https://youtu.be/r_hMWpl6xd0?t=856">PSF Modelling</a>: the "effe
 ctive PSF" describes how the light of a point source would spread out due 
 to atmospheric\, telescope\, and camera effects\; the challenge of weak le
 nsing\; how it's modelled\; comments on Fig. 2 of paper\n\n[18:00] <a href
 ="https://youtu.be/r_hMWpl6xd0?t=1080">PSF Modelling is hard</a>: details 
 on 3 different prescriptions in the literature\; caution on 2 & 3  potenti
 ally biasing cosmological inference (e.g.\, S8)\; correlation functions co
 mments\n\n[23:20] <a href="https://youtu.be/r_hMWpl6xd0?t=1400">First-orde
 r PSF Systematics Model</a>\n\n[26:24] <a href="https://youtu.be/r_hMWpl6x
 d0?t=1584">Flux/spatial dependent PSF systematics model</a>: accounting fo
 r imperfections in the CCD chips (section 3.4.1 in paper\, Fig. 4)\n\n[29:
 29] <a href="https://youtu.be/r_hMWpl6xd0?t=1769">PSF modelling takeaways<
 /a>\n\n[30:08] <a href="https://youtu.be/r_hMWpl6xd0?t=1808">Tests of the 
 joint shear-redshift data</a>\n\n[30:28] <a href="https://youtu.be/r_hMWpl
 6xd0?t=1828">Galaxy-Galaxy Lensing (GGL)</a>: how shapes of background gal
 axies are correlated with positions of foreground lensing galaxies\; typic
 ally causes a tangential shear pattern\n\n[30:55] <a href="https://youtu.b
 e/r_hMWpl6xd0?t=1855">Using GGL to detect additive systematics in the shea
 r</a>: see section 4.2 in paper\, Fig. 10\; a new test that they advocate\
 n\n[34:10] <a href="https://youtu.be/r_hMWpl6xd0?t=2050">GGL to test the j
 oint shear-redshift measurements</a>\; comments on Fig. 11 of paper\n\n[39
 :14] <a href="https://youtu.be/r_hMWpl6xd0?t=2354">Shear-Redshift Null-Tes
 t Takeaways</a>\n\n[39:30] <a href="https://youtu.be/r_hMWpl6xd0?t=2370">M
 ain Takeaways</a>: 3 points but one wasn't mentioned earlier: this is a ne
 at example of a blind paper - 3 versions of the data\, one is the true dat
 a\, other 2 are fake but derived from original data and modified\; see red
  comments in the paper for blinding details\; cosmological constraints wil
 l soon be released both from cosmic shear and 3x2pt cosmological analyses\
 n\n[42:46] <a href="https://youtu.be/r_hMWpl6xd0?t=2566">Q&A: Next Steps</
 a>\n\n[45:00] <a href="https://youtu.be/r_hMWpl6xd0?t=2700">Q&A: outside o
 f your own research\, what do you think is the most interesting thing in c
 osmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/16/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Simon Birrer (Stanford)
DTSTART:20200716T060000Z
DTEND:20200716T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/17
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/17/">TDCOSMO H0 results with more data and fewer approximations</a>\nby
  Simon Birrer (Stanford) as part of Cosmology Talks\n\n\nAbstract\nSimon t
 ells us about the strong lensing time delay measurements of the Hubble con
 stant performed by TDCOSMO. \n\nIn the recent paper he has relaxed assumpt
 ions about the density profiles around the lenses. Specifically\, in this 
 analysis it is no longer assumed that the density follows a power law\, or
  NFW profile. This naturally widens the error bars on the measurement beca
 use the "mass sheet degeneracy" is no longer pinned down.\n\nIn order to p
 in this degeneracy back down they use kinematic data from the lenses to mo
 del the density profile. They also calibrate their model on an additional 
 external data set of strong lenses. When using just TDCOSMO lenses the cen
 tral value stays the same\, but when adding the new "SLACS" lenses\, the m
 easured value of H0 drops to be almost exactly the same as the Planck valu
 e. Cat\, meet pigeons.\n\nSimon also goes into what the future will look l
 ike and what data is needed to bring the accuracy of TDCOSMO back to what 
 it was before these assumptions were relaxed.\n\nSimon: https://sibirrer.g
 ithub.io/\nThe paper: https://arxiv.org/abs/2007.02941\nThe analysis pipel
 ine: https://github.com/TDCOSMO/hierarchy_analysis_2020_public\n\n<hr>\n\n
 <b>Index to Key Parts of the Talk:</b>\n\n00:00 <a href="https://youtu.be/
 QrdqbZv_tBs?t=0">Shaun's introduction</a>\n\n01:23 <a href="https://youtu.
 be/QrdqbZv_tBs?t=83">Simon's opening comments</a>:  the key that I want pe
 ople to take away from this paper is not the numbers themselves but the me
 thodology and the possibility to add new data\; there is a huge potential 
 on how we can utilize this type of framework to move forward \n\n02:53 <a 
 href="https://youtu.be/QrdqbZv_tBs?t=173">Q&A: is there another take away 
 message from this talk that you'd like to mention?</a>\n\n04:44 <a href="h
 ttps://youtu.be/QrdqbZv_tBs?t=284">Time-delay cosmography</a>: equation co
 mponents\; geometric quantities\; if source is variable\, there is a "time
 -delay" between the multiple images\; this method provides a physical anch
 or of the scales at intermediate redshifts\, independent of CMB and distan
 ce ladder\; delay is from a few days to a few months (110 days is longest 
 in current sample)   \n\n06:59 <a href="https://youtu.be/QrdqbZv_tBs?t=419
 ">TDCOSMO project</a>: new collaboration of H0LiCOW + STRIDES + SHARP + CO
 SMOGRAIL projects\; 7 lenses analyzed to date\n\n07:55 <a href="https://yo
 utu.be/QrdqbZv_tBs?t=475">Single lens - multiple data</a>: basic ingredien
 ts: high resolution imaging to measure and describe in detail the distorti
 on of the lensing effect\; time delay measurements\; stellar kinematics\; 
 line of sight contribution\; different telescopes involved\n\n10:31 <a hre
 f="https://youtu.be/QrdqbZv_tBs?t=631">Forward modeling in action</a>: rec
 onstruct lensing phenomena from the imaging data\n\n11:02 <a href="https:/
 /youtu.be/QrdqbZv_tBs?t=662">Previous results from the H0LiCOW collaborati
 on</a>: 6 lenses\; blind analysis for all except first\; question on obser
 ved trend of decreasing H0 with increased redshift\n\n12:57 <a href="https
 ://youtu.be/QrdqbZv_tBs?t=777">H0 measurements in flat ΛCDM - performed b
 lindly</a>\n\n13:59 <a href="https://youtu.be/QrdqbZv_tBs?t=837">mass-shee
 t degeneracy</a>: see  Fig. A.1 and section 2 of paper\n\n15:44 <a href="h
 ttps://youtu.be/QrdqbZv_tBs?t=944">TDCOSMO IV: Hierarchical time-delay cos
 mography - joint inference of the Hubble constant and galaxy density profi
 les</a>\n\n16:01 <a href="https://youtu.be/QrdqbZv_tBs?t=961">Velocity dis
 persion measurements of the deflector galaxy can break the mass-sheet dege
 neracy</a>: summary of added data\; Fig. 4 in paper\n\n16:58 <a href="http
 s://youtu.be/QrdqbZv_tBs?t=1018">Constraining galaxy density profiles with
  lensing and kinematics</a>: SLACS lenses\; have excellent imaging from HS
 T and kinematics from BOSS spectra\n\n17:23 <a href="https://youtu.be/Qrdq
 bZv_tBs?t=1043">Question and discussion on the assumptions</a>\n\n19:02 <a
  href="https://youtu.be/QrdqbZv_tBs?t=1142">Returning to discussion on the
  slides</a>: Fig. 12\, 13b\, 14\, & 17 in paper\n\n26:22 <a href="https://
 youtu.be/QrdqbZv_tBs?t=1582">Q&A on details of the modeling</a>\n\n30:29 <
 a href="https://youtu.be/QrdqbZv_tBs?t=1829">More discussion on the mass-s
 heet degeneracy slide</a>\n\n33:51 <a href="https://youtu.be/QrdqbZv_tBs?t
 =2031">Next steps</a>: Fig. 18 from paper\n\n34:34 <a href="https://youtu.
 be/QrdqbZv_tBs?t=2074">Way forward 1: data on time delay lenses</a>\n\n35:
 40 <a href="https://youtu.be/QrdqbZv_tBs?t=2140">Way forward 2: adding ext
 ernal data sets</a>\n\n36:44 <a href="https://youtu.be/QrdqbZv_tBs?t=2204"
 >Way forward 3: challenge yourself</a>\n\n38:40 <a href="https://youtu.be/
 QrdqbZv_tBs?t=2320">What is the prognosis for TDCOSMO precision?</a>: opti
 mistic that within a year can get back down to 3% uncertainty\n\n39:07 <a 
 href="https://youtu.be/QrdqbZv_tBs?t=2347">Q&A: What do you expect will be
  the resolution to the H0 issue?</a>\n\n40:27 <a href="https://youtu.be/Qr
 dqbZv_tBs?t=2426">Q&A: outside of your own research\, what do you think is
  the most interesting thing in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/17/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Eva-Maria Mueller (Oxford)
DTSTART:20200720T060000Z
DTEND:20200720T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/18
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/18/">Even BAO alone requires dark energy + cosmology from the last eBOS
 S data release</a>\nby Eva-Maria Mueller (Oxford) as part of Cosmology Tal
 ks\n\n\nAbstract\nEva-Maria tells us about the cosmological results from t
 he final (cosmology relevant) SDSS/eBOSS data release. eBOSS is a spectros
 copic galaxy survey\, precisely mapping galaxies\, quasars and the Lyman-
 α forest.\n\nThe two key probes are baryon acoustic oscillations (BAO) an
 d redshift space distortions (RSD). BAO acts as a distance ladder\, and eB
 OSS now has measurements of BAO at enough redshifts that their data alone 
 constrains the expansion history of the universe precisely enough to prove
  the existence of a dark energy component. The RSD measurements probe the 
 growth of structure\, but are unable to resolve any tension between weak l
 ensing measurements and the CMB\, with their results lying right between t
 he two alternatives\, consistent with both.\n\nThe distance scale in BAO c
 an also be anchored using constraints from big bang nucleosynthesis (BBN) 
 allowing eBOSS to infer the expansion rate of the universe today without r
 eference to the CMB. Their measurement is consistent with the CMB and inco
 nsistent with the local distance ladder measurements (e.g. SH0ESS).\n\nThe
  BAO\, RSD and CMB are all consistent with the time evolution of the (unan
 chored) supernovae so all these data sets can be combined to give an overa
 ll constraint. This gives very tight bounds on any deviations from a cosmo
 logical constant in ΛCDM\, and on any deviations from a flat geometry wit
 hin our observable universe.\n\nThe next stage in spectroscopic surveys is
  DESI\, and then Euclid. COVID permitting\, we should have the first resul
 ts from DESI within three years.\n\n<a href="https://www2.physics.ox.ac.uk
 /contacts/people/muellere">Eva-Maria's Oxford page</a> \n\nThe paper: <a h
 ref="https://arxiv.org/abs/2007.08991">[2007.08991]The Completed SDSS-IV e
 BOSS: Cosmological Implications from two Decades of Spectroscopic Surveys 
 at the Apache Point observatory</a>\n\n<hr>\n\n<b>Index to Key Parts of th
 e Talk:</b>\n\n00:00 <a href="https://www.youtube.com/watch?v=S9PL1Heis5E"
 >Shaun's introduction</a>\n\n00:37 <a href="https://youtu.be/S9PL1Heis5E?t
 =37">Eva-Maria's opening comments on the paper</a>\n\n01:28 <a href="https
 ://youtu.be/S9PL1Heis5E?t=88">Q&A: what are two simple things you'd want v
 iewers to remember about this talk?</a>\n\n03:24 <a href="https://youtu.be
 /S9PL1Heis5E?t=204">1st slide: Cosmological results from 20 years of SDSS 
 redshift surveys</a>: different SDSS components\n\n05:31 <a href="https://
 youtu.be/S9PL1Heis5E?t=331">Sky coverage of eBOSS</a>: all of the data was
  taken with the 2.5m Sloan Telescope in the Apache Point Observatory in Ne
 x Mexico\n\n06:18 <a href="https://youtu.be/S9PL1Heis5E?t=378">What BAO is
  and how it's being using</a>: 1st main observable\; a preferred scale in 
 the clustering and distribution of galaxies that can be used as a standard
  ruler\n\n06:43 <a href="https://youtu.be/S9PL1Heis5E?t=403">Redshift-Spac
 e Distortions</a>: 2nd main observable\; gives the growth rate of structur
 e and is sensitive to the theory of gravity \n\n07:31 <a href="https://you
 tu.be/S9PL1Heis5E?t=451">A journey of firsts</a>: SDSS made 1st detection 
 of BAO signal in 2005\; BAO bump\n\n08:11 <a href="https://youtu.be/S9PL1H
 eis5E?t=491">BOSS had 1st detection of the BAO signal in the distribution 
 of neutral hydrogen from LyA forest in 2013</a>: also in the distribution 
 of quasars in 2017\n\n08:28 <a href="https://youtu.be/S9PL1Heis5E?t=508">Q
 &A discussion on the size and location of the peak</a>: template fitting\n
 \n08:58 <a href="https://youtu.be/S9PL1Heis5E?t=538">SDSS BAO Distance Lad
 der</a>\n\n09:47 <a href="https://youtu.be/S9PL1Heis5E?t=587">The growth o
 f structure</a>: comparison with Planck 2018 ΛCDM best-fit model\n\n10:26
  <a href="https://youtu.be/S9PL1Heis5E?t=626">The 23-paper release</a>: th
 is talk focused on what is learned about expansion of universe\, curvature
 \, mass of neutrinos\, taking the measurements and transforming them into 
 constraints of cosmological parameters\n\n11:12 <a href="https://youtu.be/
 S9PL1Heis5E?t=672">Dark Energy</a>: Takeaway - a significant detection of 
 DE with only BAO data\n\n13:07 <a href="https://youtu.be/S9PL1Heis5E?t=787
 ">Curvature</a>: CMB by itself has large degeneracy between curvature and 
 matter\; adding SN gives improvement but still can't tell for sure\; can n
 ail it down by adding BAO\, shows to high precision the universe is flat \
 n\n14:09 <a href="https://youtu.be/S9PL1Heis5E?t=849">What is the nature o
 f Dark Energy?</a>: combining different data sets supports the flat ΛCDM 
 model with constant DE \n\n16:21 <a href="https://youtu.be/S9PL1Heis5E?t=9
 81">Hubble Parameter Tension</a>\n\n17:03 <a href="https://youtu.be/S9PL1H
 eis5E?t=1023">Summary diagrams\, step-by-step going through the different 
 contours</a>\n\n18:49 <a href="https://youtu.be/S9PL1Heis5E?t=1129">Combin
 ation of BAO+BBN breaks degeneracy compared to BAO by itself</a>: clear te
 nsion with distance ladder H0 measurement\; BAO+BBN (using no CMB info) in
  good agreement with CMB\n\n19:48 <a href="https://youtu.be/S9PL1Heis5E?t=
 1188">allowing DE EoS to vary and combining CMB+BAO+SN (inverse distance l
 adder) gives H0 in agreement with CMB by itself</a>: DE is not an explanat
 ion for H0 tension\n\n21:35 <a href="https://youtu.be/S9PL1Heis5E?t=1295">
 Can rephrase H0 tension as a sound horizon tension</a>\n\n23:14 <a href="h
 ttps://youtu.be/S9PL1Heis5E?t=1394">The BAO analysis is robust</a>: hard t
 o come up with a systematic that would coherently move galaxies in a way t
 hat wouldn't move the position of the BAO bump\n\n23:50 <a href="https://y
 outu.be/S9PL1Heis5E?t=1430">sigma8 - Omega_m Discrepancy</a>: Fig. 9a in p
 aper\; results just from RSD\n\n25:52 <a href="https://youtu.be/S9PL1Heis5
 E?t=1552">Comparing full data sets - SDSS\, DES\, Planck</a>\n\n26:59 <a h
 ref="https://youtu.be/S9PL1Heis5E?t=1619">Constraint on sum of the neutrin
 o masses</a>: Fig. 13 in paper\; Planck + BAO + RSD + SN constraints is ri
 ght at minimum edge for IH but not significant enough to rule out IH (thou
 gh IH becoming less and less likely\; more data needed)\n\n29:47 <a href="
 https://youtu.be/S9PL1Heis5E?t=1787">20 years of cosmology</a>: summary of
  galaxy spectroscopic surveys\; Fig. 14 in paper\n\n31:50 <a href="https:/
 /youtu.be/S9PL1Heis5E?t=1910">Conclusion: Legacy of BOSS/eBOSS</a>\n\n32:5
 5 <a href="https://youtu.be/S9PL1Heis5E?t=1975">Q&A: Is it valid to combin
 e SN with BAO and CMB?</a>\n\n34:53 <a href="https://youtu.be/S9PL1Heis5E?
 t=2093">Q&A: Where to next? What is coming with Stage IV?</a>: DESI and Eu
 clid for spectroscopy\; other things DESI can look at\; CMB-S4\; LSST (Ver
 a C. Rubin Observatory)\n\n38:38 <a href="https://youtu.be/S9PL1Heis5E?t=2
 318">Q&A: outside of your own research\, what do you think is the most int
 eresting thing in cosmology at the moment?</a>\n\nSupplemental info: <a hr
 ef="https://www.sdss.org/science/cosmology-results-from-eboss/">One-page s
 ummary of the cosmology results and implications at the SDSS website</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/18/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Simone Aiola (Flatiron CCA and Simons Observatory\, Atacama)
DTSTART:20200805T060000Z
DTEND:20200805T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/19
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/19/">ACT+WMAP is as powerful as Planck\; CMB results on ΛCDM are robus
 t</a>\nby Simone Aiola (Flatiron CCA and Simons Observatory\, Atacama) as 
 part of Cosmology Talks\n\n\nAbstract\nSimone talks about the latest Ataca
 ma Cosmology Telescope cosmology paper(s). He goes into detail at the begi
 nning about the history of ACT and where it is now\, as well as what data 
 was in the latest results. \n\nHe then goes into how the data has been che
 cked for robustness and how it is sufficiently consistent with WMAP to mot
 ivate combining the two data sets (i.e. WMAP for the large scales and ACT 
 for the small scales and polarisation). Combined\, WMAP and ACT are as con
 straining as Planck\, but don't add much additional constraining power whe
 n added to Planck (they do measure the same sky of course!).\n\nThe ACT po
 larisation data is sufficiently high in signal to noise that you can even 
 make maps of the data that look as clear as the Planck/WMAP temperature ma
 ps\, which is quite stunning.\n\nThen Simone goes into the final cosmologi
 cal results. Overall\, Planck and WMAP+ACT are mostly consistent. In parti
 cular\, their H0 predictions are very similar. There is a small amount of 
 tension that manifests as a different value of the spectral index (or\, mo
 re precisely\, in the ns vs omega_b constraint contours). This is only ~2.
 4 sigma\, so worth keeping an eye on\, but not worth getting too excited a
 bout yet.\n\nPapers: <a href="https://arxiv.org/abs/2007.07288">arxiv.org/
 abs/2007.07288</a> and <a href="https://arxiv.org/abs/2007.07289">arxiv.or
 g/abs/2007.07289</a>\n\nData: <a href="https://lambda.gsfc.nasa.gov/produc
 t/act/actpol_prod_table.cfm">lambda.gsfc.nasa.gov/product/act/actpol_prod_
 table.cfm</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>\n\n00:00 <
 a href="https://youtu.be/Ememq6FnN1U">Shaun's introduction</a>\n\n00:37 <a
  href="https://youtu.be/Ememq6FnN1U?t=37">Simone's opening comments</a>\n\
 n01:15 <a href="https://youtu.be/Ememq6FnN1U?t=75">Q&A: what are two simpl
 e things you'd want viewers to remember about this talk?</a>: combining WM
 AP large-scale and ACT small-scale data yields cosmological constraints at
  a precision comparable to Planck\; provides a ΛCDM cross-check independe
 nt of Planck\; Planck and ACT systematics likely very different\; results 
 found to be in agreement \n\n02:43 <a href="https://youtu.be/Ememq6FnN1U?t
 =163">Q&A: what is interesting about ACT that we couldn't just get from Pl
 anck?</a>: CMB secondaries and foregrounds are not possible to do with sma
 ller telescopes\n\n04:05 <a href="https://youtu.be/Ememq6FnN1U?t=245">Brie
 f comments highlighting the ACT Collaboration</a>\n\n04:42 <a href="https:
 //youtu.be/Ememq6FnN1U?t=282">Some details on the ACT telescope</a>: plot 
 showing ACT's resolution and sky area coverage compared to other CMB missi
 ons\n\n05:46 <a href="https://youtu.be/Ememq6FnN1U?t=346">ACT Datasets</a>
 : a brief overview of past\, current\, and future ACT datasets\; results p
 resented here are based on ACTPol data taken from 2013-2016\; ACTPol measu
 red polarization\, previous ACT versions did not\; ACT to continue observi
 ng through 2021\n\n06:46 <a href="https://youtu.be/Ememq6FnN1U?t=406">Deta
 ils on the 3 cameras</a>: cross-checks ability - slightly different optics
 \, different locations in the telescope\; data recorded at 98 and 150 GHz\
 n\n07:39 <a href="https://youtu.be/Ememq6FnN1U?t=459">Q&A on removing fore
 grounds</a>: higher frequency data from Planck used for detecting any dust
  contamination\, though it has no CMB component\; foreground contamination
  is small compared to CMB signal at the frequencies used by ACT\n\n09:19 <
 a href="https://youtu.be/Ememq6FnN1U?t=559">Shaun's post-recording edit wi
 th additional unrecorded comments by Simone about foreground removal</a>\n
 \n10:23 <a href="https://youtu.be/Ememq6FnN1U?t=623">ACT DR4 Survey</a>: t
 otal map-depth varies across the sky\; noise levels compared to Planck\; F
 ig. 4 (top panel) in 2007.07288\n\n11:32 <a href="https://youtu.be/Ememq6F
 nN1U?t=692">ACT temperature and E-mode polarization maps at z~1100</a>: tw
 o different points of view of the physics of the last scattering surface\;
  comparison with Planck measurements at different scales from ACT\n\n15:22
  <a href="https://youtu.be/Ememq6FnN1U?t=922">Regions for power spectra</a
 >: depth of the map variable across the sky\; "deep" and "wide" (shallower
 ) regions\; effective area\; Fig. 2\;  <b>NOTE:</b> Figure references are 
 for 2007.07289 unless otherwise indicated\n\n17:53 <a href="https://youtu.
 be/Ememq6FnN1U?t=1073">Power spectra at 98 & 150 GHz</a>: deep vs wide plo
 ts\; Fig. 10\n\n20:16 <a href="https://youtu.be/Ememq6FnN1U?t=1216">CMB-on
 ly power spectra</a>: wide patch errors bars on intermediate scales are sm
 aller than for deep (especially visible in EE)\, whereas the deep does wel
 l in constraining foregrounds\; Figs. 15 and 24\n\n21:54 <a href="https://
 youtu.be/Ememq6FnN1U?t=1314">Parameter-level tests</a>:  Fig. 14\; some of
  the cosmological parameters are being constrained better by TE than TT\; 
 no evidence of systematic effects\n\n23:49 <a href="https://youtu.be/Ememq
 6FnN1U?t=1429">ACT DR4 Cosmology</a>: triangular plot comparing WMAP\, Pla
 nck\, ACT in 5D parameter space (all 3 have a τ prior in common)\, Fig. 1
 2 in 2007.07288\; ACT vs WMAP/Planck consistent at 2.3-2.7σ\; two expecte
 d degeneracies  \n\n26:48 <a href="https://youtu.be/Ememq6FnN1U?t=1608">Co
 mbining ACT+WMAP (baseline) and ACT+Planck</a>: ACT+WMAP breaks some of de
 generacies that are in the 2 data sets independently\; Figs. 17 & 19 in 20
 07.07288\;  ACT shows a mild preference for less damping in the small-scal
 e power spectrum than in ΛCDM\; for more info on combining ACT+WMAP\, see
  section 6.2.2 in 2007.07288\n\n30:51 <a href="https://youtu.be/Ememq6FnN1
 U?t=1851">ACT DR4 H0 Estimate</a>: Fig. 18 in 2007.07288\n\n31:30 <a href=
 "https://youtu.be/Ememq6FnN1U?t=1890">ACT DR4 Cosmology beyond ΛCDM</a>: 
 Figs. 20\, 21\, 22 in 2007.07288\n\n32:53 <a href="https://youtu.be/Ememq6
 FnN1U?t=1973">A_lens finding (consistent with unity) and discussion</a>: F
 ig. 20 in 2007.07288\; also see section 7.1.1 in 2007.07288\n\n36:20 <a hr
 ef="https://youtu.be/Ememq6FnN1U?t=2180">ACT\, WMAP\, Planck</a>: Figs. 14
 \, 15 in 2007.07288\; ACT prefers a 2.4σ lower first peak in TT\, higher 
 TE\, lower EE\n\n40:02 <a href="https://youtu.be/Ememq6FnN1U?t=2402">ACT D
 R4 Publicly Released</a>: ~0.5TB of data products and 4.5TB of simulations
  available at <a href="https://lambda.gsfc.nasa.gov/product/act/actpol_pro
 d_table.cfm">lambda.gsfc.nasa.gov</a>\n\n40:18 <a href="https://youtu.be/E
 memq6FnN1U?t=2418">Q&A: What comes next?</a>\n\n42:44 <a href="https://you
 tu.be/Ememq6FnN1U?t=2564">Simons Observatory discussion</a>\n\n43:41 <a hr
 ef="https://youtu.be/Ememq6FnN1U?t=2621">Q&A: outside of your own research
 \, what do you think is the most interesting thing in cosmology at the mom
 ent?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/19/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Marika Asgari (University of Edinburgh)
DTSTART:20200921T060000Z
DTEND:20200921T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/20
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/20/">KiDS 1000 is statistics dominated and in 3σ tension with Planck c
 osmology</a>\nby Marika Asgari (University of Edinburgh) as part of Cosmol
 ogy Talks\n\n\nAbstract\nMarika tells us about the recent Kilo Degree Surv
 ey (KiDS) cosmological results. These are the first results from KiDS afte
 r they have reached 1000 square degrees.\n\nMarika first explains how they
  know that the results are "statistics dominated" and not "systematics dom
 inated"\, meaning that the dominant uncertainty comes from statistical err
 ors\, not systematic ones. \n\nShe then presents the cosmological results\
 , which primarily constrain the clumpiness of matter in the universe\, and
  which therefore constrain Ω_m and σ_8. In the combined parameter "S_8"\
 , which is constrained almost independently from Ω_m by their data they s
 ee a more than 3σ tension with the equivalent parameter one would infer f
 rom Planck.\n\nMarika's website: <a href="https://www.roe.ac.uk/~ma/">http
 s://www.roe.ac.uk/~ma/</a>\n\nPapers: <a href="https://arxiv.org/abs/2007.
 15632">2007.15632</a> and <a href="https://arxiv.org/abs/2007.15633">2007.
 15633</a>\n\n<a href=https://www.youtube.com/watch?v=kYkN6Yl8x6M">KiDS web
 inar</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>\n\n00:00 <a hre
 f="https://youtu.be/-o-u7A4QAyE?t=0">Shaun's introduction</a>\n\n00:40 <a 
 href="https://youtu.be/-o-u7A4QAyE?t=40">Marika's opening comments about t
 wo of the five recent KiDS papers</a>: also see the KiDS Key Facts segment
  beginning at 10:39\n\n01:24 <a href="https://youtu.be/-o-u7A4QAyE?t=84">Q
 &A: what are two things you'd want viewers to remember about this talk?</a
 >\n\n02:13 <a href="https://youtu.be/-o-u7A4QAyE?t=133">Q&A: what was the 
 motivation for this work?</a>: the strength of cosmic shear in general is 
 that it rather directly measures the amount of matter compared to surveys 
 that use galaxy positions\; KiDS is a unique survey in that there's a good
  handle on the systematics\; also see segment starting at 08:50\n\n03:12 <
 a href="https://youtu.be/-o-u7A4QAyE?t=192">Q&A: What was done and what ar
 e the results?</a> \n\n04:20 <a href="https://youtu.be/-o-u7A4QAyE?t=260">
 Cosmic shear 101</a> \n\n06:47 <a href="https://youtu.be/-o-u7A4QAyE?t=407
 ">Modeling</a> \n\n07:47 <a href="https://youtu.be/-o-u7A4QAyE?t=467">Blin
 ding</a> \n\n08:50 <a href="https://youtu.be/-o-u7A4QAyE?t=530">Standard c
 osmological model</a> \n\n10:39 <a href="https://youtu.be/-o-u7A4QAyE?t=63
 9">KiDS: Key Facts</a> \n\n11:32 <a href="https://youtu.be/-o-u7A4QAyE?t=6
 92">Results: comments on Fig. 5</a>: (all figure references are to 2007.15
 633 until discussion on the 2nd paper begins at 27:17)\n\n13:01 <a href="h
 ttps://youtu.be/-o-u7A4QAyE?t=781">Two point statistics and their scale se
 nsitivity</a>\n\n13:40 <a href="https://youtu.be/-o-u7A4QAyE?t=820">Commen
 ts on the 4 panels of Fig. 1 from 2007.15633</a>\n\n17:39 <a href="https:/
 /youtu.be/-o-u7A4QAyE?t=1059">"Headline plot"\, comments on Fig. 6</a>\n\n
 19:08 <a href="https://youtu.be/-o-u7A4QAyE?t=1148">The capital S8 paramet
 er</a>\n\n21:00 <a href="https://youtu.be/-o-u7A4QAyE?t=1260">Impact of nu
 isance parameters</a>: comments on Fig. 7\n\n25:40 <a href="https://youtu.
 be/-o-u7A4QAyE?t=1540">Comparison with Planck\, DES\, and HSC</a>: comment
 s on Fig. 9\n\n27:17 <a href="https://youtu.be/-o-u7A4QAyE?t=1637">Start o
 f discussion on 2nd paper\, 2007.15632</a>All following Figure references 
 from here are for 2007.15632)\n\n27:55 <a href="https://youtu.be/-o-u7A4QA
 yE?t=1675">Survey Footprint</a> \n\n28:30 <a href="https://youtu.be/-o-u7A
 4QAyE?t=1710">Figure 1: 3x2pt: Cosmic Shear +</a>\n\n29:15 <a href="https:
 //youtu.be/-o-u7A4QAyE?t=1755">Figure 2: 3x2pt: Cosmic Shear + Clustering 
 +</a>\n\n29:55 <a href="https://youtu.be/-o-u7A4QAyE?t=1815">Figure 3\, le
 ft panel:  3x2pt: Cosmic Shear + Clustering + Galaxy-Galaxy Lensing</a>\n\
 n32:47 <a href="https://youtu.be/-o-u7A4QAyE?t=1967">Figure 6\, right pane
 l: Consistency between probes</a>\n\n33:37 <a href="https://youtu.be/-o-u7
 A4QAyE?t=2017">Figure 4\, KiDS - Planck Tension Metrics</a>\n\n35:27 <a hr
 ef="https://youtu.be/-o-u7A4QAyE?t=2127">Figure 8\, Comparison with other 
 analyses</a>\n\n36:10 <a href="https://youtu.be/-o-u7A4QAyE?t=2170">Compar
 ison of KiDS core cosmology papers</a>\n\n37:13 <a href="https://youtu.be/
 -o-u7A4QAyE?t=2233">Q&A: What's the next big thing in photometric lensing 
 after what's currently happening?</a>\n\n38:44 <a href="https://youtu.be/-
 o-u7A4QAyE?t=2324">Q&A: What are you working on next?</a>\n\n39:18 <a href
 ="https://youtu.be/-o-u7A4QAyE?t=2358">Q&A: outside of your own research\,
  what do you think is the most interesting thing in cosmology at the momen
 t?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/20/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Bodo Schwabe and Mateja Gosenca (Göttingen U and U of Auckland)
DTSTART:20200929T050000Z
DTEND:20200929T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/21
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/21/">AxioNyx - Public code to simulate both Fuzzy and Cold Dark Matter 
 in hires | FDM≡CDM on large scales</a>\nby Bodo Schwabe and Mateja Gosen
 ca (Göttingen U and U of Auckland) as part of Cosmology Talks\n\n\nAbstra
 ct\nBodo Schwabe and Mateja Gosenca tell us about AxioNyx\, which is a new
  public code for simulating both Ultralight (or "Fuzzy") dark matter (FDM)
  and Cold dark matter (CDM) simultaneously. The code simulates the FDM usi
 ng adaptive mesh refinement and the CDM using N-body particles. As far as 
 I'm aware it is the first publicly available code that can do both without
  needing adaptation out of the tin (let me know in the YouTube page commen
 ts if I'm missing any codes - sorry :-/ ).\n\nThe code passes a bunch of s
 anity/consistency checks\, matching linear theory when it should match and
  deviating when it should deviate. The paper discussed mainly just introdu
 ces AxioNyx\; the new physics will come in future papers. Things Bodo\, Ma
 teja and collaborators will be tackling are: simulations with full cosmolo
 gical initial conditions for the combination of FDM+CDM\, adding baryons (
 long-term project)\, gravitational heating of stars in FDM halos\, and re-
 assessment of earlier constraints on FDM with FDM now only a sub-fraction 
 of the total dark matter content (e.g. the Lyman Alpha constraints). Stay 
 tuned\, and/or get in touch with them if you're keen to help make any of t
 hat happen :-).\n\nOne neat result from this paper was the confirmation of
  the "Schrodinger-Vlasov" correspondence. This essentially says that FDM a
 nd CDM will behave equivalently on large enough scales. On smaller scales 
 the fuzziness of the FDM causes it to deviate (essentially\, it is so ligh
 t that its deBroglie wavelength is astrophysically relevant). This corresp
 ondence has been shown statistically\, and as a limiting result\, in earli
 er papers but this is (as far as I'm aware) the first paper where the FDM 
 and CDM are in the same gravitational potentials in the same simulation an
 d one can see them do the same stuff on large scales. It wasn't surprising
 \, but it's still good to check and see it happen. \n\nThe most interestin
 g things happen when the proportions of FDM and CDM are similar (i.e. when
  one doesn't just dominate the other entirely)\, which might be an interes
 ting thing for considering in future papers too.\n\nBodo: <a href="https:/
 /bodoschwabe.github.io/">https://bodoschwabe.github.io/</a><br>\nMateja: <
 a href="https://uk.linkedin.com/in/mateja-gosenca-99b267133">https://uk.li
 nkedin.com/in/mateja-gosenca-99b267133</a>\n\nAxioNyx: <a href="https://gi
 thub.com/axionyx">https://github.com/axionyx</a><br>\nThe paper: <a href="
 https://arxiv.org/abs/2007.08256">https://arxiv.org/abs/2007.08256</a>\n<h
 r>\n\n<b>Index to Key Parts of the Talk:</b><br>\n00:00 <a href="https://y
 outu.be/ufRKKi6CUUs?t=0">Shaun introduces Bodo Schwabe and Mateja Gosenca<
 /a><br>\n\n00:37 <a href="https://youtu.be/ufRKKi6CUUs?t=37">Mateja&#39\;s
  opening comments about this new code</a><br>\n\n02:18 <a href="https://yo
 utu.be/ufRKKi6CUUs?t=138">Q&amp\;A: what are two things you&#39\;d want vi
 ewers to remember about this talk?</a><br>\n\n03:41 <a href="https://youtu
 .be/ufRKKi6CUUs?t=221">Q&amp\;A: what was the motivation for this work?</a
 ><br>\n\n06:36 <a href="https://youtu.be/ufRKKi6CUUs?t=396">Q&amp\;A: What
  was done in the paper? What are the details about adaptive mesh refinemen
 t (AMR)?</a><br>\n\n07:05 <a href="https://youtu.be/ufRKKi6CUUs?t=425">Sli
 de: FDM Structure Formation</a><br>\n\n09:17 <a href="https://youtu.be/ufR
 KKi6CUUs?t=557">Q&amp\;A: Is there an intuitive way of explaining why the 
 Schrodinger equation is the right equation here?</a><br>\n\n10:10 <a href=
 "https://youtu.be/ufRKKi6CUUs?t=610">Slide: FDM mass constraints</a><br>\n
 \n14:49 <a href="https://youtu.be/ufRKKi6CUUs?t=889">Slide: Quantifying Mi
 xed Fuzzy Cold Dark Matter Halo Dynamics</a>: Radial density profiles\; CD
 M velocity dispersion vs FDM granular structure\; Solitonic core dynamics<
 br>\n\n16:22 <a href="https://youtu.be/ufRKKi6CUUs?t=982">Slide: AxioNyx: 
 Simulating Mixed Fuzzy and Cold Dark Matter</a>: Figure 1 from the paper<b
 r>\n\n17:54 <a href="https://youtu.be/ufRKKi6CUUs?t=1074">Slide: Spherical
  Collapse – linear</a>: Figures 2 and 3 from the paper<br>\n\n21:14 <a h
 ref="https://youtu.be/ufRKKi6CUUs?t=1274">Slide: Spherical Collapse – No
 n-linear</a>: Figure 4 from the paper<br>\n\n27:26 <a href="https://youtu.
 be/ufRKKi6CUUs?t=1646">Slide: Comments on Figures 5\, 6\, and 7 from the p
 aper</a><br>\n\n32:07 <a href="https://youtu.be/ufRKKi6CUUs?t=1927">Q&amp\
 ;A about (1) the linearity and (2) is there an intuitive explanation of th
 e equations?</a><br>\n\n35:30 <a href="https://youtu.be/ufRKKi6CUUs?t=2130
 ">Conclusions slide</a><br>\n\n38:22 <a href="https://youtu.be/ufRKKi6CUUs
 ?t=2302">Q&amp\;A: What is coming next in your work?</a><br>\n\n42:29 <a h
 ref="https://youtu.be/ufRKKi6CUUs?t=2549">Q&amp\;A asked individually to B
 odo and Mateja: outside of your own research\, what do you think is the mo
 st interesting thing in cosmology at the moment?</a><br>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/21/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Ryan Keeley (Korea Astronomy and Space Science Institute)
DTSTART:20201008T050000Z
DTEND:20201008T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/22
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/22/">Maybe inflation is the solution to the Hubble tension!?</a>\nby Ry
 an Keeley (Korea Astronomy and Space Science Institute) as part of Cosmolo
 gy Talks\n\n\nAbstract\nRyan tells us about how the Hubble tension (betwee
 n Planck measurements of the cosmic microwave background temperature aniso
 tropies and SH0ES measurements of the expansion rate of the universe) can 
 be completely solved with a non-standard primordial power spectrum for the
  curvature perturbation\, which could arise e.g. if there is a kink in the
  inflationary potential. \n\nThe non-standard power spectrum has an oscill
 atory feature that exactly mimics the effects of a slightly different valu
 e for the expansion rate today. They find this power spectrum by explicitl
 y reconstructing it\, so they aren't supplying a well motivated a priori m
 odel. However their work does represent a proof of concept that a non-stan
 dard power spectrum could mimic the effects of a different expansion rate.
 \n\nWhile the Hubble tension remains unsolved and while all other models t
 o explain it suffer from their own problems\, work like this remains well 
 motivated. It would perhaps be a bit fine tuned to have a feature at exact
 ly the right place in the primordial power spectrum to mimic the effects o
 f H0 today\, but there could be many features and if one happened to align
  then this would be what we would see\, so it can't be ruled out a priori.
 \n\nFuture work will test this with polarisation data and the matter power
  spectrum... so stay tuned. If this is the solution it might leave measura
 ble signatures in those results.\n\nRyan: http://cosmology.kasi.re.kr/memb
 ers.php?member=ryan \n\nThe paper: https://arxiv.org/abs/2006.12710 Inflat
 ion Wars: A New Hope\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>  \n\n
 00:00 <a href="https://youtu.be/kyfebUbxh6E?t=0">Shaun's introduction</a>\
 n\n01:04 <a href="https://youtu.be/kyfebUbxh6E?t=64">Ryan's opening commen
 ts</a>\n\n02:01 <a href="https://youtu.be/kyfebUbxh6E?t=121">What two simp
 le things do you want people to take away from this talk?</a>\n\n02:35 <a 
 href="https://youtu.be/kyfebUbxh6E?t=155">What is the background for this 
 work?</a>\n\n03:36 <a href="https://youtu.be/kyfebUbxh6E?t=216">Deconvolut
 ion slide</a>: decomposition is done with the modified Richardson-Lucy dec
 onvolution algorithm\n\n04:19 <a href="https://youtu.be/kyfebUbxh6E?t=259"
 >The transfer function and how it gives the modified initial power spectru
 m</a>\n\n06:47 <a href="https://youtu.be/kyfebUbxh6E?t=407">Modified Richa
 rdson-Lucy Deconvolution slide</a>\n\n07:43 <a href="https://youtu.be/kyfe
 bUbxh6E?t=463">Sound Cancellation slide</a>: Figure 1 from the paper\n\n09
 :22 <a href="https://youtu.be/kyfebUbxh6E?t=562">Features slide</a>: Figur
 e 2 bottom panel\n\n10:20 <a href="https://youtu.be/kyfebUbxh6E?t=620">Pos
 teriors slide</a>: Figure 3\n\n13:41 <a href="https://youtu.be/kyfebUbxh6E
 ?t=821">Priors slide</a>\n\n18:08 <a href="https://youtu.be/kyfebUbxh6E?t=
 1088">Filtering slide</a>: Figure 4\n\n23:59 <a href="https://youtu.be/kyf
 ebUbxh6E?t=1439">Conclusions slide</a>\n\n24:45 <a href="https://youtu.be/
 kyfebUbxh6E?t=1485">Where to next?</a>\n\n26:42 <a href="https://youtu.be/
 kyfebUbxh6E?t=1602">Outside of your own research\, what do you think is th
 e most interesting thing in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/22/
END:VEVENT
BEGIN:VEVENT
SUMMARY:George Zahariade (Arizona State University)
DTSTART:20201108T050000Z
DTEND:20201108T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/23
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/23/">Quantum gravity adds (v quiet) noise to gravitational wave detecto
 rs</a>\nby George Zahariade (Arizona State University) as part of Cosmolog
 y Talks\n\n\nAbstract\nGeorge tells us what happens in gravitational wave 
 detectors when you quantise the gravitational field.\n\nHe talks about a c
 alculation he did with Maulik Parikh and Frank Wilczek which examines what
  effect quantising the gravitational field would have on gravitational wav
 e detectors.\n\nThey first treat the detector and gravitational field quan
 tum mechanically. For certain gravitational wave states (e.g. a coherent s
 tate\, a squeezed state and a thermal state) they are then able to solve t
 he gravitational field parts of the resulting path integral (or canonical 
 expectation values).\n\nIn the resulting expression they then take the mos
 t probable path for the detector (i.e. the classical path) and determine a
 n equation of motion for the distance between the ends of the detector (i.
 e. the classical equation of motion for the detector\, with quantum effect
 s from the gravitational field included).\n\nThis new equation of motion i
 s like the purely classical one except with the addition of a new noise te
 rm. In the case of a squeezed state this noise can be exponentially enhanc
 ed\, which might have implications for gravitational waves from inflation\
 , which at least start out in a squeezed state.\n\nGeorge: <a href="https:
 //www.linkedin.com/in/george-zahariade-844b27b4">linkedin.com/george-zahar
 iade</a><br>\nPapers: <a href="https://arxiv.org/abs/2010.08208">2010.0820
 8</a> and <a href="https://arxiv.org/abs/2010.08205">2010.08205</a><br>\nE
 ssay: <a href="https://arxiv.org/abs/2005.07211">2005.07211</a>\n<hr>\n\n<
 b>Index to Key Parts of the Talk:</b>  \n\n00:00 <a href="https://www.yout
 ube.com/watch?v=zAUDogTyfVg&feature=youtu.be&t=0">Shaun's introduction</a>
 : This is on how one might measure the quantum nature of gravitational wav
 es. Being a bit outside the realm of normal cosmology\, it's at a general 
 technical level so this talk will be at maybe a colloquium level rather th
 an a seminar level.  \n\n00:42 <a href="https://www.youtube.com/watch?v=zA
 UDogTyfVg&feature=youtu.be&t=42">George's opening comments</a>  \n\n04:44 
 <a href="https://www.youtube.com/watch?v=zAUDogTyfVg&t=284">Q&A: what are 
 two things you'd want viewers to remember about this talk?</a>: (1) we pre
 dict that the quantization of the gravitational field should imply the exi
 stence of an additional source of noise that would superimpose itself to a
 ll the other noise sources that exist in a GW interferometer\, and (2) the
  characteristic of this noise depends strongly on the quantum state of the
  gravitational field\, so the noise it induces on the signal (depending on
  its state) will be very different and possibly observable.\n\n06:03 <a hr
 ef="https://www.youtube.com/watch?v=zAUDogTyfVg&t=363">Q&A: what was the m
 otivation for this work?</a> \n\n06:50 <a href="https://www.youtube.com/wa
 tch?v=zAUDogTyfVg&t=410">Q&A: Why hasn't this calculation been done before
 ?</a>   \n\n08:53 <a href="https://www.youtube.com/watch?v=zAUDogTyfVg&t=5
 33">Could LIGO do something differently now or in the future that would be
  useful to test this prediction?</a>: the signature of the quantization of
  the gravitational field is a noise term\, so we need an experiment that f
 ocuses on the noises not on the signals. \n\n09:11 <a href="https://www.yo
 utube.com/watch?v=zAUDogTyfVg&t=551">Getting into the details</a>: First s
 lide - the history of this topic and references\n\n10:00 <a href="https://
 www.youtube.com/watch?v=zAUDogTyfVg&t=600">Outline of the presentation</a>
   \n\n10:54 <a href="https://www.youtube.com/watch?v=zAUDogTyfVg&t=654">Ba
 sic Idea slide</a>  \n\n13:54 <a href="https://www.youtube.com/watch?v=zAU
 DogTyfVg&t=834">Detector Model</a>  \n\n16:00 <a href="https://www.youtube
 .com/watch?v=zAUDogTyfVg&t=960">Assumptions and approximations</a>  \n\n21
 :28 <a href="https://www.youtube.com/watch?v=zAUDogTyfVg&t=1288">Detector 
 response to quantized GW</a>  \n\n23:21 <a href="https://www.youtube.com/w
 atch?v=zAUDogTyfVg&t=1401">Calculating the transition probability from the
  initial states to the final state</a>  \n\n24:15 <a href="https://www.you
 tube.com/watch?v=zAUDogTyfVg&t=1455">Influence Functional slide</a>: basic
 ally this functional encodes all the quantum effects of the gravitational 
 field  \n\n25:46 <a href="https://www.youtube.com/watch?v=zAUDogTyfVg&t=15
 46">Able to calculate the influence function for different incoming gravit
 ational field states</a>: first consider a coherent state   \n\n29:16 <a h
 ref="https://www.youtube.com/watch?v=zAUDogTyfVg&t=1756">Analysis of the I
 nfluence Functional slide (for a coherent state)</a>  \n\n32:05 <a href="h
 ttps://www.youtube.com/watch?v=zAUDogTyfVg&t=1925">Back to the Transition 
 Probability slide</a>  \n\n33:18 <a href="https://www.youtube.com/watch?v=
 zAUDogTyfVg&t=1998">Langevin Equation slide</a>: final result - effective 
 equation of motion for the detector including quantum effects\; the quantu
 m modification of the classical geodesic deviation equation\n\n36:07 <a hr
 ef="https://www.youtube.com/watch?v=zAUDogTyfVg&t=2167">Analysis of Noise 
 slide</a>: for different states there will be different spectra of the noi
 se - equations for vacuum and coherent states\, thermal states\, and squee
 zed states\; thermal states might be of interest to cosmologists (some sto
 chastic GW backgrounds might be thermal)\; squeezed states of the gravitat
 ional fied can arise from cosmology (inflationary perturbations) \n\n41:07
  <a href="https://www.youtube.com/watch?v=zAUDogTyfVg&t=2467">Estimates of
  the noise for each case</a>: the most hopeful scenario is the case of squ
 eezed gravity states that might have a quantum noise that is measurable  \
 n\n42:39 <a href="https://www.youtube.com/watch?v=zAUDogTyfVg&t=2559">Summ
 ary slide</a>  \n\n45:08 <a href="https://www.youtube.com/watch?v=zAUDogTy
 fVg&t=2708">Q&A: Where to next?</a>  \n\n46:15 <a href="https://www.youtub
 e.com/watch?v=zAUDogTyfVg&t=2775">Q&A: outside of your own research\, what
  do you think is the most interesting thing in cosmology at the moment?</a
 >\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/23/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Moritz Haslbauer and Indranil Banik (University of Bonn)
DTSTART:20201118T050000Z
DTEND:20201118T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/24
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/24/">Maybe Milgromian gravity solves the Hubble tension!? - The KBC voi
 d & νHDM model</a>\nby Moritz Haslbauer and Indranil Banik (University of
  Bonn) as part of Cosmology Talks\n\n\nAbstract\nMoritz Haslbauer and Indr
 anil Banik talk about the Keenan\, Barger and Cowie (KBC) void and the νH
 DM model of cosmology. \n\nThe KBC void is a locally observed ~300 Mpc sca
 le under-density that appears to be impossible within ΛCDM (under-densiti
 es shouldn't have emptied out this much by now).\n\nνHDM is a model that 
 has sterile neutrinos as a hot dark matter component and enhanced gravity 
 in environments with a weak gravitational field. This dark matter adequate
 ly explains the CMB and expansion history of the universe\, but doesn't cl
 uster on the smallest scales. The modified gravity (essentially Milgromian
  dynamics\, or MOND) then kicks in on these scales to produce phenomena li
 ke the correct rotation curves in galaxies.\n\nMoritz and Indranil give an
  intro to both KBC and νHDM\, and then explain how this model is consiste
 nt with the main tent-poles of modern cosmology (e.g. the CMB anisotropies
 \, nucleosynthesis\, the displacement of the gas and weak lensing in the b
 ullet cluster\, galaxy rotation curves\, the clustering of galaxies) and c
 an also alleviate some of the tensions in the standard ΛCDM model.\n\nThe
  paper: <a href="https://arxiv.org/abs/2009.11292">2009.11292</a> \n\nMori
 tz: <a href="https://moritzhaslbauer.jimdofree.com/">moritzhaslbauer.jimdo
 free.com</a> \n\nIndranil: <a href="https://www.youtube.com/channel/UCwO0b
 EeE6oNahkt8dWQFcXw/">Youtube videos</a> \n\nA blog post by Indranil\, Mori
 tz (and co-author Pavel) on the same topic: <a href="https://tritonstation
 .com/2020/10/23/big-trouble-in-a-deep-void/">Big Trouble in a Deep Void</a
 >\n\nA blog with ongoing updates of the most serious problems for standard
  cosmology: <a href="https://darkmattercrisis.wordpress.com">The Dark Matt
 er Crisis</a>\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>\n\n[00:00] <
 a href="https://youtu.be/LMhjenB7V8g?t=0">Shaun's intro</a>\n\n[00:42] <a 
 href="https://youtu.be/LMhjenB7V8g?t=42">Opening comments (Moritz)</a>\n\n
 [00:58] <a href="https://youtu.be/LMhjenB7V8g?t=58">Brief summary of findi
 ngs</a> Overview:  Keenan-Barger-Cowie void and H_0 tension\n\n[03:36] <a 
 href="https://youtu.be/LMhjenB7V8g?t=216">Take Home Message slide</a>\n\n[
 04:08] <a href="https://youtu.be/LMhjenB7V8g?t=248">The observations that 
 motivated this project (Indranil)</a>\n\n[04:34] <a href="https://youtu.be
 /LMhjenB7V8g?t=274">The most important references and observational constr
 aints</a>\n\n[06:00] <a href="https://youtu.be/LMhjenB7V8g?t=360">The KBC 
 void and Hubble tension in ΛCDM</a>: the Millennium (MXXL) simulation\n\n
 [09:18] <a href="https://youtu.be/LMhjenB7V8g?t=558">Comments on Figure 1 
 from the paper</a>\n\n[09:46] <a href="https://youtu.be/LMhjenB7V8g?t=586"
 >Why an allowance is needed for redshift space distortion effects</a>\n\n[
 10:46] <a href="https://youtu.be/LMhjenB7V8g?t=646">One of the important r
 esults is the KBC void falsifies ΛCDM at 6.04σ</a>\n\n[10:59] <a href="h
 ttps://youtu.be/LMhjenB7V8g?t=659">The redshift space distortion is relate
 d to the impact the void has on the locally measured H_0</a>\n\n[11:56] <a
  href="https://youtu.be/LMhjenB7V8g?t=716">Observations indicate a deeper 
 underdensity and larger H_0 than is expected in ΛCDM</a>: Figure 2\n\n[13
 :22] <a href="https://youtu.be/LMhjenB7V8g?t=802">Large scale failure of 
 ΛCDM</a>: to get from z=1100 to z=0 observations\, need effectively stron
 ger gravity to grow structure faster\n\n[14:20] <a href="https://youtu.be/
 LMhjenB7V8g?t=860">Constraints from data on galaxy scales: the second moti
 vation for this work</a>\n\n[16:04] <a href="https://youtu.be/LMhjenB7V8g?
 t=964">Milgromian Dynamics (MOND)</a>\n\n[20:42] <a href="https://youtu.be
 /LMhjenB7V8g?t=1242">Cosmological MOND framework (vHDM): Overview</a>\n\n[
 23:14] <a href="https://youtu.be/LMhjenB7V8g?t=1394">vHDM framework: Impac
 t on CMB</a>\n\n[27:31] <a href="https://youtu.be/LMhjenB7V8g?t=1651">Terr
 estrial Evidence for Sterile Neutrinos</a>\n\n[28:58] <a href="https://you
 tu.be/LMhjenB7V8g?t=1738">Astronomical Evidence for Fast Collisionless Mat
 ter</a>\n\n[32:28] <a href="https://youtu.be/LMhjenB7V8g?t=1948">What the 
 vHDM Framework Can Explain</a>\n\n[34:50] <a href="https://youtu.be/LMhjen
 B7V8g?t=2090">Application to KBC void: Model assumptions (Moritz)</a>\n\n[
 36:23] <a href="https://youtu.be/LMhjenB7V8g?t=2183">Results: Growth of st
 ructure</a>: Figure 5\n\n[39:15] <a href="https://youtu.be/LMhjenB7V8g?t=2
 355">Results: Local H_0 & acceleration parameter</a>: Figure 6\n\n[43:15] 
 <a href="https://youtu.be/LMhjenB7V8g?t=2595">Results: Peculiar velocity f
 ield</a>: Figure 8\n\n[45:37] <a href="https://youtu.be/LMhjenB7V8g?t=2737
 ">Results: comparing ΛCDM with νHDM</a> \n\n[48:10] <a href="https://you
 tu.be/LMhjenB7V8g?t=2890">Summary and Conclusions</a>\n\n[50:03] <a href="
 https://youtu.be/LMhjenB7V8g?t=3003">What are the next steps? => Outlook s
 lide\; simulation videos</a>\n\n[51:14] <a href="https://youtu.be/LMhjenB7
 V8g?t=3114">Q&A on why results from many other void studies aren't getting
  large conflicts with ΛCDM</a>\n\n[53:06] <a href="https://youtu.be/LMhje
 nB7V8g?t=3186">Q&A: outside of your own research what do you think is the 
 most interesting thing in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/24/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Eiichiro Komatsu and Yuto Minami (Max Planck Institute Garching an
 d KEK Japan)
DTSTART:20201123T050000Z
DTEND:20201123T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/25
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/25/">A tantalising hint of parity violation in the cosmic microwave bac
 kground</a>\nby Eiichiro Komatsu and Yuto Minami (Max Planck Institute Gar
 ching and KEK Japan) as part of Cosmology Talks\n\n\nAbstract\nEiichiro Ko
 matsu and Yuto Minami talk about their recent work\, first devising a way 
 to extract a parity violating signature in the cosmic microwave background
  (i.e. birefringence) and then measuring it in Planck 2018 data.\n\nThey g
 et a 2.4 sigma hint of a result\, which is "important\, if true".\n\nThis 
 signal is measured via correlation of E mode and B mode polarisation in th
 e CMB. If the universe is birefringent then E mode polarisation would chan
 ge into B mode and there would be a non-zero correlation between the two m
 easured modes. Unfortunately\, if the detector angle on the telescope wasn
 't calibrated perfectly this would mimic the interesting signal. Yuto and 
 Eiichiro's new method is to measure this detector angle by looking at the 
 E-B correlation in the foregrounds\, where the light hasn't travelled far 
 enough to be affected by any potential birefringence in the universe.\n\nT
 his allows them to partially distinguish between the two types of measured
  E-B correlation. And with this method they get the hint of a signal for t
 he new physics in the Planck 2018 data.\n\nThe method can be applied to th
 e data from all other telescopes that have measured the polarisation of th
 e microwave background and can therefore be confirmed\, ruled out\, or at 
 least examined by SPT\, ACT\, Polarbear\, etc. \n\nYuto and Eiichiro are a
 lso working with Planck to see if they can further rule out other systemat
 ics\, e.g. an intrinsic E-B correlation in the foreground polarisation.\n\
 nThe paper: <a href="https://arxiv.org/abs/2011.11254">2011.11254 on the a
 rXiv</a> and <a href="https://journals.aps.org/prl/abstract/10.1103/PhysRe
 vLett.125.221301">published in PRL</a>.\n\n<a href=https://www.youtube.com
 /watch?v=9W9rDlEHg3c">Video of talk</a>\n\nEiichiro: <a href="https://wwwm
 pa.mpa-garching.mpg.de/~komatsu/">https://wwwmpa.mpa-garching.mpg.de/~koma
 tsu/</a>\n\nYuto: <a href="https://orcid.org/0000-0003-2176-8089">https://
 orcid.org/0000-0003-2176-8089</a>\n\n<hr>\n\n<b>Index to Key Parts of the 
 Talk:</b>\n\n[00:00] <a href="https://youtu.be/9W9rDlEHg3c?t=1">Shaun's in
 tro</a>\n\n[00:38] <a href="https://youtu.be/9W9rDlEHg3c?t=38">Opening com
 ments about the paper by Eiichiro</a>\n\n[01:51] <a href="https://youtu.be
 /9W9rDlEHg3c?t=111">Q&A: What two things would you want people to remember
  about this talk?</a>\n\n[03:30] <a href="https://youtu.be/9W9rDlEHg3c?t=2
 10">The methodology papers that led to this announcement</a>: they have be
 en working on this for ~2 years\n\n[04:18] <a href="https://youtu.be/9W9rD
 lEHg3c?t=258">How does the electromagnetic wave of the CMB reach us?</a>\n
 \n[04:41] <a href="https://youtu.be/9W9rDlEHg3c?t=281">Cosmic Birefringenc
 e</a>\n\n[09:24] <a href="https://youtu.be/9W9rDlEHg3c?t=564">What was the
  motivation for this work? Why study cosmic birefringence?</a>\n\n[10:17] 
 <a href="https://youtu.be/9W9rDlEHg3c?t=617">E- and B-mode decomposition o
 f linear polarisation</a>\n\n[10:53] <a href="https://youtu.be/9W9rDlEHg3c
 ?t=653">Parity flip</a>\n\n[11:30] <a href="https://youtu.be/9W9rDlEHg3c?t
 =690">Power spectra</a>\n\n[12:05] <a href="https://youtu.be/9W9rDlEHg3c?t
 =725">EB correlation from the cosmic birefringence</a>\n\n[14:46] <a href=
 "https://youtu.be/9W9rDlEHg3c?t=886">Searching for the birefringence: Impr
 ovement #1 (Zhao et al. 2015)</a>\n\n[15:15] <a href="https://youtu.be/9W9
 rDlEHg3c?t=915">The biggest problem: miscalibration of detectors. Impact o
 f miscalibration of polarisation angles.</a>\n\n[16:10] <a href="https://y
 outu.be/9W9rDlEHg3c?t=970">The past measurements</a>: Uncertainty in the c
 alibration of α has been the major limitation.\n\n[18:07] <a href="https:
 //youtu.be/9W9rDlEHg3c?t=1087">The Key Idea: The polarised Galactic foregr
 ound emission as a calibrator</a>: it would not be affected by the cosmic 
 birefringence\n\n[18:35] <a href="https://youtu.be/9W9rDlEHg3c?t=1115">Sea
 rching for the birefringence: Improvement #2 (Minami et al. 2019)</a>: Ide
 a: miscalibration of the polarisation angle α rotates both the foreground
  and CMB\, but β affects only the CMB. Key: no explicit modeling of the f
 oreground EE and BB is necessary.\n\n[20:06] <a href="https://youtu.be/9W9
 rDlEHg3c?t=1206">Assumption for the baseline result</a>: What about the in
 trinsic EB correlation of the foreground emission?\n\n[20:57] <a href="htt
 ps://youtu.be/9W9rDlEHg3c?t=1257">Likelihood for the simplest case: single
 -frequency\, full sky data</a>\n\n[21:08] <a href="https://youtu.be/9W9rDl
 EHg3c?t=1268">How does it work? Simulation of future CMB data (LiteBIRD)</
 a>\n\n[23:18] <a href="https://youtu.be/9W9rDlEHg3c?t=1398">Question that 
 provides an idea for possible follow-up research</a>\n\n[24:20] <a href="h
 ttps://youtu.be/9W9rDlEHg3c?t=1460">Application to the Planck Data (PR3)</
 a>: (information for experts)\n\n[25:21] <a href="https://youtu.be/9W9rDlE
 Hg3c?t=1521">Validation by FFP10 (Planck team's "Full Focal Plane Simulati
 on")</a>\n\n[25:55] <a href="https://youtu.be/9W9rDlEHg3c?t=1555">Main Res
 ults</a>: Figure 1 from the paper\n\n[27:12] <a href="https://youtu.be/9W9
 rDlEHg3c?t=1632">Can we see β = 0.35 +/- 0.14 deg by eyes?</a>: Figure 2\
 n\n[30:00] <a href="https://youtu.be/9W9rDlEHg3c?t=">How about the foregro
 und EB?</a>\n\n[32:31] <a href="https://youtu.be/9W9rDlEHg3c?t=1951">Q&A: 
 if it turns out to be a systematic error\, what is the most likely error s
 ource?</a>\n\n[33:14] <a href="https://youtu.be/9W9rDlEHg3c?t=1994">Implic
 ations: what does it mean for models of dark matter and energy?</a>\n\n[34
 :19] <a href="https://youtu.be/9W9rDlEHg3c?t=2059">Conclusion</a>\n\n[38:4
 3] <a href="https://youtu.be/9W9rDlEHg3c?t=2323">Comment by Yuto on compar
 ison with Planck data</a>\n\n[39:00] <a href="https://youtu.be/9W9rDlEHg3c
 ?t=2340">What comes next?</a>\n\n[39:56] <a href="https://youtu.be/9W9rDlE
 Hg3c?t=2396">Q&A: outside of your own research what do you think is the mo
 st interesting thing in cosmology at the moment?</a>: Yuto at <a href="htt
 ps://youtu.be/9W9rDlEHg3c?t=2404">40:04</a> and Eiichiro at <a href="https
 ://youtu.be/9W9rDlEHg3c?t=2413">40.13</a>.\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/25/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Alvaro Pozo (University of the Basque Country)
DTSTART:20210213T050000Z
DTEND:20210213T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/26
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/26/">Potential evidence for wave dark matter (via core-halo transition 
 in dwarf galaxies)</a>\nby Alvaro Pozo (University of the Basque Country) 
 as part of Cosmology Talks\n\n\nAbstract\nAlvaro tells us about a recent p
 aper where he an collaborators detect the transition between a core (flat 
 density profile) and halo (power law density profile) in dwarf galaxies.\n
 \nThe full core + halo profile matches very closely what is expected in wa
 ve/ultralight/fuzzy/axionic dark matter simulations (without baryonic effe
 cts included). That is\, there is a very flat core\, which then drops off 
 suddenly and then flattens off to a decaying power-law profile. The core m
 atches the soliton expected in wave dark matter and the halo matches an ou
 ter NFW profile expected outside the soliton.\n\nThey also detect evidence
  for tidal stripping of the matter in the galaxies. The galaxies closer to
  the centre of the milky way have their transition point between core and 
 halo happen at smaller densities (despite the core density itself not bein
 g systematically smaller). The transition also appears to happen closer to
  the centre of the galaxy\, which matches simulations.\n\nOf course the co
 re-+halo pattern they have clearly observed might be due to something else
 \, but the match between wave dark matter simulations and observations is 
 impressive.\n\nThe huge caveat is that the mass for the dark matter that t
 hey use is very small and in significant tension with Lyman Alpha constrai
 nts for wave-like dark matter. This might indicate that the source of this
  universal core+halo pattern they're observing comes from something else\,
  or it might indicate that the wave dark matter is more complicated than v
 anilla models... \n\nStay tuned to the arXiv for future papers looking at 
 this in more detail!\n\nPaper: <a href="https://arxiv.org/abs/2010.10337">
 2010.10337</a>\n<hr>\n\n<b>Index to Key Parts of the Talk:</b>\n\n[00:00] 
 <a href="https://youtu.be/HeARhCr0Wr0?t=0">Shaun's intro</a>\n\n[00:38] <a
  href="https://youtu.be/HeARhCr0Wr0?t=38">Alvaro's opening remarks and bri
 ef summary of paper</a>\n\n[00:48] <a href="https://youtu.be/HeARhCr0Wr0?t
 =48">Q&A: What two things would you want people to remember about this tal
 k?</a>\n\n[01:12] <a href="https://youtu.be/HeARhCr0Wr0?t=72">Abstract and
  Introduction\; main objectives of this work</a>\n\n[02:58] <a href="https
 ://youtu.be/HeARhCr0Wr0?t=178">Focus on dwarf galaxies</a>\n\n[04:52] <a h
 ref="https://youtu.be/HeARhCr0Wr0?t=292">Main Two Results</a>\n\n[06:55] <
 a href="https://youtu.be/HeARhCr0Wr0?t=415">Context - general info of dwar
 f galaxies and classification between isolated and orbiting galaxies\; Tab
 le 1 from the 2010.10337 paper</a>\n\n[09:00] <a href="https://youtu.be/He
 ARhCr0Wr0?t=540">Motivation for this work</a>\n\n[12:03] <a href="https://
 youtu.be/HeARhCr0Wr0?t=723">Context: NFW inefficient to describe the densi
 ty profile in the centre -> solution: add wave dark matter profile\; Plumm
 er model</a>\n\n[14:28] <a href="https://youtu.be/HeARhCr0Wr0?t=868">Metho
 dology</a>\n\n[19:17] <a href="https://youtu.be/HeARhCr0Wr0?t=1157">Explan
 atory comment insert from Shaun while editing</a>\n\n[21:02] <a href="http
 s://youtu.be/HeARhCr0Wr0?t=1262">Results\; Figure 5 from the paper</a>\n\n
 [24:06] <a href="https://youtu.be/HeARhCr0Wr0?t=1446">Figure 1 from the pa
 per</a>\n\n[24:58] <a href="https://youtu.be/HeARhCr0Wr0?t=1498">Figure 2<
 /a>\n\n[28:12] <a href="https://youtu.be/HeARhCr0Wr0?t=1692">Figure 3: "th
 e most important\, or one of the most important plots of the paper"</a>\n\
 n[31:38] <a href="https://youtu.be/HeARhCr0Wr0?t=1898">Figure 4</a>\n\n[36
 :47] <a href="https://youtu.be/HeARhCr0Wr0?t=2207">Conclusions</a>\n\n[41:
 08] <a href="https://youtu.be/HeARhCr0Wr0?t=2468">Where to next?</a>\n\n[4
 2:49] <a href="https://youtu.be/HeARhCr0Wr0?t=2569">Outside of your own re
 search what do you think are the most interesting things in cosmology at t
 he moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/26/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Volker Springel (Max Planck Institute for Astrophysics)
DTSTART:20210226T050000Z
DTEND:20210226T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/27
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/27/">Simulating cosmic structure formation with the GADGET-4 code</a>\n
 by Volker Springel (Max Planck Institute for Astrophysics) as part of Cosm
 ology Talks\n\n\nAbstract\nCosmology Talks moderator Shaun Hotchkiss welco
 mes guest speaker Volker Springel\, who talks about the new GADGET-4 code.
 \n\nFeaturing all the things you wanted to know about GADGET-4 but were af
 raid to ask\, including:\n\n- What new algorithms are used to make it bett
 er and faster than earlier versions\n\n- Why you never heard of GADGET-3\n
 \n- What new features you can now use when running cosmological simulation
 s (e.g. varying the algorithms\; or outputting lightcones\, halo catalogue
 s and merger trees "on the fly")\n\n- why storing the locations of your si
 mulation particles as integers is better than storing them as floating poi
 nt numbers\n\n- and what the author of the most used simulation code in co
 smology thinks are the most interesting questions in cosmology at the mome
 nt (both related and unrelated to simulations)\n\nVolker Springel: <a href
 ="https://www.mpa-garching.mpg.de/person/55019/2377">Home page on Max Plan
 ck Insitute site</a>\n\nGADGET-4 code: <a href="https://wwwmpa.mpa-garchin
 g.mpg.de/gadget4/">wwwmpa.mpa-garching.mpg.de/gadget4/</a>\n\nPaper: <a hr
 ef="https://arxiv.org/abs/2010.03567">2010.03567</a>\n<hr>\n\n<b>Index to 
 Key Parts of the Talk:</b>\n\n[00:00] <a href="https://youtu.be/4zFlSP-_C5
 4?t=0">Shaun's intro</a>\n\n[00:45] <a href="https://youtu.be/4zFlSP-_C54?
 t=45">Volker's opening comments about the paper and the code</a>\n\n[01:26
 ] <a href="https://youtu.be/4zFlSP-_C54?t=86">Q&A: What two things would y
 ou want people to remember about this talk?</a>\n\n[02:48] <a href="https:
 //youtu.be/4zFlSP-_C54?t=168">Diving into the details</a>\n\n[03:51] <a hr
 ef="https://youtu.be/4zFlSP-_C54?t=231">Upcoming extremely large galaxy su
 rveys promise the next advances in cosmology</a>: EUCLID\, LSST\, WFIRST\;
  their goals\; accurate theoretical predictions of comparable size as the 
 surveys are needed\n\n[05:32] <a href="https://youtu.be/4zFlSP-_C54?t=332"
 >For GADGET to remain a useful code\, it needed profound upgrades\; what w
 e tried to achieve with GADGET-4</a>\n\n[07:21] <a href="https://youtu.be/
 4zFlSP-_C54?t=441">Historical evolution of GADGET code</a>\n\n[08:52] <a h
 ref="https://youtu.be/4zFlSP-_C54?t=532">Recent GADGET history</a>\n\n[11:
 36] <a href="https://youtu.be/4zFlSP-_C54?t=696">Comments on the 2010.0356
 7 paper</a>\n\n[12:55] <a href="https://youtu.be/4zFlSP-_C54?t=775">Simula
 tion output: Millennium-TNG example</a>\n\n[14:33] <a href="https://youtu.
 be/4zFlSP-_C54?t=873">The new GADGET-4 code scales beyond 10^5 cores</a>\n
 \n[17:12] <a href="https://youtu.be/4zFlSP-_C54?t=1032">GADGET-4 shows muc
 h better strong and weak scaling as GADGET-2</a>: Figure 61 in the paper\n
 \n[24:00] <a href="https://youtu.be/4zFlSP-_C54?t=1440">GADGET-4 can be us
 ed in a number of different configurations</a>\n\n[25:01] <a href="https:/
 /youtu.be/4zFlSP-_C54?t=1501">The fast mulitpole method (FMM)</a>\n\n[26:5
 3] <a href="https://youtu.be/4zFlSP-_C54?t=1613">Novel MPI-3 based shared 
 memory parallelization paradigm</a>\n\n[28:08] <a href="https://youtu.be/4
 zFlSP-_C54?t=1688">Scaling of force errors</a>: Fig 10\n\n[30:56] <a href=
 "https://youtu.be/4zFlSP-_C54?t=1856">The optimum multipole order in terms
  of CPU consumption</a>: Fig 13\n\n[32:43] <a href="https://youtu.be/4zFlS
 P-_C54?t=1963">Comparison with other codes</a>\n\n[33:51] <a href="https:/
 /youtu.be/4zFlSP-_C54?t=2031">The tree force approximation</a>: Fig 25/26\
 , left panel\n\n[35:24] <a href="https://youtu.be/4zFlSP-_C54?t=2124">The 
 FMM force field expansions</a>: Fig 25/26\, right panel\n\n[37:25] <a href
 ="https://youtu.be/4zFlSP-_C54?t=2245">Integer coordinates</a>\n\n[40:42] 
 <a href="https://youtu.be/4zFlSP-_C54?t=2442">Lightcones\, merger trees\, 
 power-spectra\, etc</a>: Fig 41\n\n[43:00] <a href="https://youtu.be/4zFlS
 P-_C54?t=2580">Subhalo tracking\; subhalo catalogues\; merger trees</a>\n\
 n[47:05] <a href="https://youtu.be/4zFlSP-_C54?t=2825">Summary</a>\n\n[49:
 00] <a href="https://youtu.be/4zFlSP-_C54?t=2940">Where to next?</a>\n\n[5
 2:37] <a href="https://youtu.be/4zFlSP-_C54?t=3157">Q&A: outside of your o
 wn research what do you think is the most interesting thing in cosmology a
 t the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/27/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Azadeh Maleknejad (CERN Department of Theoretical Physics)
DTSTART:20210310T050000Z
DTEND:20210310T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/28
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/28/">A common origin for inflation\, neutrino mass\, baryogenesis\, and
  dark matter</a>\nby Azadeh Maleknejad (CERN Department of Theoretical Phy
 sics) as part of Cosmology Talks\n\n\nAbstract\nAzadeh talks about a "beyo
 nd the standard model" of particle physics framework that appears able to 
 simultaneously...\n\n- provide a particle physics backbone to inflation<br
 >\n- give neutrinos mass<br>\n- generate a dark matter candidate<br>\n- an
 d solve baryogenesis<br>\n\n...thus linking all of these cosmological prob
 lems. The framework can also deal with various particle physics problems\,
  such as the origin of the accidental B-L symmetry in the standard model\,
  the strong CP problem\, and the vacuum stability problem.\n\nSo\, it's sa
 fe to say that if the framework survives scrutiny it is a massive achievem
 ent.\n\nThe framework takes ideas from the "neutrino minimal standard mode
 l"\, specifically a new SU(2) gauge field that couples only to right hande
 d particles and can generate neutrino masses\, as well as provide a dark m
 atter candidate via the lightest right handed neutrino.\n\nIt then combine
 s those ideas with some from Azadeh's earlier work creating the model of g
 auge-flation. Specifically\, it allows for the fields that interact under 
 this new SU(2) gauge symmetry to be actively generated during inflation. T
 his allows the vacuum fluctuations present during inflation\, and which ge
 nerate the curvature perturbation\, to also generate the particles that wi
 ll decay to dark matter and to generate the asymmetry in baryon number tha
 t eventually becomes the matter asymmetry.\n\nWhat's more\, the model make
 s a number of specific predictions. The primordial gravitational waves fro
 m inflation would have some non-Gaussianity and will be chiral. And\, the 
 dark matter mass will be ~GeV - and would thus generate gamma rays in regi
 ons of very large dark matter density.\n\nIt will be fascinating to see ho
 w this framework develops\, and whether numerical reheating studies can sh
 ed light on the various particle production processes that generate the ma
 tter and dark matter during and after inflation...\n\nAzadeh: <a href="htt
 ps://theory.cern/roster/maleknejad-azadeh">https://theory.cern/roster/male
 knejad-azadeh</a>\n\nThe paper: <a href="https://arxiv.org/abs/2012.11516"
 >SU(2)R and its Axion in Cosmology: A common Origin for Inflation\, Cold S
 terile Neutrinos\, and Baryogenesis [2012.11516]</a>\n\n<hr>\n\n<b>Index t
 o Key Parts of the Talk:</b>\n\n[00:00] <a href="https://youtu.be/oiH64cGQ
 yCE?t=0s">Shaun's intro</a>\n\n[00:26] <a href="https://youtu.be/oiH64cGQy
 CE?t=26">Azadeh's opening comments about the paper</a>\n\n[01:10] <a href=
 "https://youtu.be/oiH64cGQyCE?t=70">Q&A: What two things would you want pe
 ople to remember about this talk?</a>\n\n[01:59] <a href="https://youtu.be
 /oiH64cGQyCE?t=119">Q&A: What was the motivation for this work? What has c
 hanged based on this research?</a>\n\n[03:13] <a href="https://youtu.be/oi
 H64cGQyCE?t=193">Getting into the details</a>\n\n[03:51] <a href="https://
 youtu.be/oiH64cGQyCE?t=231">Curious cosmological coincidences</a>\n\n[04:3
 0] <a href="https://youtu.be/oiH64cGQyCE?t=270">Some conceptual issues in 
 the SM of particle physics</a>\n\n[06:17] <a href="https://youtu.be/oiH64c
 GQyCE?t=377">The kinds of questions that Azadeh tried to answer in this pr
 oject</a>\n\n[06:58] <a href="https://youtu.be/oiH64cGQyCE?t=418">What do 
 Gauge Fields do in Inflation?</a>\n\n[07:43] <a href="https://youtu.be/oiH
 64cGQyCE?t=463">Does it come with a cosmological signature?</a>\n\n[08:49]
  <a href="https://youtu.be/oiH64cGQyCE?t=529">How the Inflaton and its Gau
 ge Field are connected to the SM?</a>\n\n[09:44] <a href="https://youtu.be
 /oiH64cGQyCE?t=584">Is there a simple\, elementary\, & minimal set-up that
  can explain these cosmological and particle physics issues?</a>\n\n[11:04
 ] <a href="https://youtu.be/oiH64cGQyCE?t=664">Primordial gravitational wa
 ves</a>\n\n[12:30] <a href="https://youtu.be/oiH64cGQyCE?t=750">Origin of 
 matter asymmetry</a>\n\n[13:36] <a href="https://youtu.be/oiH64cGQyCE?t=81
 6">Baryogenesis via Leptogenesis</a>\n\n[16:56] <a href="https://youtu.be/
 oiH64cGQyCE?t=1016">Origin of neutrino mass and a dark matter particle nat
 ure possibility</a>\n\n[19:54] <a href="https://youtu.be/oiH64cGQyCE?t=119
 4">Why Gauge Fields in Inflation?</a>\n\n[20:43] <a href="https://youtu.be
 /oiH64cGQyCE?t=1243">SU(2)-Axion Model Building</a>\; Gauge-flation and th
 e Chromo-natural model\; now ruled out by the data\; minimal scenario of S
 U(2)-axion inflation\n\n[24:45] <a href="https://youtu.be/oiH64cGQyCE?t=14
 85">Left-Right Symmetric Model</a>\n\n[27:23] <a href="https://youtu.be/oi
 H64cGQyCE?t=1643">SU(2)R-Axion Inflation</a>\n\n[31:02] <a href="https://y
 outu.be/oiH64cGQyCE?t=1862">SU(2)R Gauge Field Production by Axion</a>\n\n
 [34:05] <a href="https://youtu.be/oiH64cGQyCE?t=2045">New Tensorial mode &
  Chiral GWs</a>\n\n[35:04] <a href="https://youtu.be/oiH64cGQyCE?t=2104">N
 ovel Observable Signature: CMB</a>\n\n[35:57] <a href="https://youtu.be/oi
 H64cGQyCE?t=2157">Parity Odd CMB Correlations: TB & EB != 0</a>\n\n[38:11]
  <a href="https://youtu.be/oiH64cGQyCE?t=2291">Right-handed Lepton & Quark
  Production by SU(2)</a>\n\n[39:48] <a href="https://youtu.be/oiH64cGQyCE?
 t=2389">Summary of the Mechanism</a>\n\n[44:34] <a href="https://youtu.be/
 oiH64cGQyCE?t=2674">Compare the Minimal Set-up to SU(2)R-Axion Inflation</
 a>\n\n[46:51] <a href="https://youtu.be/oiH64cGQyCE?t=2811">Q&A: Where to 
 next?</a>\n\n[51:20] <a href="https://youtu.be/oiH64cGQyCE?t=3080">Q&A: ou
 tside of your own research what do you think is the most interesting thing
  in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/28/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Scott Melville and Johannes Noller (Noller: ICG at Portsmouth\; Me
 lville: Cambridge)
DTSTART:20210325T050000Z
DTEND:20210325T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/29
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/29/">Unitarity\, causality & locality: impacts on dark energy and gravi
 ty's speed</a>\nby Scott Melville and Johannes Noller (Noller: ICG at Port
 smouth\; Melville: Cambridge) as part of Cosmology Talks\n\n\nAbstract\nJo
 hannes Noller and Scott Melville talk about their recent paper exploring t
 he impacts of certain positivity bounds on cosmological parameters.\n\nPos
 itivity bounds are restrictions on low energy effective parameters that ar
 ise from requiring the full high energy fundamental theory to satisfy cert
 ain criteria. It is possible to show that if\, e.g. all the interactions o
 f a full theory satisfies unitarity (conservation of information/probabili
 ty)\, causality and locality\, then a specific class of low energy theorie
 s must have the speed of light less than the speed of gravity.\n\nThe spec
 ific interactions Johannes\, Scott (and collaborator Claudia) used to show
  this are interactions between dark energy and standard model matter.\n\nT
 his condition actually ends up lying right in the region that observations
  prefer for this model\, effectively cutting the allowed parameter space i
 n half.\n\nPaper: <a href="https://arxiv.org/abs/2103.06855">https://arxiv
 .org/abs/2103.06855</a><br>\nJohannes Noller: <a href="https://www.icg.por
 t.ac.uk/author/nollerj/">https://www.icg.port.ac.uk/author/nollerj/</a><br
 >\nScott Melville: <a href="http://www.scottamelville.com/">http://www.sco
 ttamelville.com</a><br>\nSupplemental Video: <a href="https://youtu.be/Z3L
 x7VXB78E">https://youtu.be/Z3Lx7VXB78E</a>\n\n<hr>\n\n[00:00] <a href="htt
 ps://youtu.be/F7YaeAyz-yg?t=0s">Shaun's intro</a>\n\n[00:46] <a href="http
 s://youtu.be/F7YaeAyz-yg?t=46">Noller: overview comments about the paper</
 a>\n\n[04:24] <a href="https://youtu.be/F7YaeAyz-yg?t=264">Melville: two t
 akeaway messages to remember about this talk</a>\n\n[05:47] <a href="https
 ://youtu.be/F7YaeAyz-yg?t=347">Noller on the background motivation for thi
 s work</a>\n\n[08:52] <a href="https://youtu.be/F7YaeAyz-yg?t=532">How thi
 s work relates to other papers in this area</a>\n\n[09:05] <a href="https:
 //youtu.be/F7YaeAyz-yg?t=545">A final comment on the motivation for this w
 ork</a>\n\n[10:21] <a href="https://youtu.be/F7YaeAyz-yg?t=621">Q&A: Melvi
 lle comments on importing particle physics knowledge and understanding int
 o cosmology to constrain theories like dark energy</a>\n\n[12:59] <a href=
 "https://youtu.be/F7YaeAyz-yg?t=719">Q&A: Why had this not been done befor
 e?</a> \n\n[13:59] <a href="https://youtu.be/F7YaeAyz-yg?t=839">Getting in
 to the details</a> \n\n[16:41] <a href="https://youtu.be/F7YaeAyz-yg?t=100
 1">The main idea behind the positivity bounds</a>\n\n[16:57] <a href="http
 s://youtu.be/F7YaeAyz-yg?t=1017">A discussion on unitarity\, causality\, a
 nd locality</a>\n\n[19:52] <a href="https://youtu.be/F7YaeAyz-yg?t=1192">S
 ean's insert when editing: comments on the reason for the supplementary vi
 deo</a>\n\n[20:54] <a href="https://youtu.be/F7YaeAyz-yg?t=1254">Buildup t
 o the consequence in this specific model that speed of matter <= speed of 
 gravity </a>\n\n[24:15] <a href="https://youtu.be/F7YaeAyz-yg?t=1455">Noll
 er: How these bounds impact current observational constraints\; a case stu
 dy</a>\n\n[31:16] <a href="https://youtu.be/F7YaeAyz-yg?t=1876">Data const
 raints with the positivity prior</a>\n\n[34:54] <a href="https://youtu.be/
 F7YaeAyz-yg?t=2094">Sean's explanatory comment insert during editing</a>\n
 \n[36:22] <a href="https://youtu.be/F7YaeAyz-yg?t=2182">Noller continuing 
 the talk</a>\n\n[37:34] <a href="https://youtu.be/F7YaeAyz-yg?t=2254">Case
  study: 3 key observations</a>\n\n[43:29] <a href="https://youtu.be/F7YaeA
 yz-yg?t=2609">Melville reponds to a question by Shaun</a>\n\n[46:07] <a hr
 ef="https://youtu.be/F7YaeAyz-yg?t=2767">Final comment by Noller</a>\n\n[4
 6:32] <a href="https://youtu.be/F7YaeAyz-yg?t=2792">Q&A: Where to next?</a
 >\n\n[47:44] <a href="https://youtu.be/F7YaeAyz-yg?t=2864">Q&A: What do yo
 u foresee over the next 24 months?</a>\n\n[53:04] <a href="https://youtu.b
 e/F7YaeAyz-yg?t=3184">Q&A: outside of your own research what do you think 
 is the most interesting thing in cosmology at the moment?</a>\n\n<hr>\n\n<
 b>Supplemental Video:</b>\n\n[00:00] <a href="https://youtu.be/Z3Lx7VXB78E
 ?&t=0">Sean's comments on the reason for this supplementary video</a>\n\n[
 00:46] <a href="https://youtu.be/Z3Lx7VXB78E?&t=46">Melville on the standa
 rd procedure for deriving positivity bounds\; a physical picture</a>\n\n[0
 4:17] <a href="https://youtu.be/Z3Lx7VXB78E?&t=257">Two important things</
 a>\; and what causality buys you\n\n[05:15] <a href="https://youtu.be/Z3Lx
 7VXB78E?&t=315">Unitarity</a>\n\n[06:07] <a href="https://youtu.be/Z3Lx7VX
 B78E?&t=367">Put both ingredients together</a>\; why causality and unitari
 ty come together to give a positivity statement\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/29/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Dan Thomas (Queen Mary University London)
DTSTART:20210406T060000Z
DTEND:20210406T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/30
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/30/">The first model independent cosmological simulations of modified g
 ravity</a>\nby Dan Thomas (Queen Mary University London) as part of Cosmol
 ogy Talks\n\n\nAbstract\nDan Thomas tells us about recent work first creat
 ing a framework for describing modified gravity in a model independent way
  on non-linear scales and then running N-body simulations in that framewor
 k.\n\nThe framework involves finding a correspondence between large scale 
 linear theory where everything is under control and small scale non-linear
  post-Newtonian dynamics. After a lot of care and rigour it boils down to 
 a modified Poisson equation - on both large and small scales (in a particu
 lar gauge).\n\nThe full generality of the modification to the Poisson equa
 tion allows\, essentially\, for a time and space dependent value for Newto
 n's constant. For most modified gravity models\, the first level of deviat
 ion from general relativity can be parameterised in this way (and we know 
 that the deviations from general relativity are small because so far we ha
 ven't found any!!)\n\nThe cosmological simulations are then done by having
  Newton's constant just vary over time (i.e. it is constant in space). Thi
 s allows them to actually do some simulations\, but in future work they wi
 ll go beyond this particular simplification.\n\nThey then compare the simu
 lation results to semi-analytic models like Halofit and ReACT. Halofit is 
 explicitly just applicable to ΛCDM model but does surprisingly well. ReAC
 T however still does much better at fitting e.g. the matter power spectrum
  and model Euclid lensing observables.\n\nFuture work will examine more cl
 osely why ReACT fits so well and aim to improve the fit even better so tha
 t e.g. Euclid and/or the Vera C. Rubin Observatory (LSST) will be able to 
 use this method to constrain modified gravity without needing to run a new
  simulation for every step of a Monte Carlo parameter fit.\n\nTheory frame
 work paper: <a href="https://arxiv.org/abs/2004.13051">https://arxiv.org/a
 bs/2004.13051</a>\n\nSimulation paper: <a href="https://arxiv.org/abs/2103
 .05051">https://arxiv.org/abs/2103.05051</a>\n\nDan: <a href="https://danb
 thomas1.wixsite.com/research">https://danbthomas1.wixsite.com/research</a>
 \n\n<hr>\n\n[00:00] <a href="https://youtu.be/orMFALXtU8g?t=0s">Shaun's in
 tro</a>\n\n[00:40] <a href="https://youtu.be/orMFALXtU8g?t=40">Dan's summa
 ry comments about the paper</a>\n\n[01:15] <a href="https://youtu.be/orMFA
 LXtU8g?t=75">Q&A: What are two takeaway messages to remember about this ta
 lk?</a>\n\n[01:54] <a href="https://youtu.be/orMFALXtU8g?t=114">Q&A: What 
 is the specific motivation for this work? What was unsolved? Why didn't it
  happen earlier?</a>\n\n[03:20] <a href="https://youtu.be/orMFALXtU8g?t=20
 0">Recap summarizing 15 years work: Model independent modified gravity in 
 cosmology</a>\n\n[05:30] <a href="https://youtu.be/orMFALXtU8g?t=330">What
 's the problem? The elephant in the room</a>\n\n[06:06] <a href="https://y
 outu.be/orMFALXtU8g?t=366">Poisson: a clue to the path forward?</a>\n\n[08
 :06] <a href="https://youtu.be/orMFALXtU8g?t=486">Getting into the details
  of the papers (theory and simulation)</a>\n\n[08:22] <a href="https://you
 tu.be/orMFALXtU8g?t=502">A tale of two limits\, and the non-linear scale</
 a>\n\n[11:43] <a href="https://youtu.be/orMFALXtU8g?t=703">A quick aside</
 a>\n\n[12:12] <a href="https://youtu.be/orMFALXtU8g?t=732">GR+LCDM: 2 ingr
 edients</a>: Comment that has relevance on next slide: "there is no interm
 ediate regime in a LCDM cosmology"\n\n[13:01] <a href="https://youtu.be/or
 MFALXtU8g?t=781">Post-Friedmann: "master" equations</a>\n\n[17:19] <a href
 ="https://youtu.be/orMFALXtU8g?t=1039">GR + LCDM</a>\n\n[19:50] <a href="h
 ttps://youtu.be/orMFALXtU8g?t=1190">Back to modified gravity</a>\n\n[21:40
 ] <a href="https://youtu.be/orMFALXtU8g?t=1300">Building towards something
  that's useful for data analysis</a>: 7 simulations\; Table 1 and Figure 2
  in 2103.05051\n\n[27:23] <a href="https://youtu.be/orMFALXtU8g?t=1643">z=
 0 phenomenology</a>: Figure 7 upper left panel in 2103.05051 \n\n[29:28] <
 a href="https://youtu.be/orMFALXtU8g?t=1768">Lensing observables</a>: Figu
 re 9 in 2103.05051\n\n[33:21] <a href="https://youtu.be/orMFALXtU8g?t=2001
 ">Fitting functions</a>: Figure 3\n\n[36:58] <a href="https://youtu.be/orM
 FALXtU8g?t=2218">Fitting functions and Lensing</a>: Figure 10\n\n[40:59] <
 a href="https://youtu.be/orMFALXtU8g?t=2459">Where to next?</a>\n\n[44:00]
  <a href="https://youtu.be/orMFALXtU8g?t=2640">Q&A: outside of your own re
 search\, what do you think is the most interesting thing in cosmology at t
 he moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/30/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Steffen Hagstotz (Stockholm University)
DTSTART:20210422T060000Z
DTEND:20210422T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/31
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/31/">The Hubble parameter measured with Fast Radio Bursts</a>\nby Steff
 en Hagstotz (Stockholm University) as part of Cosmology Talks\n\n\nAbstrac
 t\nSteffen tells us about how the dispersion measure of fast radio bursts 
 (FRBs)can be used to measure the distance to FRBs. Therefore\, if we can f
 ind the host galaxies of FRBs and measure their redshifts we can measure t
 he expansion rate (Hubble parameter) with FRBs.\n\nAnd\, he and his collab
 orators have done just that. At the moment the uncertainty is relatively l
 arge\, but they still get a result within 10% of the more precise measurem
 ents (and consistent with both CMB and supernovae)\, indicating that they'
 re doing the right thing.\n\nIn the near future (less than five years) we'
 ll have (hopefully) more than 500 FRBs and a ~% level accuracy measurement
  of H0. These are exciting times for FRBs!\n\nPaper: <a href="https://arxi
 v.org/abs/2104.04538">https://arxiv.org/abs/2104.04538</a>\n\nSteffen: <a 
 href="https://www.su.se/english/profiles/stha5722-1.400226">https://www.su
 .se/english/profiles/...</a>\n\n<hr>\n\n<strong>Index to Key Parts of the 
 Talk</strong>\n\n[00:00] <a href="https://youtu.be/oHuuzOz68FY?t=0s">Shaun
 's intro</a>\n\n[01:16] <a href="https://youtu.be/oHuuzOz68FY?t=76">Q&A: W
 hat two things would you want people to remember about this talk?</a>\n\n[
 02:06] <a href="https://youtu.be/oHuuzOz68FY?t=126">Q&A: What was the moti
 vation for this work? What was unsolved? Why wasn't this done earlier?</a>
 \n\n[03:47] <a href="https://youtu.be/oHuuzOz68FY?t=227">Getting into the 
 details</a>\n\n[07:40] <a href="https://youtu.be/oHuuzOz68FY?t=460">Overvi
 ew of Proposed Mechanisms</a>\n\n[09:05] <a href="https://youtu.be/oHuuzOz
 68FY?t=545">Known FRBs</a>\n\n[10:04] <a href="https://youtu.be/oHuuzOz68F
 Y?t=604">Dispersion measure</a>: basically\, the integrated electron densi
 ty along the LoS\n\n[12:52] <a href="https://youtu.be/oHuuzOz68FY?t=772">3
  contributions to the dispersion measure</a>: Milky Way\, LSS\, host galax
 y\; modeling for each component\n\n[16:21] <a href="https://youtu.be/oHuuz
 Oz68FY?t=981">The LSS component</a>\n\n[18:14] <a href="https://youtu.be/o
 HuuzOz68FY?t=1094">FRB statistics</a>\n\n[22:16] <a href="https://youtu.be
 /oHuuzOz68FY?t=1336">FRB distance scale</a>: baryon density issues\n\n[26:
 44] <a href="https://youtu.be/oHuuzOz68FY?t=1604">Figure 2 from the 2104.0
 4538 paper</a>: Dispersion measure - redshift relation\n\n[29:47] <a href=
 "https://youtu.be/oHuuzOz68FY?t=1787">Figure 1: Hubble constant constraint
 s</a>\n\n[33:03] <a href="https://youtu.be/oHuuzOz68FY?t=1983">The Future:
  When can FRBs be competitive to measure H0 at the percent level?</a>\n\n[
 34:02] <a href="https://youtu.be/oHuuzOz68FY?t=2042">Figure 3</a>: Expecte
 d joint constraints on H0\, the matter density\, and the mean host dispers
 ion measure contribution from a mock sample of 500 FRBs\n\n[36:04] <a href
 ="https://youtu.be/oHuuzOz68FY?t=2164">Forecast</a>\n\n[36:36] <a href="ht
 tps://youtu.be/oHuuzOz68FY?t=2196">When do we expect to get to 500 events?
 </a>\n\n[39:48] <a href="https://youtu.be/oHuuzOz68FY?t=2388">What can be 
 done with larger samples</a>\n\n[40:26] <a href="https://youtu.be/oHuuzOz6
 8FY?t=2426">Summary</a>\n\n[43:54] <a href="https://youtu.be/oHuuzOz68FY?t
 =2634">What's coming next?</a>\n\n[45:39] <a href="https://youtu.be/oHuuzO
 z68FY?t=2739">A new final question: What current cosmology work do you thi
 nk is particularly under-appreciated by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/31/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Peter Coles (Maynooth University)
DTSTART:20210502T060000Z
DTEND:20210502T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/32
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/32/">The Open Journal of Astrophysics (and why you should be publishing
  in it)</a>\nby Peter Coles (Maynooth University) as part of Cosmology Tal
 ks\n\n\nAbstract\nPeter shares his thoughts on the nature of scientific pu
 blishing and why it is so profitable for the big publishing companies. Pet
 er isn't a fan of the current state and has taken practical steps to impro
 ve it.\n\nThe biggest practical step he's taken is to create The Open Jour
 nal of Astrophysics. This journal is entirely not for profit runs off a $1
 000 a year budget and (unlike for-profit journals) charges nothing to anyo
 ne in the scientific publishing process (authors\, libraries\, etc). And a
 ll the papers it publishes are  100% open access on the arXiv.\n\nThe jour
 nal is a fully functioning journal. If you submit a paper there it will ge
 t peer-reviewed\, if it is accepted it will get cross-referenced at all th
 e relevant places\, will receive a doi and will have its citations counted
  at Inspire\, ADS\, etc.\n\nThe journal needs to be running for three year
 s to get an impact factor\, which won't happen until 2022\, but it will be
  approximately 10-ish (by my extrapolation of his minimum estimate - see v
 ideo for details) which is very high by astrophysics journal standards (if
  you care about that sort of thing).\n\nAnd... they've already published p
 apers by big consortia like LSST and eROSITA.\n\nIt's a baby step in overt
 hrowing the early 20th century system we're still using in 2021\, but it i
 s at least a step. We should embrace it.\n\nPeter: <a href="https://www.ma
 ynoothuniversity.ie/people/peter-coles">https://www.maynoothuniversity.ie/
 people/peter-coles</a><br>\nHis blog: <a href="https://telescoper.wordpres
 s.com/">https://telescoper.wordpress.com/</a><br>\nThe Journal: <a href="h
 ttps://astro.theoj.org/">https://astro.theoj.org/</a>\n\n<hr>\n\n[00:00] <
 a href="https://youtu.be/EjKp-XX7S80?t=0s">Shaun's intro</a>\n\n[01:43] <a
  href="https://youtu.be/EjKp-XX7S80?t=103">Peter's opening comments about 
 the Open Journal of Astrophysics (OJAp) </a>\n\n[02:07] <a href="https://y
 outu.be/EjKp-XX7S80?t=127">Q&A: What two things would you want people to r
 emember about this talk?</a>\n\n[03:25] <a href="https://youtu.be/EjKp-XX7
 S80?t=205">Peter's thanks to Maynooth U for it's support of OJAp</a>\n\n[0
 4:02] <a href="https://youtu.be/EjKp-XX7S80?t=242">The Academic Publishing
  Industry (an exposé!)</a>\n\n[10:10] <a href="https://youtu.be/EjKp-XX7S
 80?t=610">Why Open Access?</a>\n\n[17:40] <a href="https://youtu.be/EjKp-X
 X7S80?t=1060">Open Access: Green\, Gold\, & Diamond</a>: 3 categories of o
 pen access\n\n[20:34] <a href="https://youtu.be/EjKp-XX7S80?t=1234">Peter'
 s comments about the arXiv</a>\n\n[24:51] <a href="https://youtu.be/EjKp-X
 X7S80?t=1491">Why Academic Journals?</a>: the OJAp as an arXiv overlay jou
 rnal to referee the arXiv submissions\, issue a DOI\, register metadata an
 d citations thru the crossref system\n\n[27:16] <a href="https://youtu.be/
 EjKp-XX7S80?t=1636">The Open Journal of Astrophysics</a>: also note sister
  journal - the Journal of Open Source Software\n\n[31:02] <a href="https:/
 /youtu.be/EjKp-XX7S80?t=1862">The author keeps the copyright</a>: with mos
 t journals\, the author signs the copyright to the journal\n\n[32:37] <a h
 ref="https://youtu.be/EjKp-XX7S80?t=1957">The arXiv id is the DOI identifi
 er for all OJAp papers</a>\n\n[32:57] <a href="https://youtu.be/EjKp-XX7S8
 0?t=1977">The paper submission process</a>\n\n[34:45] <a href="https://you
 tu.be/EjKp-XX7S80?t=2085">The Journal blog</a>\n\n[35:50] <a href="https:/
 /youtu.be/EjKp-XX7S80?t=2150">The 6 arXiv astro-ph categories in relation 
 to the OJAp </a>\n\n[37:30] <a href="https://youtu.be/EjKp-XX7S80?t=2250">
 What the OJAp does</a>\n\n[39:06] <a href="https://youtu.be/EjKp-XX7S80?t=
 2346">What the OJAp does differently</a>\n\n[44:00] <a href="https://youtu
 .be/EjKp-XX7S80?t=2640">In two networks: DOAJ and Free Journal Network</a>
 \n\n[44:42] <a href="https://youtu.be/EjKp-XX7S80?t=2682">Some Statistics<
 /a>: includes comments on the acceptance rate\, reviewers\, review process
 \, and issues re fees\n\n[55:23] <a href="https://youtu.be/EjKp-XX7S80?t=3
 323">The future?</a>: much discussion on Journal Impact Factor\n\n[01:04:1
 5] <a href="https://youtu.be/EjKp-XX7S80?t=3855">How to support the OJAp</
 a>: e.g.\, consider submitting papers\, refereeing\, and supporting use of
  the arXiv\; OJAp does not need financial contributions but arXiv does\n\n
 [01:10:26] <a href="https://youtu.be/EjKp-XX7S80?t=4226">Q&A: What current
  cosmology work do you think is particularly under-appreciated by the comm
 unity?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/32/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Eloisa Bentivegna (IBM)
DTSTART:20210525T060000Z
DTEND:20210525T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/33
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/33/">Evolution of a periodic eight-black-hole lattice in numerical rela
 tivity</a>\nby Eloisa Bentivegna (IBM) as part of Cosmology Talks\n\n\nAbs
 tract\nEloisa tells us about her work from 2012 (and following years) cons
 tructing a model universe space-time out of lattices of blackholes. \n\nTh
 e motivation for this is to take a very bottom up approach to cosmology. W
 e know that around isolated objects the correct metric is close to the Sch
 warzschild metric\, so in principle the full metric of the universe should
  be able to be written as a patching together of such metrics. On the othe
 r hand\, the universe on large scales is statistically homogeneous and iso
 tropic and the Friedmann-Robertson-Walker metric appears to fit the data w
 ell. \n\nWhat Eloisa and colleagues wanted to know is how these two paradi
 gms come together\, and they more or less found the answer.\n\nEloisa is a
 lso employed not at a university\, or any other institute we might normall
 y expect to find a cosmologist. She is employed at IBM. However\, she hasn
 't stopped doing cosmology research\, IBM pay her to do numerical relativi
 ty and cosmology. In the video she talks a lot about how this is possible 
 and what IBM want from her as an employee and why this isn't so unique. In
  fact\, she's not even IBM's first numerical relativist!\n\nEloisa: <a hre
 f="https://researcher.watson.ibm.com/researcher/view.php?person=ibm-Eloisa
 .Bentivegna">https://researcher.watson.ibm.com/researcher/view.php?person=
 ibm-Eloisa.Bentivegna</a><br>\n1st paper: <a href="https://arxiv.org/abs/1
 204.3568">[1204.3568] Evolution of a periodic eight-black-hole lattice in 
 numerical relativity</a><br>\n2018 review article on the topic: <a href="h
 ttps://arxiv.org/abs/1801.01083">[1801.01083] Black-Hole Lattices as Cosmo
 logical Models<a><br>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/Ch_irlO
 F0F8?t=0s">Shaun's intro</a>\n\n[02:33] <a href="https://youtu.be/Ch_irlOF
 0F8?t=153">Eloisa's historical overview and motivation for this work</a>\n
 \n[04:54] <a href="https://youtu.be/Ch_irlOF0F8?t=294">Black hole lattices
 </a>\n\n[09:54] <a href="https://youtu.be/Ch_irlOF0F8?t=594">Initial choic
 e between two options</a>: (1) keep a zero extrinsic curvature\, but choos
 e a conformal metric that's not flat\, vs (2) keep a flat conformal metric
  but use a non-zero extrinsic curvature\n\n[12:21] <a href="https://youtu.
 be/Ch_irlOF0F8?t=741">Completely analytic initial conditions - huge simpli
 fication</a>\n\n[14:45] <a href="https://youtu.be/Ch_irlOF0F8?t=885">Speci
 al solution - multiple black holes can be obtained by superimposing the fu
 ndamental solution</a>\n\n[16:20] <a href="https://youtu.be/Ch_irlOF0F8?t=
 980">Six possible configurations</a>\n\n[17:01] <a href="https://youtu.be/
 Ch_irlOF0F8?t=1021">Invert the stereographic projection</a>\n\n[17:54] <a 
 href="https://youtu.be/Ch_irlOF0F8?t=1074">Eloisa's email update subsequen
 t to talk</a>\n\n[19:51] <a href="https://youtu.be/Ch_irlOF0F8?t=1191">The
  8-black hole universe and its full-GR evolution</a>\n\n[21:02] <a href="h
 ttps://youtu.be/Ch_irlOF0F8?t=1262">Tools used: Einstein Toolkit and Cosmo
 Toolkit</a>\n\n[21:29] <a href="https://youtu.be/Ch_irlOF0F8?t=1289">Evolu
 tion equations away from the hypersurfaces</a>\n\n[24:14] <a href="https:/
 /youtu.be/Ch_irlOF0F8?t=1454">Plots of some of the observables measured du
 ring the evolution</a>\n\n[26:26] <a href="https://youtu.be/Ch_irlOF0F8?t=
 1586">Status slide\; main conclusions</a>\n\n[28:28] <a href="https://yout
 u.be/Ch_irlOF0F8?t=1708">Where to from here?</a>\n\n[32:09] <a href="https
 ://youtu.be/Ch_irlOF0F8?t=1929">Q&A: Can inhomogeneous but purely GR effec
 ts model the H0 tension?</a>\n\n[35:56] <a href="https://youtu.be/Ch_irlOF
 0F8?t=2156">Eloisa's role as a computational physicist at IBM</a>\n\n[39:1
 4] <a href="https://youtu.be/Ch_irlOF0F8?t=2354">Comments on her job descr
 iption</a>\n\n[42:05] <a href="https://youtu.be/Ch_irlOF0F8?t=2525">Why wo
 uld a business be interested in basic science? And in cosmology and numeri
 cal relativity?</a>\n\n[45:42] <a href="https://youtu.be/Ch_irlOF0F8?t=274
 2">A historical trivia example of an early numerical relativity paper\; fi
 rst author is an IBMer</a>\n\n[46:58] <a href="https://youtu.be/Ch_irlOF0F
 8?t=2818">Q&A: What do you think is an especially underappreciated aspect 
 of cosmology research being done currently?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/33/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Asta Heinesen and Hayley Macpherson (Canterbury U.\, Cambridge)
DTSTART:20210603T060000Z
DTEND:20210603T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/34
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/34/">How much are local anisotropies biasing our measurements (e.g. H0)
 ?</a>\nby Asta Heinesen and Hayley Macpherson (Canterbury U.\, Cambridge) 
 as part of Cosmology Talks\n\n\nAbstract\nAsta Heinesen and Hayley Macpher
 son tell us about their recent papers developing a formalism for measuring
  local parameters without assuming local isotropy (and homogeneity) and pr
 edicting what we should expect for the parameters in this formalism when w
 e go beyond the isotropic approximation of FRW.\n\nAsta talks about her pa
 per from last year which developed the formalism\, and how a finite number
  of terms can capture all the expected behaviour in the anisotropic lumino
 sity distance\, at each order of redshift.\n\nHayley then talks about how\
 , together\, they applied Asta's formalism to Hayley's fully relativistic 
 simulations of cosmology.\n\nThey show the results for the generalised Hub
 ble\, "deceleration" and jerk parameters. It turns out that when you remov
 e the assumption of isotropy these parameters do indeed depend\, sometimes
  very significantly\, on which direction you look on the sky.\n\nHow much 
 this is impacting our measurements depends\, among other things\, on how f
 ull your sky coverage is.\n\nAsta: <a href="https://inspirehep.net/authors
 /1726735">https://inspirehep.net/authors/1726735</a><br>\nHayley: <a href=
 "https://hayleyjm.github.io/">https://hayleyjm.github.io/</a>\n\nAsta's pa
 per: <a href="https://arxiv.org/abs/2010.06534">https://arxiv.org/abs/2010
 .06534</a><br>\nAsta and Hayley's paper: <a href="https://arxiv.org/abs/21
 03.11918">https://arxiv.org/abs/2103.11918</a>\n\nThe paper Hayley mention
 s where she went as non-linear as possible with full general relativity: <
 a href="https://arxiv.org/abs/1807.01711">https://arxiv.org/abs/1807.01711
 </a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/cbmMhICi-6c?t=0s">Shaun'
 s intro</a>\n\n[01:39] <a href="https://youtu.be/cbmMhICi-6c?t=99">Hayley 
 - quick summary of this work</a>\n\n[02:24] <a href="https://youtu.be/cbmM
 hICi-6c?t=144">Q&A: What two things would you want people to remember abou
 t this talk?</a>\n\n[03:33] <a href="https://youtu.be/cbmMhICi-6c?t=213">A
 sta - background and motivation for this work</a>\n\n[08:12] <a href="http
 s://youtu.be/cbmMhICi-6c?t=492">Review of FLRW models\; "FLRW cosmography"
 </a>\n\n[10:53] <a href="https://youtu.be/cbmMhICi-6c?t=653">The general g
 eometric case</a>\n\n[12:05] <a href="https://youtu.be/cbmMhICi-6c?t=725">
 General luminosity distance "Hubble law"</a>\n\n[15:22] <a href="https://y
 outu.be/cbmMhICi-6c?t=922">Observer congruence</a>\n\n[17:59] <a href="htt
 ps://youtu.be/cbmMhICi-6c?t=1079">Hayley clarifies these are naturally tru
 ncated multipole series</a>\n\n[18:34] <a href="https://youtu.be/cbmMhICi-
 6c?t=1114">Finite set of degrees of freedom</a>\n\n[20:59] <a href="https:
 //youtu.be/cbmMhICi-6c?t=1259">The deceleration parameter</a>\n\n[22:36] <
 a href="https://youtu.be/cbmMhICi-6c?t=1356">Q&A about luminosity distance
  in this work</a>\n\n[25:39] <a href="https://youtu.be/cbmMhICi-6c?t=1539"
 >Hayley - background on the simulations</a>: mimicking as closely as possi
 ble the generality of the formalism\, using numerical relativity\n\n[27:44
 ] <a href="https://youtu.be/cbmMhICi-6c?t=1664">Numerical relativty codes<
 /a>\n\n[28:14] <a href="https://youtu.be/cbmMhICi-6c?t=1694">Numerical rel
 ativity for inhomogeneous and anisotropic cosmology</a>\n\n[30:26] <a href
 ="https://youtu.be/cbmMhICi-6c?t=1826">A note about smoothing</a>\n\n[33:0
 6] <a href="https://youtu.be/cbmMhICi-6c?t=1986">Discussion on gevolution<
 /a>\n\n[35:14] <a href="https://youtu.be/cbmMhICi-6c?t=2114">Comments on F
 igure 1 from the 2103.11918 paper</a>\n\n[37:07] <a href="https://youtu.be
 /cbmMhICi-6c?t=2227">What the cosmological parameters would look like for 
 individual observers in the simulations</a>\n\n[39:13] <a href="https://yo
 utu.be/cbmMhICi-6c?t=2353">Comments on Figure 3 from the 2103.11918 paper<
 /a>\n\n[43:16] <a href="https://youtu.be/cbmMhICi-6c?t=2596">Figures 2 and
  4</a>\n\n[45:08] <a href="https://youtu.be/cbmMhICi-6c?t=2708">Anisotropi
 c contributions</a>: "maximal sky deviation"\n\n[46:29] <a href="https://y
 outu.be/cbmMhICi-6c?t=2789">Exaggerated case of an "unfairly sampled sky"<
 /a>: Figures 2b and 5\n\n[49:49] <a href="https://youtu.be/cbmMhICi-6c?t=2
 989">Main take-aways</a>\n\n[53:19] <a href="https://youtu.be/cbmMhICi-6c?
 t=3199">Wrap-up: additional points not previously mentioned</a>\n\n[56:39]
  <a href="https://youtu.be/cbmMhICi-6c?t=3399">Q&A: What do you think is a
 n especially underappreciated aspect of cosmology research being done curr
 ently?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/34/
END:VEVENT
BEGIN:VEVENT
SUMMARY:H. Gil Marín\, M. Simonovic\, T. Tröster (U Barcelona\, CERN\, U
  Edinburgh)
DTSTART:20210623T060000Z
DTEND:20210623T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/35
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/35/">What is the best way to analyse galaxy clustering data? Panel even
 t</a>\nby H. Gil Marín\, M. Simonovic\, T. Tröster (U Barcelona\, CERN\,
  U Edinburgh) as part of Cosmology Talks\n\n\nAbstract\nThis is a recordin
 g of a panel event run by the organisers of the Cosmology from Home confer
 ence series: <a href="https://cosmologyfromhome.com/" rel="noopener" targe
 t="_blank">https://cosmologyfromhome.com/</a>\n\nThe topic was a compariso
 n of the relative merits of "full shape" and "template" methods to analyse
  galaxy clustering data. Essentially the difference comes down to whether 
 you consider the entire power spectrum as a whole and fit to it in all its
  glory\, or break into separate pieces that encapsulate specific physics e
 ffects.<!--more-->\n\nEach method has its own merits and issues.\n\n<a hre
 f="https://youtu.be/9yVcD9cvzPo">Recorded video on YouTube</a>\n\nThe thre
 e panelists were:\n\nHéctor Gil Marín: <a href="https://www.ub.edu/bispe
 ctrum" rel="noopener" target="_blank">https://www.ub.edu/bispectrum</a>\n\
 nMarko Simonovic: <a href="https://theory.cern/roster/simonovic-marko" rel
 ="noopener" target="_blank">https://theory.cern/roster/simonovic-marko</a>
 \n\nTilman Tröster: <a href="https://tilman.troester.space" rel="noopener
 " target="_blank">https://tilman.troester.space</a>\n\nThe papers that cam
 e up in discussion were:\n\nShapeFit: Extracting the power spectrum shape 
 information in galaxy surveys beyond BAO and RSD: <a href="https://arxiv.o
 rg/abs/2106.07641" rel="noopener" target="_blank">https://arxiv.org/abs/21
 06.07641</a>\n\nThe Completed SDSS-IV Extended Baryon Oscillation Spectros
 copic Survey: N-body Mock Challenge for the Quasar Sample: <a href="https:
 //arxiv.org/abs/2007.09003" rel="noopener" target="_blank">https://arxiv.o
 rg/abs/2007.09003</a>\n\nThe Completed SDSS-IV extended Baryon Oscillation
  Spectroscopic Survey: measurement of the BAO and growth rate of structure
  of the luminous red galaxy sample from the anisotropic power spectrum bet
 ween redshifts 0.6 and 1.0: <a href="https://arxiv.org/abs/2007.08994" rel
 ="noopener" target="_blank">https://arxiv.org/abs/2007.08994</a>\n\n<hr>\n
 \n[00:00] <a href="https://youtu.be/9yVcD9cvzPo&t=0s">Shaun's intro</a>:  
 this is a new format partially as an experiment for Cosmology from Home bu
 t also as an interesting event in it's own right\; the aim is a collaborat
 ive pursuit of understanding\, not a debate\n\n[01:32] <a href="https://yo
 utu.be/9yVcD9cvzPo&t=92">Intro to the panelists' discussion issue</a>: ful
 l-shape vs template methods\; Shaun's video is a little blurry at first\, 
 audio is clear\, panelists' video is clear\n\n[04:09] <a href="https://you
 tu.be/9yVcD9cvzPo&t=249">Héctor Gil Marín introduces himself</a>\n\n[04:
 53] <a href="https://youtu.be/9yVcD9cvzPo&t=293">Marko Simonovic introduce
 s himself</a>\n\n[05:14] <a href="https://youtu.be/9yVcD9cvzPo&t=314">Tilm
 an Tröster introduces himself</a>\n\n[05:33] <a href="https://youtu.be/9y
 VcD9cvzPo&t=333">Shaun: three separate directions to the discussion</a>\n\
 n[06:26] <a href="https://youtu.be/9yVcD9cvzPo&t=387">Héctor: what do we 
 want from a cosmological analysis?</a>\n\n[08:49] <a href="https://youtu.b
 e/9yVcD9cvzPo&t=529">Marko: defending the concept of assuming a model and 
 doing parameter fits to the model\; not a problem\, a strength of the full
  shape analysis approach</a>\n\n[10:52] <a href="https://youtu.be/9yVcD9cv
 zPo&t=652">Responses by Héctor and Tilman</a>\n\n[13:03] <a href="https:/
 /youtu.be/9yVcD9cvzPo&t=783">Marko - what to do when have systematics or b
 ad chi-squared analysis</a>\n\n[14:41] <a href="https://youtu.be/9yVcD9cvz
 Po&t=881">Héctor:  fσ8 overview\; what compressing the variables allows<
 /a>\n\n[18:34] <a href="https://youtu.be/9yVcD9cvzPo&t=1114">Marko - the b
 enefits of full shape analysis</a>\n\n[20:22] <a href="https://youtu.be/9y
 VcD9cvzPo&t=1222">Tilman's agreement and further comments</a>\n\n[20:58] <
 a href="https://youtu.be/9yVcD9cvzPo&t=1258">What info are we gaining by g
 etting extra precision on model parameters? Marko response and Héctor rep
 ly</a>\n\n[25:27] <a href="https://youtu.be/9yVcD9cvzPo&t=1527">Héctor on
  the claim that templates are more model independent\; Marko reply and fur
 ther discussion based on Figures 2 & 3 from 2106.07641</a>\n\n[37:56] <a h
 ref="https://youtu.be/9yVcD9cvzPo&t=2276">Seeking input for a summary stat
 ement at this point of discussion</a>\n\n[42:36] <a href="https://youtu.be
 /9yVcD9cvzPo&t=2556">Héctor on what fσ8 means and what template correcti
 ons may be needed\; discussion</a>\n\n[49:35] <a href="https://youtu.be/9y
 VcD9cvzPo&t=2975">Tilman's input on the issues\; further discussion</a>\n\
 n[52:08] <a href="https://youtu.be/9yVcD9cvzPo&t=3128">Last question: when
  data isn't independent\, how do you combine the data? </a>\n\n[01:00:08] 
 <a href="https://youtu.be/9yVcD9cvzPo&t=3608">If someone in the audience w
 ants to work on this\, what is something they could dive into? Also\, what
  about a template method for the CMB?</a>\n\n[01:03:55] <a href="https://y
 outu.be/9yVcD9cvzPo&t=3835">Comments by attendee and co-author Licia Verde
  (2106.07641)</a>\n\n[01:07:54] <a href="https://youtu.be/9yVcD9cvzPo&t=40
 74">Marko believes next generation surveys will transition to full shape a
 nalysis</a>\n\n[01:08:43] <a href="https://youtu.be/9yVcD9cvzPo&t=4123">In
  what ways you've gained important insights or changed your mind between t
 he pre-discussion and this panel event?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/35/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Harry Goodhew and Gordon Lee (University of Cambridge)
DTSTART:20210802T060000Z
DTEND:20210802T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/36
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/36/">Unitarity constraints on cosmological correlators (valid in *any* 
 flat FLRW metric)</a>\nby Harry Goodhew and Gordon Lee (University of Camb
 ridge) as part of Cosmology Talks\n\n\nAbstract\nHarry Goodhew and Gordon 
 Lee talk about their recent work on “cosmological correlators”.\n\nObs
 ervationally these would be power spectra\, bispectra\, etc\; however on t
 he theory side they find it easier to work with pieces of the “wavefunct
 ion of the universe”\, which are closely related to observational correl
 ation functions.\n\nThey show constraints on the form these correlators ca
 n take that arise from imposing unitarity during inflation. Contrary to pr
 ior expectations these constraints apply not just in space-times that are 
 exactly de Sitter\, but in fact in any flat FLRW space-time.\n\nThe most r
 elevant paper: <a href="https://arxiv.org/abs/2104.06587">https://arxiv.or
 g/abs/2104.06587</a>\n\nHarry: <a href="https://www.maths.cam.ac.uk/person
 /hfg23">https://www.maths.cam.ac.uk/person/hfg23</a><br>\nGordon: <a href=
 "https://www.damtp.cam.ac.uk/person/mhgl2">https://www.damtp.cam.ac.uk/per
 son/mhgl2</a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/Iz9AIE0zJNU?t=0
 s">Shaun's intro and overview</a>\n\n[01:23] <a href="https://youtu.be/Iz9
 AIE0zJNU?t=83">Harry describes the work done in this paper</a>:  (Harry's 
 part of the talk)\n\n[02:01] <a href="https://youtu.be/Iz9AIE0zJNU?t=121">
 Q&A: What two things do  you want people to remember about this talk?</a>\
 n\n[02:34] <a href="https://youtu.be/Iz9AIE0zJNU?t=154">Q&A: The motivatio
 n for this paper\, and why was this work done now and not earlier? </a>\n\
 n[03:48 <a href="https://youtu.be/Iz9AIE0zJNU?t=228">The wave function of 
 the universe</a>\n\n[08:07] <a href="https://youtu.be/Iz9AIE0zJNU?t=487">M
 odel Based Calculations</a>\n\n[10:51] <a href="https://youtu.be/Iz9AIE0zJ
 NU?t=651">Bootstrapping</a>: try to directly calculate what the observable
 s are from fundamental principles\; benefits over the model-based approach
 \n\n[12:38] <a href="https://youtu.be/Iz9AIE0zJNU?t=758">The ultimate goal
  of the cosmological bootstrap program</a>\n\n[12:53] <a href="https://you
 tu.be/Iz9AIE0zJNU?t=773">The most important fundamental principles in the 
 Cosmological Bootstrap</a>\n\n[15:22 <a href="https://youtu.be/Iz9AIE0zJNU
 ?t=922">Q&A: what about multi-field models?</a>\n\n[16:34] <a href="https:
 //youtu.be/Iz9AIE0zJNU?t=994">What is unitarity? (Gordon's part of the tal
 k)</a>\n\n[17:52] <a href="https://youtu.be/Iz9AIE0zJNU?t=1072">How to see
  unitarity?</a>\n\n[19:01] <a href="https://youtu.be/Iz9AIE0zJNU?t=1141">H
 ermitian analyticity</a>\n\n[21:27] <a href="https://youtu.be/Iz9AIE0zJNU?
 t=1287">Discontinuity</a>: (culminating in Figure 1 of paper)\n\n[26:29] <
 a href="https://youtu.be/Iz9AIE0zJNU?t=1589">How do we find out if a field
  is Hermitian analytic?</a>: main result of paper\n\n[28:49] <a href="http
 s://youtu.be/Iz9AIE0zJNU?t=1729">Q&A: What is the implication of these res
 ults?</a>\n\n[29:08] <a href="https://youtu.be/Iz9AIE0zJNU?t=1748">Manifes
 t Locality</a>\n\n[32:12] <a href="https://youtu.be/Iz9AIE0zJNU?t=1932">Co
 mbining unitarity and locality</a>\n\n[33:13] <a href="https://youtu.be/Iz
 9AIE0zJNU?t=1993">What next?</a>\n\n[37:51] <a href="https://youtu.be/Iz9A
 IE0zJNU?t=2271">Q&A on observations that would be a consequence of this wo
 rk</a>\n\n[42:14] <a href="https://youtu.be/Iz9AIE0zJNU?t=2534">Q&A: What 
 is an especially underappreciated aspect of cosmology research being done 
 currently?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/36/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Lloyd E. Knox\, Frances-Yan Cyr-Racine (U of New Mexico\, UC Davis
 )
DTSTART:20210909T060000Z
DTEND:20210909T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/37
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/37/">A subtle cosmological symmetry & mirror dark sector might fix H0</
 a>\nby Lloyd E. Knox\, Frances-Yan Cyr-Racine (U of New Mexico\, UC Davis)
  as part of Cosmology Talks\n\n\nAbstract\nFrancis-Yan Cyr-Racine and Lloy
 d Knox talk about their work with Fei Ge pointing out a symmetry present i
 n most cosmological observables. \n\nThe symmetry involves rescaling (almo
 st) *all* the densities and temperatures in the universe thus leaving any 
 dimensionless observables unchanged. When exploited it might pave a way to
  solving the Hubble tension as it allows one to change H0 without changing
  predictions for other crucial cosmological measurements (most of which ar
 e e.g. temperature\, density\, etc *contrasts* not absolute measurements).
  \n\nThe first major road-block is that the CMB temperature is an absolute
  measurement and a very precise one and thus one can't just casually chang
 e it in one's model\n\nOne way to implement this is therefore to introduce
  a mirror dark sector. This allows the measured photons to be unchanged\, 
 but the overall density of radiation to be rescaled. The mirror world must
  be very similar to our world so that the exact rescaling happens (i.e. th
 ere must be mirror electrons\, mirror protons\, mirror neutrinos\, etc too
 ).\n\nThere's is one remaining (potentially fatal) flaw\, which is that on
 e must also rescale the photon mean free path near to CMB formation as it 
 affect observables and doesn't change just be adding a dark sector. One wa
 y to approach a solution there would be to modify the primordial helium ab
 undance\, as this would change the density of free electrons at the time o
 f CMB formation. However\, this runs into trouble with observations and wo
 uld need a model of nucleosynthesis that allows for this change...\n\n... 
 so this isn't a complete solution at this point\, but definitely something
  to keep an eye on. \n\nMaybe the dark sector affects the helium abundance
 \, maybe it changes the free electron density\, maybe something else can e
 xploit this symmetry and not run into this problem!?\n\nThe model has just
  *one* free parameter though and\, at least phenomenologically\, is able t
 o completely solve the Hubble tension - albeit with the creation of a prim
 ordial helium tension!\n\nCuriously\, the best fit temperature of the dark
  photons is very close to the temperature of the cosmic neutrino backgroun
 d\, suggesting that *maybe* the production of the mirror world is related 
 to neutrino physics somehow.(!?)\n\nLloyd: <a href="https://www.lloydknox.
 com/">https://www.lloydknox.com/</a><br>\nFrancis-Yan: <a href="http://dar
 kuniverse.unm.edu/">https://darkuniverse.unm.edu/</a><br>\nThe paper: <a h
 ref="https://arxiv.org/abs/2107.13000">https://arxiv.org/abs/2107.13000</a
 ><br>\n\n<hr>\n[00:00] <a href="https://youtu.be/Gg7B7bIYf7U?t=0s">Shaun's
  intro</a>\n\n[00:50] <a href="https://youtu.be/Gg7B7bIYf7U?t=50">Summary 
 overview by Lloyd</a>\n\n[02:17] <a href="https://youtu.be/Gg7B7bIYf7U?t=1
 37">Q&A: What two things do you want people to remember about this talk?</
 a>\n\n[03:56] <a href="https://youtu.be/Gg7B7bIYf7U?t=236">What were the m
 otivations for this work?</a>\n\n[05:47] <a href="https://youtu.be/Gg7B7bI
 Yf7U?t=347">Frances-Yan on the motivations and how this work developed</a>
 \n\n[07:56] <a href="https://youtu.be/Gg7B7bIYf7U?t=476">Getting into the 
 details</a>\n\n[08:26] <a href="https://youtu.be/Gg7B7bIYf7U?t=506">The Hu
 bble constant\, measuring angles and redshifts\, insensitivity of redshift
 s/angles to actual distances</a>\n\n[09:34] <a href="https://youtu.be/Gg7B
 7bIYf7U?t=574">Invariance of angles under uniform rescaling of the Hubble 
 rate</a>\n\n[10:26] <a href="https://youtu.be/Gg7B7bIYf7U?t=626">But what 
 if all length scales are uniformly rescaled?</a>\n\n[11:38] <a href="https
 ://youtu.be/Gg7B7bIYf7U?t=698">Basic geometry and dimensional analysis</a>
 \n\n[12:25] <a href="https://youtu.be/Gg7B7bIYf7U?t=745">Special feature o
 f our universe: initial conditions</a>\n\n[14:40] <a href="https://youtu.b
 e/Gg7B7bIYf7U?t=880">The scaling "recipe"</a>\n\n[16:14] <a href="https://
 youtu.be/Gg7B7bIYf7U?t=974">An exact (if unphysical) scaling symmetry</a>\
 n\n[17:40] <a href="https://youtu.be/Gg7B7bIYf7U?t=1060">This recipe works
  - it really leaves the CMB temperature/polarization invariant</a>\n\n[18:
 49] <a href="https://youtu.be/Gg7B7bIYf7U?t=1129">Reality check: Symmetry 
 breaking</a>\n\n[21:05] <a href="https://youtu.be/Gg7B7bIYf7U?t=1265">Disc
 ussion on recombination not being an equilibrium process</a>\n\n[22:40] <a
  href="https://youtu.be/Gg7B7bIYf7U?t=1360">Exploiting the symmetry: Mirro
 r World</a> - plus comments on the many mirror sector studies done for oth
 er reasons than cosmology\n\n[27:07] <a href="https://youtu.be/Gg7B7bIYf7U
 ?t=1627">Adjusting the photon scattering rate</a>\n\n[29:08] <a href="http
 s://youtu.be/Gg7B7bIYf7U?t=1748">Zeroth Test: The exact symmetry</a>\n\n[3
 1:29] <a href="https://youtu.be/Gg7B7bIYf7U?t=1889">First (real!) test: Re
 combination</a>\n\n[32:14] <a href="https://youtu.be/Gg7B7bIYf7U?t=1934">S
 econd test: Compatibility with the cepheid-calibrated distance ladder</a> 
 (Fig. 1 top left panel from the paper)\n\n[34:55] <a href="https://youtu.b
 e/Gg7B7bIYf7U?t=2095">Mirror Sector Freedom</a> (Fig. 2)\n\n[40:37] <a hre
 f="https://youtu.be/Gg7B7bIYf7U?t=2437">Open Questions\; What Comes Next?<
 /a> (comments by both Lloyd and Frances-Yan)\n\n[46:10] <a href="https://y
 outu.be/Gg7B7bIYf7U?t=2770">Q&A: What work being done in cosmology at the 
 moment do you think is particularly underappreciated? (Frances-Yan)</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/37/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Helen Shao\, Francisco Villaescusa-Navarro (Princeton University)
DTSTART:20210927T050000Z
DTEND:20210927T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/38
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/38/">Machine learning unveiling cosmology | subhalo masses and the viri
 al theorem</a>\nby Helen Shao\, Francisco Villaescusa-Navarro (Princeton U
 niversity) as part of Cosmology Talks\n\n\nAbstract\nHelen and Francisco (
 Paco) tell us about their recent work using neural networks to predict the
  masses of subhalos within simulations. They find that the neural network 
 trained on a subset of the subhalos is very good at predicting subhalo mas
 ses for the rest of the data.\n\nRestricting themselves to just three para
 meters\, the radius\, the velocity dispersion and "Vmax" (the maximum circ
 ular velocity of the subhalo) the neural network does almost as well. With
  this as motivation they look for analytic models that might capture what 
 the neural network is seeing. they find a simple three parameter power-law
  does OK using just radius and velocity dispersion as inputs - but a runni
 ng power-law with all three (radius\, velocity dispersion and Vmax) does e
 xtremely well (almost as well as the neural network).\n\nInterestingly\, a
 lthough the neural network starts to perform poorly when extrapolated to m
 asses beyond its training set\, the analytical model manages to still perf
 orm well. This suggests that they might be on to some genuine new physical
  insight about how these parameters combine to determine a subhalo mass.\n
 \nVarious subtleties suggest that this new insight might be related to the
  virial theorem\, but more exploration would be needed to be absolutely su
 re how.\n\nThe work here is part of the CAMELS project\, which has thousan
 ds of N-body and hydrodynamic simulations of the universe from which to tr
 ain neural networks on.\n\nHelen: <a href="https://www.linkedin.com/in/hel
 en-shao-794641169">https://www.linkedin.com/in/helen-shao-794641169</a><br
 >\nPaco:  <a href="https://franciscovillaescusa.github.io/">https://franci
 scovillaescusa.github.io/</a><br>\nCAMELS: <a href="https://www.camel-simu
 lations.org/">https://www.camel-simulations.org/</a><br>\n\nThe paper: <a 
 href="https://arxiv.org/abs/2109.04484">https://arxiv.org/abs/2109.04484</
 a><br>\n\n<hr>\n[00:00] <a href="https://youtu.be/_lIXL4-wkZ0?t=0s">Shaun'
 s intro</a>\n\n[00:59] <a href="https://youtu.be/_lIXL4-wkZ0?t=59">Summary
  overview by Helen</a>\n\n[01:21] <a href="https://youtu.be/_lIXL4-wkZ0?t=
 81">What two things do you want people to remember about this talk? (Paco)
 </a>\n\n[02:06] <a href="https://youtu.be/_lIXL4-wkZ0?t=126">What was the 
 motivation for this work? (Helen)</a>\n\n[03:53] <a href="https://youtu.be
 /_lIXL4-wkZ0?t=233">What are the parameters of interest in this work?</a> 
 \n\n[05:30] <a href="https://youtu.be/_lIXL4-wkZ0?t=330">What some of the 
 parameters mean (Paco)</a>\n\n[07:15] <a href="https://youtu.be/_lIXL4-wkZ
 0?t=435">General Methodology (Helen)</a>\n\n[08:23] <a href="https://youtu
 .be/_lIXL4-wkZ0?t=503">Symbolic Regression</a>\n\n[09:02] <a href="https:/
 /youtu.be/_lIXL4-wkZ0?t=542">Are the parent halo properties relevant in th
 is work? (Paco)</a>\n\n[09:33] <a href="https://youtu.be/_lIXL4-wkZ0?t=573
 ">Continuing with Methodology (Helen)</a>\n\n[13:13] <a href="https://yout
 u.be/_lIXL4-wkZ0?t=793">CAMELS-IllustrisTNG (and TNG100/TNG300) vs CAMELS-
 SIMBA</a>\n\n[15:55] <a href="https://youtu.be/_lIXL4-wkZ0?t=955">Other Te
 sts</a>: higher z\, central subhalos vs satellites\, N-body simulations\, 
 etc\n\n[17:56] <a href="https://youtu.be/_lIXL4-wkZ0?t=1076">The neural ne
 twork found a universal relation</a>\n\n[20:37] <a href="https://youtu.be/
 _lIXL4-wkZ0?t=1237">Testing the analytic equations vs the four simulations
 </a>\n\n[23:00] <a href="https://youtu.be/_lIXL4-wkZ0?t=1380">Conclusions<
 /a>\n\n[24:15] <a href="https://youtu.be/_lIXL4-wkZ0?t=1455">Physical Inte
 rpretation</a>\n\n[26:10] <a href="https://youtu.be/_lIXL4-wkZ0?t=1570">Qu
 estions period</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/38/
END:VEVENT
BEGIN:VEVENT
SUMMARY:James Alvey (U. Amsterdam\, GRAPPA)
DTSTART:20211014T050000Z
DTEND:20211014T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/39
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/39/">Big Bang Nucleosynthesis in 2021</a>\nby James Alvey (U. Amsterdam
 \, GRAPPA) as part of Cosmology Talks\n\n\nAbstract\nJames Alvey tells us 
 about the general state of BBN in 2021.\n\nHe gives a really nice pedagogi
 cal overview of the physics that goes into BBN calculations relevant for 2
 021 observations\, talking through each of the relevant epochs (neutrino d
 ecoupling\, the deuterium bottleneck\, etc).\n\nHe gives particular emphas
 is to the recent LUNA measurements of the D + p →γ + 3He reaction (or d
 euterium + proton goes to photon and 3-Helium). This was previously the so
 urce of greatest uncertainty in predicting the final deuterium abundance o
 f BBN.\n\nFinally\, he talks about the implications of the LUNA measuremen
 ts on possible new physics beyond the standard model\, in particular possi
 ble thermal relics.\n\nThe Talk: <a href="https://youtu.be/Hv8sbRwbSU8">ht
 tps://youtu.be/Hv8sbRwbSU8</a><br>\nThe LUNA paper: <a href="https://www.n
 ature.com/articles/s41586-020-2878-4">https://www.nature.com/articles/s415
 86-020-2878-4</a> (no arXiv version\, I think?)<br>\nJames' original paper
  on thermal relics: <a href="https://arxiv.org/abs/1910.01649">https://arx
 iv.org/abs/1910.01649</a><br>\nAddendum to James' paper analysing implicat
 ions of LUNA: <a href="https://arxiv.org/abs/2107.11232">https://arxiv.org
 /abs/2107.11232</a><br>\n\n<hr>\n\n<b>Index to Key Parts of the Talk:</b><
 br>\n<br>\n[00:00] <a href="https://youtu.be/Hv8sbRwbSU8?t=0s">Shaun's int
 ro</a>\n\n[00:25] <a href="https://youtu.be/Hv8sbRwbSU8?t=25">Summary over
 view by James</a>: a theme: why BBN in 2021 is different than BBN in 2019\
 n\n[01:52] <a href="https://youtu.be/Hv8sbRwbSU8?t=112">What two things do
  you want people to remember about this talk?</a>\n\n[03:07] <a href="http
 s://youtu.be/Hv8sbRwbSU8?t=187">More detail on why this is important for u
 s in 2021</a>\n\n[04:59] <a href="https://youtu.be/Hv8sbRwbSU8?t=299">Comm
 ents on the baryon-photon ratio (used interchangeably with the baryon dens
 ity)</a>\n\n[05:50] <a href="https://youtu.be/Hv8sbRwbSU8?t=350">Getting i
 nto the details: What Can You Measure with BBN in 2021?</a>\n\n[06:23] <a 
 href="https://youtu.be/Hv8sbRwbSU8?t=383">Why an addendum rather than a wh
 ole new paper?</a>\n\n[07:12] <a href="https://youtu.be/Hv8sbRwbSU8?t=432"
 >Why Now? Current Status of BBN</a>\n\n[09:29] <a href="https://youtu.be/H
 v8sbRwbSU8?t=569">Q&A on the primordial lithium abundance</a>\n\n[10:27] <
 a href="https://youtu.be/Hv8sbRwbSU8?t=627">Discussion on nuclear reaction
  rate measurements</a>\n\n[13:09] <a href="https://youtu.be/Hv8sbRwbSU8?t=
 789">What Quantities Does BBN "See"?</a>\n\n[14:00] <a href="https://youtu
 .be/Hv8sbRwbSU8?t=840">The Physics of BBN</a>\n\n[20:40] <a href="https://
 youtu.be/Hv8sbRwbSU8?t=1240">Solving the Cosmology</a>\n\n[23:19] <a href=
 "https://youtu.be/Hv8sbRwbSU8?t=1399">Temperature-to-Time Relation</a>\n\n
 [24:39] <a href="https://youtu.be/Hv8sbRwbSU8?t=1479">Neutrino decoupling<
 /a>\n\n[25:40] <a href="https://youtu.be/Hv8sbRwbSU8?t=1540">Electron-posi
 tron annihilation</a>\n\n[25:50] <a href="https://youtu.be/Hv8sbRwbSU8?t=1
 610">The BBN Reaction Network</a>\n\n[29:43] <a href="https://youtu.be/Hv8
 sbRwbSU8?t=1783">Protons and Neutrons: weak freeze-out</a>\n\n[31:06] <a h
 ref="https://youtu.be/Hv8sbRwbSU8?t=1866">Neutron Decays</a>\n\n[32:52] <a
  href="https://youtu.be/Hv8sbRwbSU8?t=1972">The Bottleneck</a>\n\n[36:38] 
 <a href="https://youtu.be/Hv8sbRwbSU8?t=2198">Producing Helium-4</a>\n\n[4
 4:46] <a href="https://youtu.be/Hv8sbRwbSU8?t=2686">Describing the Network
 </a>\n\n[46:42] <a href="https://youtu.be/Hv8sbRwbSU8?t=2802">LUNA and Deu
 terium</a>\n\n[54:25] <a href="https://youtu.be/Hv8sbRwbSU8?t=3265">Impact
  on Constraints</a>\n\n[58:02] <a href="https://youtu.be/Hv8sbRwbSU8?t=348
 2">Summary and Conclusions</a>\n\n[01:01:56] <a href="https://youtu.be/Hv8
 sbRwbSU8?t=3716">Q&A: What is an especially underappreciated aspect of cos
 mology research being done currently?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/39/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Song Huang and Alexie Leauthaud (Princeton and UCSC)
DTSTART:20211029T050000Z
DTEND:20211029T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/40
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/40/">Stellar mass in a *single* galaxy's outskirts reveals the *whole* 
 cluster mass</a>\nby Song Huang and Alexie Leauthaud (Princeton and UCSC) 
 as part of Cosmology Talks\n\n\nAbstract\nSong Huang and Alexie Leauthaud 
 tell us about their new galaxy cluster finder\, which uses the stellar mas
 s in the outer region of a galaxy as a method to determine the mass of the
  galaxy's cluster.\n\nIt feels a bit like magic (to me) that the stars in 
 individual galaxies can be used to weigh the mass of the whole cluster\, b
 ut like other mass proxies one can devise a scaling relationship between t
 he proxy and the mass - and then the proof is in the empirical pudding.\n\
 nConcerning that pudding\, Song and Alexie's new proxy has a comparably sm
 all scatter in its scaling relation i.e. when compared to the most common 
 proxy for optical surveys\, the richness (i.e. the number of galaxies of a
  certain type in the cluster).\n\nThe most massive clusters found by this 
 method are also more easily modelled than the most massive clusters found 
 via richness. i.e. there seem to be smaller systematic effects that need t
 o be taken account.\n\nSo\, whatever magic is going on\, it's working!\n\n
 Overall\, Song and Alexie think a holistic approach to weighing galaxy clu
 sters is the best way to go\, using richness and stellar mass estimates\, 
 as well as observables from surveys at other wavelengths like X-Ray temper
 ature and the SZ effect on CMB photons that are scattered by hot gas insid
 e clusters.\n\nIt looks like an exciting\, multiwavelength\, future for ga
 laxy cluster cosmology\, which should further open up a very non-linear di
 stance scale to precision tests of the growth of structure\, modified grav
 ity and the primordial density perturbations.\n\nSong: <a href="https://dr
 -guangtou.github.io/">https://dr-guangtou.github.io/</a><br>\nAlexie: <a h
 ref="https://alexie.sites.ucsc.edu/">https://alexie.sites.ucsc.edu/</a><br
 >\nThe paper: <a href="https://arxiv.org/abs/2109.02646">https://arxiv.org
 /abs/2109.02646</a><br>\n<hr>\n\n[00:00] <a href="https://youtu.be/YnMqWwi
 p-gY?t=0s">Shaun's intro to the work</a>\n\n[00:45] <a href="https://youtu
 .be/YnMqWwip-gY?t=0s">Song's summary</a>\n\n[04:50] <a href="https://youtu
 .be/YnMqWwip-gY?t=0s">Two simple thing to remember about the talk</a>\n\n[
 06:16] <a href="https://youtu.be/YnMqWwip-gY?t=0s">What makes this work re
 levant in 2021?</a>\n\n[12:18] <a href="https://youtu.be/YnMqWwip-gY?t=0s"
 >The details...</a>\n\n[40:33] <a href="https://youtu.be/YnMqWwip-gY?t=0s"
 >What comes next?</a>\n\n[46:17] <a href="https://youtu.be/YnMqWwip-gY?t=0
 s">What is particularly underappreciated in cosmology at the moment?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/40/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Hironao Miyatake (Nagoya University\, NASA/Caltech Jet Propulsion 
 Lab)
DTSTART:20211104T050000Z
DTEND:20211104T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/41
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/41/">Hyper Suprime Cam's (HSC) latest constraints on Ωm and σ8!</a>\n
 by Hironao Miyatake (Nagoya University\, NASA/Caltech Jet Propulsion Lab) 
 as part of Cosmology Talks\n\n\nAbstract\nHironao tells about how the Hype
 r Suprime Cam survey collaboration have taken their own data\, and the BOS
 S data from SDSS to do a joint cosmology constraint.\n\nSpecifically\, the
 y take the autocorrelation function of the BOSS galaxies and the cross-cor
 relation of HSC weak lensing data with the BOSS galaxies to break degenera
 cies between cosmology and galaxy bias\, thus allowing the full informatio
 n in the galaxy data to be usable (or at least\, lots more of it).\n\nThey
  work hard to extract information from the small scales in these two probe
 s\, using a cosmology emulator and halo occupation model\, and they includ
 e various consistency tests to show that their analysis is robust. (They a
 lso did the analysis blind\, to avoid human bias as much as possible).\n\n
 The final constraints are comparable to recent similar DES and KiDS constr
 aints\, and consistent with both\, but this analysis have a somewhat diffe
 rent degeneracy in the Ωm and σ8 plane.\n\nPersonally\, I'd now love to 
 see some sort of combined analysis of all three weak lensing probes as the
 y're all consistent with each other and I expect the combined constraints 
 would be in a lot of tension with Planck (especially because of this diffe
 rent degeneracy direction).\n\nHironao: <a href="https://sites.google.com/
 view/hironaomiyatake/home">https://sites.google.com/view/hironaomiyatake/h
 ome</a>\n\nPaper: <a href="https://arxiv.org/abs/2111.02419">https://arxiv
 .org/abs/2111.02419</a>\n<hr>\n\n[00:00] <a href="https://youtu.be/jRhQvue
 e97Q?t=0s">Shaun's introduction</a>\n\n[01:47] <a href="https://youtu.be/j
 RhQvuee97Q?t=107">Two things to remember from the talk</a>\n\n[03:05] <a h
 ref="https://youtu.be/jRhQvuee97Q?t=185s">What is the background?</a>\n\n[
 05:30] <a href="https://youtu.be/jRhQvuee97Q?t=330">Galaxy-galaxy lensing 
 x galaxy-galaxy clustering</a>\n\n[11:59] <a href="https://youtu.be/jRhQvu
 ee97Q?t=719">Subaru Hyper Suprime-Cam (HSC)</a>\n\n[14:32] <a href="https:
 //youtu.be/jRhQvuee97Q?t=872">HSC SSP Survey</a>\n\n[17:10] <a href="https
 ://youtu.be/jRhQvuee97Q?t=1030">G-g lensing and clustering measurements by
  HSC-Y1 and BOSS</a>\n\n[22:33] <a href="https://youtu.be/jRhQvuee97Q?t=13
 53">Emulator-based halo model</a>\n\n[23:55] <a href="https://youtu.be/jRh
 Qvuee97Q?t=1435">Dark Emulator modeling</a>\n\n[26:43] <a href="https://yo
 utu.be/jRhQvuee97Q?t=1603">Modeling galaxy-halo connection</a>\n\n[32:18] 
 <a href="https://youtu.be/jRhQvuee97Q?t=1938">Cosmological inference: syst
 ematic tests</a>\n\n[35:38] <a href="https://youtu.be/jRhQvuee97Q?t=2138">
 Cosmological inference: results</a>\n\n[40:52] <a href="https://youtu.be/j
 RhQvuee97Q?t=2452">What is coming next?</a>\n\n[42:42] <a href="https://yo
 utu.be/jRhQvuee97Q?t=2562">What is underappreciated by the cosmology commu
 nity?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/41/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Tilman Tröster (University of Edinburgh)
DTSTART:20211115T050000Z
DTEND:20211115T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/42
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/42/">Baryon feedback measured via tSZ (cosmological error bars 50% smal
 ler)</a>\nby Tilman Tröster (University of Edinburgh) as part of Cosmolog
 y Talks\n\n\nAbstract\nTilman tells us about his recent work combining KiD
 S cosmic shear measurements and Planck measurements of the thermal Sunyaev
  Zeldovich (tSZ) effect from the cosmic microwave background scattering of
 f hot gas in galaxy clusters and galaxy groups. The long term goal is to u
 se cross-correlation of shear and the tSZ effect to help constrain (or ess
 entially measure) baryon feedback and thus push to smaller scales.\n\nIn t
 his work\, they don't push to smaller scales\, partially because doing so 
 would require many more careful checks and partially because Planck's beam
  isn't small enough to make it worthwhile. However they still gain approxi
 mately two times tighter constraints in the Ωm vs σ8 plane compared to s
 hear alone because of the additional information available in tSZ about wh
 ere matter clusters\, and what the baryons are actually up to.\n\nThe resu
 lts themselves are awesome (error bars shrinking by a factor of two is imp
 ressive enough) but also are a great proof of concept that we can measure 
 baryon feedback like this (and don't have to necessarily predict it entire
 ly from first principles). \n\nWith CMB Stage 4 beam sizes and sky coverag
 e\, it will be fascinating to see what can be done with this method...\n\n
 Tilman: <a href="https://tilman.troester.space/">https://tilman.troester.s
 pace/</a><br>\nPaper: <a href="https://arxiv.org/abs/2109.04458">https://a
 rxiv.org/abs/2109.04458</a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/O
 sX5PNxnkl4?t=0s">Shaun's intro</a>\n\n[00:46] <a href="https://youtu.be/Os
 X5PNxnkl4?t=46">Summary overview by Tilman</a>\n\n[02:04] <a href="https:/
 /youtu.be/OsX5PNxnkl4?t=124">What two things do you want people to remembe
 r about this talk?</a>\n\n[02:56] <a href="https://youtu.be/OsX5PNxnkl4?t=
 176">More background detail on why this is being done now</a>\n\n[07:13] <
 a href="https://youtu.be/OsX5PNxnkl4?t=433">Details of what was done in th
 e paper</a>\n\n[10:02] <a href="https://youtu.be/OsX5PNxnkl4?t=602">Q&A on
  the Cosmic Infrared Background importance in this work</a>\n\n[11:33] <a 
 href="https://youtu.be/OsX5PNxnkl4?t=693">Usage of data from KiDS (weak le
 nsing survey designed to optimize for gravitational lensing cosmology\; fu
 ll overlap with VIKING infrared survey)</a>\n\n[13:11] <a href="https://yo
 utu.be/OsX5PNxnkl4?t=791">Plot of measured cross-correlation as angular po
 wer spectrum between KiDS-1000 and Planck data</a>\n\n[13:55] <a href="htt
 ps://youtu.be/OsX5PNxnkl4?t=835">Modelling</a>\n\n[16:59] <a href="https:/
 /youtu.be/OsX5PNxnkl4?t=1019">HMx paper 2005.00009 hydrodynamical halo mod
 el for weak-lensing cross-correlations</a>\n\n[20:08] <a href="https://you
 tu.be/OsX5PNxnkl4?t=1208">Applying the model to the data</a>\n\n[22:40] <a
  href="https://youtu.be/OsX5PNxnkl4?t=1360">Joint analysis with cosmic she
 ar\; Fig. 5\, 6\, 9 from paper</a>\n\n[30:01] <a href="https://youtu.be/Os
 X5PNxnkl4?t=1801">Systematics and results plots\; Fig. 3\, 7 from paper</a
 >\n\n[37:03] <a href="https://youtu.be/OsX5PNxnkl4?t=2223">Baryon feedback
  - intrinsic alignment interaction</a>\n\n[42:21] <a href="https://youtu.b
 e/OsX5PNxnkl4?t=2541">Where to next?</a>\n\n[43:46] <a href="https://youtu
 .be/OsX5PNxnkl4?t=2626">What current cosmology work is particularly under-
 appreciated by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/42/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Charles Dalang (University of Geneva)
DTSTART:20211124T050000Z
DTEND:20211124T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/43
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/43/">The 4.9σ dipole anisotropy tension *might* be astrophysical redsh
 ift evolution</a>\nby Charles Dalang (University of Geneva) as part of Cos
 mology Talks\n\n\nAbstract\nCharles tells us about his recent work with Ca
 mille Bonvin on the dipole anisotropy tension. \n\nWe expect there to be d
 ipoles in most observables because of our motion through the (statisticall
 y) homogeneous and isotropic universe. However\, there appears to be a 4.9
 σ tension between the magnitude of the dipole as measured from the CMB an
 d as measured from quasars in the local-ish universe.\n\nCharles and Camil
 le have looked at the redshift evolution of the relevant physics that goes
  into the local-ish prediction for the dipole. They find that if both the 
 magnification bias and the spectral index of the source change with redshi
 ft\, the naive expectation for the magnitude of the dipole\, given a parti
 cular velocity can change.\n\nTherefore\, they re-derive an alternative fo
 rmula that is explicitly redshift dependent and more easily applied direct
 ly to redshift dependent observations\n\nThey look at a sample of quasars 
 observed by eBOSS to see how the relevant quantities change with redshift.
  They do change and Charles and Camille show that *if* the larger observed
  sample of quasars did have the same redshift dependence then the tension 
 would be substantially reduced.\n\nIt is more difficult to measure the ful
 l redshift dependence of the larger quasar sample used to measure the dipo
 le as they haven't all been measured with one telescope/survey. It is uncl
 ear what the actual tension would be between theory and observation were o
 ne to be able to take the effect C&C point out into account.\n\nTime will 
 tell with more detailed and larger surveys...\n\nCharles: <a href="https:/
 /cosmology.unige.ch/users/charles-dalang">https://cosmology.unige.ch/users
 /charles-dalang</a>\n\nPaper: <a href="https://arxiv.org/abs/2111.03616">h
 ttps://arxiv.org/abs/2111.03616</a>\n\n<hr>\n\n[00:00] <a href="https://yo
 utu.be/xAuaE32E6Vc?t=0s">Shaun's introduction</a>\n\n[00:58] <a href="http
 s://youtu.be/xAuaE32E6Vc?t=58">Charles' introduction</a>\n\n[01:53] <a hre
 f="https://youtu.be/xAuaE32E6Vc?t=113">Two simple things to take away from
  the talk</a>\n\n[02:36] <a href="https://youtu.be/xAuaE32E6Vc?t=156">What
  is the background?</a>\n\n[05:05] <a href="https://youtu.be/xAuaE32E6Vc?t
 =305">Source number count kinematic dipole</a>\n\n[06:15] <a href="https:/
 /youtu.be/xAuaE32E6Vc?t=375">Theory</a>\n\n[10:50] <a href="https://youtu.
 be/xAuaE32E6Vc?t=650">What are the details?</a>\n\n[11:04] <a href="https:
 //youtu.be/xAuaE32E6Vc?t=664">Integrating over comoving distance</a>\n\n[1
 3:22] <a href="https://youtu.be/xAuaE32E6Vc?t=802">Integrating over redshi
 ft\; Figs. 1 and 2 from paper</a>\n\n[17:32] <a href="https://youtu.be/xAu
 aE32E6Vc?t=1052">Redshift evolution\; Figs. 3 and 4</a>\n\n[20:43] <a href
 ="https://youtu.be/xAuaE32E6Vc?t=1243">Theoretical Prediction\; Fig. 6</a>
 \n\n[22:25] <a href="https://youtu.be/xAuaE32E6Vc?t=1345">Playing around\;
  Figs. 7 and 8</a>\n\n[29:31] <a href="https://youtu.be/xAuaE32E6Vc?t=1771
 ">Conclusions</a>\n\n[30:33] <a href="https://youtu.be/xAuaE32E6Vc?t=1833"
 >What comes next?</a>\n\n[32:55] <a href="https://youtu.be/xAuaE32E6Vc?t=1
 975">What is under-appreciated by the cosmology community as a whole?</a>\
 n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/43/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Dillon Brout\, Adam Riess\, Dan Scolnic (Harvard Smithsonian Cente
 r for Astrophysics\, Johns Hopkins U\, Duke U)
DTSTART:20211209T050000Z
DTEND:20211209T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/44
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/44/">SH0ES | H₀ = 73.0 ± 1.0 km s⁻¹ Mpc⁻¹</a>\nby Dillon Brout
 \, Adam Riess\, Dan Scolnic (Harvard Smithsonian Center for Astrophysics\,
  Johns Hopkins U\, Duke U) as part of Cosmology Talks\n\n\nAbstract\nDillo
 n Brout\, Adam Riess and Dan Scolnic talk about the latest SH0ES measureme
 nt of the Hubble parameter\, making use of the new Pantheon+ supernovae da
 ta set.\n\nThe measurement accuracy has reached ± 1.0 km s⁻¹ Mpc⁻¹\
 , and they analysed the data in 67 different possible ways and every time 
 reach a result that is in significant tension with Planck + ΛCDM. Their b
 aseline analysis\, the one with the best χ² with the fewest free paramet
 ers\, is now in 5σ tension\, on its own\, with Planck.\n\nIt isn't clear 
 where the solution to the Hubble tension will come from\, but the fact tha
 t all local measurements of H₀ come in above Planck\, and that the most 
 accurate measurement is now in 5σ tension is very interesting. It's worth
  also noting that the prediction from the early universe + ΛCDM doesn't r
 ely uniquely on Planck. Other CMB experiments give the same small value\, 
 and even just Big Bang Nucleosynthesis and local Baryon Acoustic Oscillati
 on measurements\, combined with ΛCDM give a small value of H₀. \n\nSo\,
  if this isn't evidence of new physics in cosmology\, it will be a very st
 range series of errors that is causing it.\n\n<a href="https://youtu.be/WF
 KzEtScvw4">Talk video</a>\n\nDillon: <a href="http://djbrout.github.io/">h
 ttp://djbrout.github.io/</a><br>\nAdam: <a href="https://www.stsci.edu/~ar
 iess/">https://www.stsci.edu/~ariess/</a><br>\nDan: <a href="https://schol
 ars.duke.edu/person/dscolnic">https://scholars.duke.edu/person/dscolnic</a
 ><br>\n\nThe paper: <a href="https://arxiv.org/abs/2112.04510">https://arx
 iv.org/abs/2112.04510</a>\n\n<hr>\n\n[00:00] <a href="https://www.youtube.
 com/watch?v=WFKzEtScvw4&t=0s">Shaun's introduction</a>\n\n[01:06] <a href=
 "https://www.youtube.com/watch?v=WFKzEtScvw4&t=66s">Adam's introduction</a
 >\n\n[02:36] <a href="https://www.youtube.com/watch?v=WFKzEtScvw4&t=156s">
 Dan and Dillon's additional thoughts</a>\n\n[03:21] <a href="https://www.y
 outube.com/watch?v=WFKzEtScvw4&t=201s">Two things to take away from the pa
 per(s) (Adam & Dan)</a>\n\n[05:04] <a href="https://youtu.be/WFKzEtScvw4?t
 =304">Shaun's intro for diving into the details</a>\n\n[05:21] <a href="ht
 tps://youtu.be/WFKzEtScvw4?t=321">Pantheon+ Overview: 7 Papers Improving u
 pon every major facet of Type Ia SN Cosmology (Dan)</a>\n\n[08:14] <a href
 ="https://youtu.be/WFKzEtScvw4?t=494">The Pantheon+ Compilation of SNe (Di
 llon)</a>\n\n[11:12] <a href="https://www.youtube.com/watch?v=WFKzEtScvw4&
 t=672s">SH0ES 2021 details: First Major Update Since 2016 (>1000 orbits HS
 T) (Adam)</a>\n\n[12:53] <a href="https://youtu.be/WFKzEtScvw4?t=773">SH0E
 S Distance Ladder Data Sources (Adam)</a>\n\n[17:59] <a href="https://yout
 u.be/WFKzEtScvw4?t=1079">New Cepheid Measurements (Adam)</a>\n\n[19:11] <a
  href="https://youtu.be/WFKzEtScvw4?t=1151">PSF Photometry\, Artificial st
 ars in pipeline measure backgrounds (Adam)</a>\n\n[19:34] <a href="https:/
 /youtu.be/WFKzEtScvw4?t=1174">Photometry Validation Tests (Adam)</a>\n\n[2
 0:48] <a href="https://youtu.be/WFKzEtScvw4?t=1248">Baseline Fit: 3200 Cep
 heids\, 300 SN\, non-diagonal covariance - 5 free params (Adam)</a>\n\n[22
 :29] <a href="https://youtu.be/WFKzEtScvw4?t=1349">Baseline Fit: H0=73.04 
 ± 1.04 km s⁻¹ Mpc⁻¹\, w/ systematics\n\n[24:50] <a href="https://yo
 utu.be/WFKzEtScvw4?t=1490">Baseline Fit: Geometric anchor consistency (Ada
 m)</a>\n\n[26:57] <a href="https://youtu.be/WFKzEtScvw4?t=1617">Baseline F
 it Residuals vs Background/Crowding (Adam)</a>\n\n[28:51] <a href="https:/
 /youtu.be/WFKzEtScvw4?t=1731">How to: Simultaneous H0 and H(z) (Adam\, Dil
 lon-public code will be available)</a>\n\n[32:13] <a href="https://youtu.b
 e/WFKzEtScvw4?t=1933">Analysis Variants: 12 categories\, 67 variants\, bif
 urcations\, extensions\, etc (Adam)</a>\n\n[36:12] <a href="https://youtu.
 be/WFKzEtScvw4?t=2172">SH0ES Error Budget (Adam)</a>\n\n[37:00] <a href="h
 ttps://www.youtube.com/watch?v=WFKzEtScvw4&t=2220s">Main Conclusions\, Sum
 mary of new details (Adam)</a>\n\n[37:45] <a href="https://www.youtube.com
 /watch?v=WFKzEtScvw4&t=2265s">Additional thoughts and discussion (Dan\, Ad
 am)</a>\n\n[41:41] <a href="https://www.youtube.com/watch?v=WFKzEtScvw4&t=
 2501s">Where to next? (All)</a>\n\n[46:14] <a href="https://www.youtube.co
 m/watch?v=WFKzEtScvw4&t=2774s">What do you think is the solution to the Hu
 bble tension?(All)</a>\n\n[50:28] <a href="https://www.youtube.com/watch?v
 =WFKzEtScvw4&t=3028s">What do you think is under-appreciated by the cosmol
 ogy community? (Adam\, Dan)</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/44/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Paco Villaescusa (Simons Foundation)
DTSTART:20220110T050000Z
DTEND:20220110T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/45
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/45/">CAMELS - Data Release & Series Introduction</a>\nby Paco Villaescu
 sa (Simons Foundation) as part of Cosmology Talks\n\n\nAbstract\nThis is t
 he first video in a series of videos covering research that the CAMELS gro
 up have done. CAMELS are applying machine learning to cosmology\, using a 
 suite of 1000s of simulations to train neural networks\, see what the netw
 orks learn and then try to unveil what it learned in a way we mere humans 
 can understand.\n\nThis video does a brief intro to CAMELS as well as the 
 data release (and how to access the data).\n\nCAMELS: <a href="https://www
 .camel-simulations.org/">https://www.camel-simulations.org/</a><br>\nTalk 
 video: <a href="https://youtu.be/6Vgc72a_VpY">https://youtu.be/6Vgc72a_VpY
 </a><br>\nPaper: <a href="https://arxiv.org/abs/2201.01300">https://arxiv.
 org/abs/2201.01300</a>\n\nCAMELS talk at Cosmology from Home: <a href="htt
 ps://www.youtube.com/watch?v=NxR_kDlHhGM&amp\;t=0s">https://www.youtube.co
 m/watch?v=NxR_kDlHhGM&amp\;t=0s</a><br>\nPlaylist of CAMELS video series: 
 <a href="https://www.youtube.com/playlist?list=PLvy7h0l2rJHq03inVPqYnC3llK
 t0IwwLT">https://www.youtube.com/playlist?list=PLvy7h0l2rJHq03inVPqYnC3llK
 t0IwwLT</a>\n\n<hr>\n\n<strong>Index to Key Parts of the Talk</strong>\n\n
 [00:00] <a href="https://youtu.be/6Vgc72a_VpY?t=0s">Shaun's introduction t
 o the 8-video series</a>\n\n[01:02] <a href="https://youtu.be/6Vgc72a_VpY?
 t=62s">What is CAMELS?</a>\n\n[01:39] <a href="https://youtu.be/6Vgc72a_Vp
 Y?t=99s">What can CAMELS do that normal cosmology can't?</a>\n\n[03:10] <a
  href="https://youtu.be/6Vgc72a_VpY?t=190s">Getting into the details (simu
 lations\, algorithms\, code\, parameters)</a>\n\n[05:25] <a href="https://
 youtu.be/6Vgc72a_VpY?t=325s">CAMELS in relation to IllustrisTNG\, SIMBA</a
 >\n\n[06:31] <a href="https://youtu.be/6Vgc72a_VpY?t=391s">Accessing the d
 ata</a>\n\n[07:22] <a href="https://youtu.be/6Vgc72a_VpY?t=442s">Technical
  documentation</a>\n\n[08:00] <a href="https://youtu.be/6Vgc72a_VpY?t=480s
 ">Using Binder</a>\n\n[08:25] <a href="https://youtu.be/6Vgc72a_VpY?t=505s
 ">Machine learning tutorials</a>\n\n[09:34] <a href="https://youtu.be/6Vgc
 72a_VpY?t=574s">Terminology definitions</a>\n\n[11:44] <a href="https://yo
 utu.be/6Vgc72a_VpY?t=704s">Using Jupyter Notebook example</a>\n\n[13:32] <
 a href="https://youtu.be/6Vgc72a_VpY?t=812s">What's been done up to now?</
 a>\n\n[14:45] <a href="https://youtu.be/6Vgc72a_VpY?t=885s">Future directi
 ons</a>\n\n[16:43] <a href="https://youtu.be/6Vgc72a_VpY?t=1003s">How to g
 et involved</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/45/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Paco Villaescusa (Simons Foundation)
DTSTART:20220111T050000Z
DTEND:20220111T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/46
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/46/">Cosmology with a single galaxy!? (CAMELS)</a>\nby Paco Villaescusa
  (Simons Foundation) as part of Cosmology Talks\n\n\nAbstract\nPaco tells 
 us about how CAMELS have used machine learning to be able to predict\, wit
 h a single galaxy's properties\, the value of Ωm used to simulate the gal
 axy. \n\nThis is fascinating and if a real physical effect has some far-re
 aching consequences.\n\n- We might one day be able to learn cosmological p
 arameters by studying the Milky Way<br>\n- Running a hydrodynamical simula
 tion with the wrong Ωm would mean\, in principle\, that you'll never repr
 oduce the exact properties of a galaxy correctly.\n\nCAMELS: <a href="http
 s://www.camel-simulations.org/">https://www.camel-simulations.org/</a><br>
 \nTalk video: <a href="https://youtu.be/4AfjqEj_MaI">https://youtu.be/4Afj
 qEj_MaI</a><br>\nPaco: <a href="https://franciscovillaescusa.github.io/">h
 ttps://franciscovillaescusa.github.io/</a><br>\nPaper: <a href="https://ar
 xiv.org/abs/2201.02202">https://arxiv.org/abs/2201.02202</a>\n\nCAMELS ser
 ies overview: <a href="https://www.youtube.com/watch?v=6Vgc72a_VpY&amp\;t=
 0s">https://www.youtube.com/watch?v=6Vgc72a_VpY&amp\;t=0s</a><br>\nPlaylis
 t of CAMELS video series: <a href="https://www.youtube.com/playlist?list=P
 Lvy7h0l2rJHq03inVPqYnC3llKt0IwwLT">https://www.youtube.com/playlist?list=P
 Lvy7h0l2rJHq03inVPqYnC3llKt0IwwLT</a>\n\n<hr>\n\n<strong>Index to Key Part
 s of the Talk></strong>\n\n[00:00] <a href="https://youtu.be/4AfjqEj_MaI?t
 =0s">Shaun's intro</a>\n\n[01:06] <a href="https://youtu.be/4AfjqEj_MaI?t=
 66s">Paco's introductory comments</a>\n\n[01:41] <a href="https://youtu.be
 /4AfjqEj_MaI?t=101s">What questions were you trying to answer?</a>\n\n[02:
 21] <a href="https://youtu.be/4AfjqEj_MaI?t=141s">Getting into the details
 </a>\n\n[04:17] <a href="https://youtu.be/4AfjqEj_MaI?t=257s">Training the
  neural network and testing</a>\n\n[05:56] <a href="https://youtu.be/4Afjq
 Ej_MaI?t=356s">How correlated are the error bars?</a>\n\n[06:50] <a href="
 https://youtu.be/4AfjqEj_MaI?t=410s">Does it work for other parameters bes
 ides Ωm?</a>\n\n[07:17] <a href="https://youtu.be/4AfjqEj_MaI?t=437s">Doe
 s this really work for all galaxies?</a>\n\n[09:10] <a href="https://youtu
 .be/4AfjqEj_MaI?t=550s">The galaxy properties that are responsible for thi
 s result</a>\n\n[16:17] <a href="https://youtu.be/4AfjqEj_MaI?t=977s">What
  happens if you train on Illustris and test on SIMBA?</a>\n\n[18:07] <a hr
 ef="https://youtu.be/4AfjqEj_MaI?t=1087s">What about environmental depende
 nce?</a>\n\n[20:14] <a href="https://youtu.be/4AfjqEj_MaI?t=1214s">Conclus
 ions and what should the cosmology community take away from this?</a>\n\n[
 20:54] <a href="https://youtu.be/4AfjqEj_MaI?t=1254s">What would you want 
 to discuss with other experts?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/46/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Jay Wadekar (Institute of Advanced Study)
DTSTART:20220112T050000Z
DTEND:20220112T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/47
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/47/">Galaxy cluster mass estimates improved with AI (CAMELS)</a>\nby Ja
 y Wadekar (Institute of Advanced Study) as part of Cosmology Talks\n\n\nAb
 stract\nJay tells us about how he has used the CAMELS suit of simulations 
 to improve upon existing galaxy cluster scaling relations (i.e. trends we 
 use to measure cluster masses using observational probes). \n\nOne example
  is using the concentration of ionised gas in a cluster to add a little bi
 t more precision to a Sunyaev Zeldovich effect - mass scaling relation. Th
 e value of the concentration makes a small change to the prediction.\n\nJa
 y specifically uses symbolic regression (or similar algorithms) to find ex
 pressions that link the properties of interest (e.g. mass\, concentration 
 and SZ effect)\, thus allowing us as human beings to also gain some intuit
 ion from what the machine finds.\n\nJay: <a href="https://jaywadekar.githu
 b.io/">https://jaywadekar.github.io/</a><br>\nPaper: <a href="https://arxi
 v.org/abs/2201.01305">https://arxiv.org/abs/2201.01305</a><br>\nTalk video
 : <a href="https://youtu.be/w_ohkLYMSzs">https://youtu.be/w_ohkLYMSzs</a>\
 n\nCAMELS playlist: <a href="https://www.youtube.com/watch?v=6Vgc72a_VpY&a
 mp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT&amp\;t=0s">https://www.youtube
 .com/watch?v=6Vgc72a_VpY&amp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT&amp\
 ;t=0s</a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/w_ohkLYMSzs?t=0s">S
 haun's Intro</a>\n\n[00:59] <a href="https://youtu.be/w_ohkLYMSzs?t=59s">J
 ay's opening comments</a>\n\n[01:48] <a href="https://youtu.be/w_ohkLYMSzs
 ?t=108s">What is the motivation for this work?</a>\n\n[03:17] <a href="htt
 ps://youtu.be/w_ohkLYMSzs?t=197s">Comparison of Machine Learning approache
 s\, starting with deep neural networks</a>\n\n[03:44] <a href="https://you
 tu.be/w_ohkLYMSzs?t=224s">Symbolic regression overview</a>\n\n[05:40] <a h
 ref="https://youtu.be/w_ohkLYMSzs?t=340s">How symbolic regression was used
  in this work</a>\n\n[08:16] <a href="https://youtu.be/w_ohkLYMSzs?t=496s"
 >Question about the 25 Mpc box size in CAMELS</a>\n\n[11:01] <a href="http
 s://youtu.be/w_ohkLYMSzs?t=661s">Is the result robust w.r.t. feedback pres
 criptions?</a>\n\n[13:02] <a href="https://youtu.be/w_ohkLYMSzs?t=782s">Im
 proving the domain of validity of scaling relations</a>\n\n[14:59] <a href
 ="https://youtu.be/w_ohkLYMSzs?t=899s">Summary and takeaway</a>\n\n[16:01]
  <a href="https://youtu.be/w_ohkLYMSzs?t=961s">What would you like to talk
  about with other experts?</a>\n\n[16:43] <a href="https://youtu.be/w_ohkL
 YMSzs?t=1003s">Application to other scaling relations?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/47/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Andrina Nicola (Princeton University)
DTSTART:20220113T050000Z
DTEND:20220113T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/48
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/48/">Electron density breaks baryon-cosmology degeneracy (CAMELS)</a>\n
 by Andrina Nicola (Princeton University) as part of Cosmology Talks\n\n\nA
 bstract\nAndrina tells us about her work using CAMELS and machine learning
  to constrain baryon feedback using the electron density power spectrum. \
 n\nThe electron density is not itself an observable thing\, but it is a go
 od proxy for observable things like the thermal Sunyaev Zeldovich effect a
 nd Fast Radio Burst dispersion (or they are good proxies for the electron 
 density).\n\nAndrina is able to get nice constraints on baryon feedback an
 d cosmological parameters within the CAMELS simulations. This sort of obse
 rvational probe of baryon feedback is going to be an important tool for co
 smologists if we want to use smaller scales to do cosmology\, and the sort
  of connections spotted by Andrina and CAMELS will be valuable for improvi
 ng these probes.\n\nAndrina: <a href="https://www.astro.princeton.edu/~ani
 cola/">https://www.astro.princeton.edu/~anicola/</a><br>\nPaper: <a href="
 https://arxiv.org/abs/2201.04142">https://arxiv.org/abs/2201.04142</a><br>
 \nVideo of talk: <a href="https://youtu.be/D_CLangkIDE">https://youtu.be/D
 _CLangkIDE</a>\n\nCAMELS playlist: <a href="https://youtu.be/D_CLangkIDE&a
 mp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT">https://youtu.be/D_CLangkIDE&
 amp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT</a>\n\n<hr>\n\n[00:00] <a hre
 f="https://youtu.be/D_CLangkIDE?t=0s">Shaun's intro</a>\n\n[00:51] <a href
 ="https://youtu.be/D_CLangkIDE?t=51s">Andrina's overview comments</a>\n\n[
 01:40] <a href="https://youtu.be/D_CLangkIDE?t=100s">What is the motivatio
 n for this work?</a>\n\n[03:44] <a href="https://youtu.be/D_CLangkIDE?t=22
 4s">Getting into the details</a>\n\n[04:03] <a href="https://youtu.be/D_CL
 angkIDE?t=243s">Constraining cosmology & baryon physics from 2pt-functions
  (X-ray\, tSZ\, FRBs)</a>\n\n[04:44] <a href="https://youtu.be/D_CLangkIDE
 ?t=284s">How well can the electron density power spectrum constrain both c
 osmology and baryonic feedback?</a>\n\n[05:32] <a href="https://youtu.be/D
 _CLangkIDE?t=332s">Simulations (IllustrisTNG and SIMBA)</a>\n\n[06:35] <a 
 href="https://youtu.be/D_CLangkIDE?t=395s">Plots of the electron power spe
 ctra from IllustrisTNG & SIMBA simulations (Fig. 1 in paper)</a>\n\n[08:03
 ] <a href="https://youtu.be/D_CLangkIDE?t=483s">Baryon fraction as predict
 or of feedback (Fig. 2)</a>\n\n[09:24] <a href="https://youtu.be/D_CLangkI
 DE?t=564s">Forecasting constraints (Fig. 3 top panels)</a>\n\n[11:10] <a h
 ref="https://youtu.be/D_CLangkIDE?t=670s">Robustness of constraints to sub
 grid physics (Fig. 3 bottom panels)</a>\n\n[13:37] <a href="https://youtu.
 be/D_CLangkIDE?t=817s">Q&A on a common theme among several of the speakers
 </a>\n\n[14:53] <a href="https://youtu.be/D_CLangkIDE?t=893s">Summary</a>\
 n\n[16:57] <a href="https://youtu.be/D_CLangkIDE?t=1017s">Comments on samp
 le variance in CAMELS</a>\n\n[17:18] <a href="https://youtu.be/D_CLangkIDE
 ?t=1038s">Lingering questions and what would you like to discuss with othe
 r experts?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/48/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Leander Thiele (Princeton University)
DTSTART:20220114T050000Z
DTEND:20220114T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/49
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/49/">Spectral distortions will measure baryon feedback at % level (CAME
 LS)</a>\nby Leander Thiele (Princeton University) as part of Cosmology Tal
 ks\n\nAbstract: TBA\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/49/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Leander Thiele (Princeton University)
DTSTART:20220114T050000Z
DTEND:20220114T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/50
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/50/">Spectral distortions will measure baryon feedback at % level (CAME
 LS)</a>\nby Leander Thiele (Princeton University) as part of Cosmology Tal
 ks\n\n\nAbstract\nLeander tells us about work using CAMELS simulations and
  neural networks to forecast how well future spectral distortion measureme
 nts will be able to constrain baryon feedback. The answer is "very well" a
 s it seems the measurements of PIXIE would give even % level measurements 
 of some feedback mechanisms.\n\nLeander: <a href="https://phy.princeton.ed
 u/people/leander-thiele">https://phy.princeton.edu/people/leander-thiele</
 a><br>\nPaper: <a href="https://arxiv.org/abs/2201.01663">https://arxiv.or
 g/abs/2201.01663</a><br>\nVideo of talk: <a href="https://youtu.be/u2tEG1n
 LwV8">https://youtu.be/u2tEG1nLwV8</a>\n\nCAMELS playlist: <a href="https:
 //youtu.be/6Vgc72a_VpY&amp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT">https
 ://youtu.be/6Vgc72a_VpY&amp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT</a>\n
 \n<hr>\n\n[00:00] <a href="https://youtu.be/u2tEG1nLwV8?t=0s">Shaun's intr
 o</a>\n\n[00:58] <a href="https://youtu.be/u2tEG1nLwV8?t=58s">Leander's ov
 erview comments</a>\n\n[01:47] <a href="https://youtu.be/u2tEG1nLwV8?t=107
 s">Motivation for this work: baryonic physics is an impediment to cosmolog
 y understanding\, e.g.\, huge uncertainty on baryonic feedback mechanisms\
 , primarily due to AGN and SN</a>\n\n[02:22] <a href="https://youtu.be/u2t
 EG1nLwV8?t=142s">Spectral distortions</a>\n\n[03:51] <a href="https://yout
 u.be/u2tEG1nLwV8?t=231s">CAMELS feature of small simulation boxes</a>\n\n[
 04:39] <a href="https://youtu.be/u2tEG1nLwV8?t=279s">The thermal Sunyaev-Z
 el'dovich effect\; parameter dependence</a>\n\n[06:25] <a href="https://yo
 utu.be/u2tEG1nLwV8?t=385s">Forecast constraints</a>\n\n[09:47] <a href="ht
 tps://youtu.be/u2tEG1nLwV8?t=587s">Conclusions and takeaways for the cosmo
 logy community</a>\n\n[10:25] <a href="https://youtu.be/u2tEG1nLwV8?t=625s
 ">To-Do follow-up</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/50/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Pablo Villanueva Domingo (Instituto de Física Corpuscular)
DTSTART:20220117T050000Z
DTEND:20220117T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/51
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/51/">Weighing the Milky Way with AI (CAMELS)</a>\nby Pablo Villanueva D
 omingo (Instituto de Física Corpuscular) as part of Cosmology Talks\n\n\n
 Abstract\nPablo talks about an actual observational result from CAMELS\, t
 he measurement of the masses of the Milky Way and Andromeda. The results a
 re in agreement with other methods we've used to measure the masses of the
 se galaxies.\n\nPablo: <a href="https://pablovd.github.io/">https://pablov
 d.github.io/</a><br>\n\nPaper: <a href="https://arxiv.org/abs/2111.14874">
 https://arxiv.org/abs/2111.14874</a><br>\n\nVideo of talk: <a href="https:
 //youtu.be/yGdcBrYfs8k">https://youtu.be/yGdcBrYfs8k</a>\n\nCAMELS playlis
 t: <a href="https://youtu.be/6Vgc72a_VpY&amp\;list=PLvy7h0l2rJHq03inVPqYnC
 3llKt0IwwLT">https://youtu.be/6Vgc72a_VpY&amp\;list=PLvy7h0l2rJHq03inVPqYn
 C3llKt0IwwLT</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b> \n\n[00:
 00] <a href="https://youtu.be/yGdcBrYfs8k?t=0s">Shaun's intro</a>\n\n[00:4
 6] <a href="https://youtu.be/yGdcBrYfs8k?t=46s">Pablo's overview comments<
 /a>\n\n[01:59] <a href="https://youtu.be/yGdcBrYfs8k?t=119s">Weighing Dark
  Matter Halos</a>\n\n[03:04] <a href="https://youtu.be/yGdcBrYfs8k?t=184s"
 >Is the Milky Way big enough that the baryonic/dark matter ratio is expect
 ed to be the same as on a cosmological or galaxy cluster scale?</a>\n\n[05
 :37] <a href="https://youtu.be/yGdcBrYfs8k?t=337s">Halos as graphs</a>\n\n
 [06:32] <a href="https://youtu.be/yGdcBrYfs8k?t=392s">Why graph neural net
 works? NN type depends on data structure</a>\n\n[07:55] <a href="https://y
 outu.be/yGdcBrYfs8k?t=475s">Inferring halo masses in IllustrisTNG</a>\n\n[
 09:20] <a href="https://youtu.be/yGdcBrYfs8k?t=560s">Cross testing in SIMB
 A</a>\n\n[10:10] <a href="https://youtu.be/yGdcBrYfs8k?t=610s">Application
  to the Milky Way and Andromeda</a>\n\n[10:50] <a href="https://youtu.be/y
 GdcBrYfs8k?t=650s">Inferring the MW and M31 masses (Fig. 1 of paper)</a>\n
 \n[14:10] <a href="https://youtu.be/yGdcBrYfs8k?t=850s">Conclusions</a>\n\
 n[16:07] <a href="https://youtu.be/yGdcBrYfs8k?t=967s">Lingering questions
  and what would you like to discuss with other experts?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/51/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Lucia Perez (Arizona State University)
DTSTART:20220118T050000Z
DTEND:20220118T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/52
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/52/">Fixing CAMELS biggest flaw (small box sizes) with semi-analytic mo
 dels</a>\nby Lucia Perez (Arizona State University) as part of Cosmology T
 alks\n\n\nAbstract\nLucia tells us about her work with CAMELS trying to ov
 ercome the biggest barrier CAMELS faces\, small box size. It might never b
 e possible to run 1000s of large volume hydrodynamical simulations simply 
 because the hierarchy of scales is too big (baryon feedback happens on sma
 ll scales\, overcoming sample variance requires very large boxes). \n\nThe
 refore\, to get many many simulation boxes\, with baryonic effects in them
  one option is semi-analytic models. This is what Lucia has and is doing a
 nd what she discusses in the video...\n\nLucia: <a href="https://isearch.a
 su.edu/profile/2606833">https://isearch.asu.edu/profile/2606833</a>\n\nPap
 er: <a href="https://arxiv.org/abs/2204.02408">Constraining cosmology with
  machine learning and galaxy clustering: the CAMELS-SAM suite [2204.02408]
 </a><br>\n\nTalk video: <a href="https://youtu.be/sx0RCW2p4eU">https://you
 tu.be/sx0RCW2p4eU</a>\n\nCAMELS playlist: <a href="https://youtu.be/6Vgc72
 a_VpY&amp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT">https://youtu.be/6Vgc7
 2a_VpY&amp\;list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT</a>\n\n<hr>\n\n[00:00]
  <a href="https://youtu.be/sx0RCW2p4eU?t=0s">Shaun's intro</a>\n\n[01:15] 
 <a href="https://youtu.be/sx0RCW2p4eU?t=75s">Lucia's overview comments</a>
 \n\n[01:49] <a href="https://youtu.be/sx0RCW2p4eU?t=109s">The massiveness 
 of this work\; why it's still not feasible to do this on a much larger sca
 le</a>\n\n[02:12] <a href="https://youtu.be/sx0RCW2p4eU?t=132s">Video of a
  simulation</a>\n\n[02:37] <a href="https://youtu.be/sx0RCW2p4eU?t=157s">H
 ow this work fits within the rest of the project</a>\n\n[03:53] <a href="h
 ttps://youtu.be/sx0RCW2p4eU?t=233s">Why do this?</a>\n\n[05:34] <a href="h
 ttps://youtu.be/sx0RCW2p4eU?t=334s">Science questions</a>\n\n[08:23] <a hr
 ef="https://youtu.be/sx0RCW2p4eU?t=503s">Getting to smaller scales\; neura
 l networks</a>\n\n[09:14] <a href="https://youtu.be/sx0RCW2p4eU?t=554s">Ta
 ke-away 1: use more than just two-point statistics</a>\n\n[10:38] <a href=
 "https://youtu.be/sx0RCW2p4eU?t=638s">Issue about summary statistics</a>\n
 \n[12:49] <a href="https://youtu.be/sx0RCW2p4eU?t=769s">Discussion on vari
 ous meanings of voids</a>\n\n[13:33] <a href="https://youtu.be/sx0RCW2p4eU
 ?t=813s">How does each statistic perform alone? Or all together?</a>\n\n[1
 5:50] <a href="https://youtu.be/sx0RCW2p4eU?t=950s">Take-away 2: SAM (semi
 -analytic model) galaxy clustering measures cosmology well</a>\n\n[16:49] 
 <a href="https://youtu.be/sx0RCW2p4eU?t=1008s">Take-away 3: with a SAM\, c
 lustering still feels astrophysics</a>\n\n[18:38] <a href="https://youtu.b
 e/sx0RCW2p4eU?t=1118s">Conclusions</a>\n\n[19:37] <a href="https://youtu.b
 e/sx0RCW2p4eU?t=1177s">The big picture implications and questions...</a>\n
 \n[22:28] <a href="https://youtu.be/sx0RCW2p4eU?t=1348s">What would you li
 ke to discuss with other experts?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/52/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Sultan Hassan (Center for Computational Astrophysics\, Flatiron In
 stitute)
DTSTART:20220211T050000Z
DTEND:20220211T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/53
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/53/">Full non-linear density fields without simulations! (HIFlow/CAMELS
 )</a>\nby Sultan Hassan (Center for Computational Astrophysics\, Flatiron 
 Institute) as part of Cosmology Talks\n\n\nAbstract\nSultan tells us about
  his work training neural networks on the neutral hydrogen density fields 
 in the CAMELS simulations. \n\nHe uses a process known as normalising flow
 s to find a mapping between the non-linear\, very non-Gaussian 2D projecte
 d density field and a different Gaussian field. Once this mapping is found
 \, the idea is that one can do full statistics on the non-linear field\, b
 y sampling from the Gaussian one. The bold ambition is to use this process
  to reduce the need for running computationally expensive hydrodynamical s
 imulations - making it more feasible to get precise cosmological constrain
 ts from future surveys.\n\nIt's early days in the project\, but the result
 s are already promising as the model is able to generate density fields th
 at match both the histogram of density values and the power spectrum (as w
 ell as the scatter in both functions) reasonably well.\n\nSultan: <a href=
 "https://sultanier.wixsite.com/website">https://sultanier.wixsite.com/webs
 ite</a>\n\nThe Talk: <a href="https://youtu.be/wDRd7MojD3I">https://youtu.
 be/wDRd7MojD3I</a>\n\nThe Paper: <a href="https://arxiv.org/abs/2110.02983
 ">https://arxiv.org/abs/2110.02983</a>\n\nCAMELS playlist: <a href="https:
 //www.youtube.com/playlist?list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT">https:
 //www.youtube.com/playlist?list=PLvy7h0l2rJHq03inVPqYnC3llKt0IwwLT</a>\n\n
 CAMELS intro: <a href="https://www.youtube.com/watch?v=6Vgc72a_VpY&t=0s">h
 ttps://www.youtube.com/watch?v=6Vgc72a_VpY</a>\n\n<hr>\n\n[00:00] <a href=
 "https://youtu.be/wDRd7MojD3I?t=0s">Shaun's intro</a>\n\n[01:29] <a href="
 https://youtu.be/wDRd7MojD3I?t=89s">Sultans's overview comments</a>\n\n[02
 :26] <a href="https://youtu.be/wDRd7MojD3I?t=146s">At what point in traini
 ng does the model reach a saturation point?</a>\n\n[02:57] <a href="https:
 //youtu.be/wDRd7MojD3I?t=177s">What questions were you trying to answer an
 d why are they important?</a>\n\n[04:10] <a href="https://youtu.be/wDRd7Mo
 jD3I?t=250s">The main idea of this work</a>\n\n[05:02] <a href="https://yo
 utu.be/wDRd7MojD3I?t=302s">Details on how it's done\; addressing the probl
 ems</a>\n\n[07:38] <a href="https://youtu.be/wDRd7MojD3I?t=458s">Details o
 f the results\; Figure 2 from the paper</a>\n\n[10:21] <a href="https://yo
 utu.be/wDRd7MojD3I?t=621s">Power spectra and PDFs over the testing set\; F
 igure 3</a>\n\n[11:05] <a href="https://youtu.be/wDRd7MojD3I?t=665s">Norma
 lizing flow</a>\n\n[12:58] <a href="https://youtu.be/wDRd7MojD3I?t=778s">A
 dditional details on the power spectra slide</a>\n\n[15:31] <a href="https
 ://youtu.be/wDRd7MojD3I?t=931s">Conditioned on Cosmology slide\, Figure 5\
 ; comparison between HIFlow and CAMELS</a>\n\n[16:31] <a href="https://you
 tu.be/wDRd7MojD3I?t=991s">Accuracy over all testing set\, R^2 > 90%\, Figu
 re 7</a>\n\n[18:08] <a href="https://youtu.be/wDRd7MojD3I?t=1088s">Take-aw
 ays for the rest of the cosmology community from this work</a>\n\n[19:37] 
 <a href="https://youtu.be/wDRd7MojD3I?t=1177s">What would you like to disc
 uss with other experts inside or outside of CAMELS?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/53/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Dillon Brout (Harvard Smithsonian Center for Astrophysics)
DTSTART:20220301T050000Z
DTEND:20220301T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/54
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/54/">Pantheon+: Cosmology results & Dust</a>\nby Dillon Brout (Harvard 
 Smithsonian Center for Astrophysics) as part of Cosmology Talks\n\n\nAbstr
 act\nDillon Brout tells us about the recent Pantheon+ supernovae catalogue
  and cosmology results. The cosmology results are excellent\, including a 
 factor of two improvement in the "figure of merit" compared to the previou
 s Pantheon result (essentially a halving of error bars). \n\nHowever\, the
  results aren't going to help anyone looking for a clue for a source of ne
 w physics. The supernovae themselves appear to follow the ΛCDM model very
  closely. If one anchors them to Planck\, or to the SH0ES Cepheids\, eithe
 r way\, one finds tight constraints on beyond ΛCDM parameters like an equ
 ation of state "w" or evolution of an equation of state "w_a".\n\nThere is
  of course the baffling Hubble tension among all of this\, and that is ver
 y clearly visible here. Both the Planck+Pantheon and the SH0ES+Pantheon re
 sults match up with ΛCDM\, but at different values of H0. Any solution to
  the H0 tension that involves beyond ΛCDM evolution in the late-universe 
 appears to be heavily constrained.\n\nThe most interesting part of this ta
 lk (for me) was actually the introduction in the answer to "what needed to
  be done before this analysis could happen" (in fact\, this makes up the l
 argest portion of the talk!). Dillon goes into quite a bit of detail about
  an earlier paper he wrote with Dan Scolnic\, examining the affects of dus
 t on supernovae observations. It appears that three of the most important 
 mysteries in SN analysis were all explainable by the same dust affect and 
 Dillon explains why here.\n\nTalk video: <a href="https://youtu.be/lVN1-Fc
 CBDc">https://youtu.be/lVN1-FcCBDc</a>\n\nDillon:  <a href="https://djbrou
 t.github.io/">https://djbrout.github.io/</a>\n\nPantheon+ cosmology paper:
  <a href="https://arxiv.org/abs/2202.04077">https://arxiv.org/abs/2202.040
 77</a>\n\nEffects of dust on supernovae paper: <a href="https://arxiv.org/
 abs/2004.10206">https://arxiv.org/abs/2004.10206</a>\n\n<hr>\n\n<b>Index t
 o Key Parts of the Talk</b>\n\n[00:00] <a href="https://youtu.be/lVN1-FcCB
 Dc?t=0s">Shaun's intro</a>\n\n[00:57] <a href="https://youtu.be/lVN1-FcCBD
 c?t=57s">Dillon's introductory comments</a>\n\n[01:23] <a href="https://yo
 utu.be/lVN1-FcCBDc?t=83s">Two things for people to remember from this talk
 ?</a>\n\n[05:14] <a href="https://youtu.be/lVN1-FcCBDc?t=314s">The motivat
 ional and the logistical aspects for this work?</a>\n\n[08:41] <a href="ht
 tps://youtu.be/lVN1-FcCBDc?t=521s">Structure formation work based on super
 novae peculiar velocities</a>\n\n[10:17] <a href="https://youtu.be/lVN1-Fc
 CBDc?t=617s">Why wasn't some of this work done in 2018? Why now?</a>\n\n[1
 1:33] <a href="https://youtu.be/lVN1-FcCBDc?t=693s">What questions were un
 solved that you wanted to address? Figure 4 from the 2202.04077 paper</a>\
 n\n[12:03] <a href="https://youtu.be/lVN1-FcCBDc?t=723s">3 Lingering Myste
 ries Central to SNIa Cosmology</a>\n\n[12:45] <a href="https://youtu.be/lV
 N1-FcCBDc?t=765s">1. What drives the observed SN colors and color/luminosi
 ty relations?</a>\n\n[14:14] <a href="https://youtu.be/lVN1-FcCBDc?t=854s"
 >2. What drives the underlying residual scatter of standardized SNe Ia?</a
 >\n\n[15:45] <a href="https://youtu.be/lVN1-FcCBDc?t=945s">3. What's drivi
 ng the evidence for additional standardization?</a>\n\n[17:13] <a href="ht
 tps://youtu.be/lVN1-FcCBDc?t=1033s">Cepheid calibration question relating 
 to the number of SN used in this work</a>\n\n[19:19] <a href="https://yout
 u.be/lVN1-FcCBDc?t=1159s">The SH0ES measurement: host galaxy demographics\
 , calibrator set of hosts\, distance ladder rung</a>\n\n[20:33] <a href="h
 ttps://youtu.be/lVN1-FcCBDc?t=1233s">The "aha moment"</a>\n\n[21:04] <a hr
 ef="https://youtu.be/lVN1-FcCBDc?t=1264s">Dust can be the solution to all 
 three mysteries!</a>\n\n[23:08] <a href="https://youtu.be/lVN1-FcCBDc?t=13
 84s">We can forward the whole sample to learn about SN/Host physics</a>\n\
 n[25:10] <a href="https://youtu.be/lVN1-FcCBDc?t=1510s">The mass step is a
  consequence of differing dust properties for hosts of different masses</a
 >\n\n[25:35] <a href="https://youtu.be/lVN1-FcCBDc?t=1535s">Dust attenuati
 on as a function of host galaxy properties</a>\n\n[27:06] <a href="https:/
 /youtu.be/lVN1-FcCBDc?t=1626s">Dust is the solution!</a>\n\n[27:38] <a hre
 f="https://youtu.be/lVN1-FcCBDc?t=1658s">Predictions from the model</a>\n\
 n[28:13] <a href="https://youtu.be/lVN1-FcCBDc?t=1693s">What are the cosmo
 logical results in this paper? Figures 4\, 6\;  It's important to use the 
 covariance matrix</a>\n\n[29:43] <a href="https://youtu.be/lVN1-FcCBDc?t=1
 783s">Constraints on LCDM\, Figure 8\; Consistency with other probes</a>\n
 \n[32:02] <a href="https://youtu.be/lVN1-FcCBDc?t=1922s">The data set with
  and without SH0ES\; Figure 9</a>\n\n[32:34] <a href="https://youtu.be/lVN
 1-FcCBDc?t=1954s">Measuring w_a\, the evolution of dark energy\; Figure 10
 </a>\n\n[34:50] <a href="https://youtu.be/lVN1-FcCBDc?t=2090s">Including B
 AO\; Figures 11\, 12</a>\n\n[35:31] <a href="https://youtu.be/lVN1-FcCBDc?
 t=2131s">What's next? DES\, LSST\, Machine Learning</a>\n\n[38:36] <a href
 ="https://youtu.be/lVN1-FcCBDc?t=2316s">Comments on the cosmology communit
 y follow-up to this work</a>\n\n[40:49] <a href="https://youtu.be/lVN1-FcC
 BDc?t=2449s">What current cosmology work do you think is particularly unde
 r-appreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/54/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Alexandra Amon & Naomi Robertson (University of Cambridge)
DTSTART:20220324T050000Z
DTEND:20220324T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/55
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/55/">Lensing & clustering are consistent. Small scales are tough but ke
 y to solving S8</a>\nby Alexandra Amon & Naomi Robertson (University of Ca
 mbridge) as part of Cosmology Talks\n\n\nAbstract\nAlex Amon and Naomi Rob
 ertson talk about their recent work analysing all of the Dark Energy Surve
 y (DES)\, the Hyper Suprime Cam survey (HSC)\, and the Kilo Degree Survey 
 (KiDS) and the Baryon Oscillation Spectroscopic Survey (BOSS). In particul
 ar they look to see whether the three lensing surveys (DES\, HSC and KiDS)
  are consistent with the clustering of galaxies in BOSS.\n\nConsistency ch
 ecks are always good just for their own sake\, but this has particular rel
 evance in the context of the S8 tension\, as the lensing surveys provide t
 he strongest evidence of this tension.\n\nThey find that the lensing surve
 ys are (broadly) consistent with each other and are then also consistent w
 ith the clustering in BOSS. When restricting to larger scales\, they also 
 don't find evidence for a different cosmology to Planck. When they include
  smaller scales there is a strong tension between the lensing/clustering p
 robes and the Planck cosmology (i.e. the S8 tension).\n\nTakeaways are tha
 t the local probes of matter appear to be consistent with each other and t
 he S8 tension is best probed by smaller scales. Unfortunately this is also
  where baryonic effects dominate so we need more data constraining them an
 d improved modelling to make further progress.\n\nAlex: <a href="https://a
 monalexandra.com/">https://amonalexandra.com/</a>\n\nNaomi: <a href="https
 ://www.ast.cam.ac.uk/people/naomi.robertson">https://www.ast.cam.ac.uk/peo
 ple/naomi.robertson</a>\n\nTalk video: <a href="https://youtu.be/4gjlNyJ0A
 KY">https://youtu.be/4gjlNyJ0AKY</a>\n\nThe paper: <a href="https://arxiv.
 org/abs/2202.07440">https://arxiv.org/abs/2202.07440</a>\n\n<hr>\n\n<b>Ind
 ex to Key Parts of the Talk</b>\n\n[00:00] <a href="https://youtu.be/4gjlN
 yJ0AKY?t=0s">Shaun's intro</a>\n\n[01:15] <a href="https://youtu.be/4gjlNy
 J0AKY?t=75s">Alex and Naomi's introductory comments</a>\n\n[02:12] <a href
 ="https://youtu.be/4gjlNyJ0AKY?t=132s">Two things for people to remember f
 rom this talk</a>\n\n[03:43] <a href="https://youtu.be/4gjlNyJ0AKY?t=223s"
 >The motivation for this work</a>\n\n[06:24] <a href="https://youtu.be/4gj
 lNyJ0AKY?t=384s">State of the art lensing data</a>\n\n[07:20] <a href="htt
 ps://youtu.be/4gjlNyJ0AKY?t=440s">Challenges with small-scale modeling</a>
 \n\n[10:00] <a href="https://youtu.be/4gjlNyJ0AKY?t=600s">Clustering and L
 ensing 101</a>\n\n[11:41] <a href="https://youtu.be/4gjlNyJ0AKY?t=701s">Da
 ta</a>: Fig. 2 top panel and Fig. 3 from paper\n\n[14:12] <a href="https:/
 /youtu.be/4gjlNyJ0AKY?t=852s">Source sample: Lensing from DES-Y3\, KiDS-10
 00\, & HSC-Y1</a>: Table 1 from paper and Fig. 2 all panels\n\n[15:50] <a 
 href="https://youtu.be/4gjlNyJ0AKY?t=950s">Consistency of Lensing Measurem
 ents</a>: Fig. A1\, Table A1\n\n[18:22] <a href="https://youtu.be/4gjlNyJ0
 AKY?t=1102s">DarkEmulator and HOD</a>\n\n[20:15] <a href="https://youtu.be
 /4gjlNyJ0AKY?t=1215s">Joint Lensing and Clustering Fits</a>\n\n[22:39] <a 
 href="https://youtu.be/4gjlNyJ0AKY?t=1359s">Small Scale Modelling Systemat
 ics</a>: Fig. 4\n\n[30:10] <a href="https://youtu.be/4gjlNyJ0AKY?t=1810s">
 Consistency of Clustering and GGL</a>\n\n[30:50] <a href="https://youtu.be
 /4gjlNyJ0AKY?t=1850s">Consistency of Clustering and GGL: Large Scales</a>:
  Fig. 6 left panel\n\n[32:55] <a href="https://youtu.be/4gjlNyJ0AKY?t=1975
 s">Consistency of Clustering and GGL: All Scales</a>: Fig. 6 right panel\n
 \n[34:18] <a href="https://youtu.be/4gjlNyJ0AKY?t=2058s">Cosmology vs. sma
 ll-scale systematics</a>: Fig. 7\n\n[37:42] <a href="https://youtu.be/4gjl
 NyJ0AKY?t=2262s">Summary</a>\n\n[38:40] <a href="https://youtu.be/4gjlNyJ0
 AKY?t=2320s">What's next?</a>\n\n[41:58] <a href="https://youtu.be/4gjlNyJ
 0AKY?t=2518s">What current cosmology work do you think is particularly und
 er-appreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/55/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Colin Hill\, Adrien La Posta\, and Evan McDonough (Université Par
 is-Saclay\, Columbia University\, University of Winnipeg)
DTSTART:20220410T060000Z
DTEND:20220410T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/56
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/56/">The CMB's mixed messages on early dark energy... &amp\; theory's r
 esponse</a>\nby Colin Hill\, Adrien La Posta\, and Evan McDonough (Univers
 ité Paris-Saclay\, Columbia University\, University of Winnipeg) as part 
 of Cosmology Talks\n\n\nAbstract\nColin Hill\, Adrien La Posta\, and Evan 
 McDonough tell us about the state of play with early dark energy (EDE). Th
 ey cover both observation\, primarily the CMB\; and fundamental physics mo
 dels that might generate EDE phenomenology.\n\nColin gives an intro to EDE
 \, the Hubble tension\, how the CMB is sensitive to EDE\, and EDE models\,
  and then shows how the observational evidence for/against EDE from the CM
 B is... curious. \n\nThe Atacama Cosmology Telescope (ACT) + large scales 
 of Planck/WMAP appear to favour\, or even detect(!?)\, EDE at more than 3 
 sigma\, more or less "solving" the Hubble tension (if you ignore large sca
 le structure\, which you shouldn't!). However\, the full Planck data sees 
 no evidence at all\, even excluding Hubble tension solving values of EDE a
 t about 3 sigma. ACT+Planck also excludes EDE\, because small scale Planck
  is just so constraining that any ACT preference is washed out\; there's j
 ust so much more statistical information in Planck small scales!\n\nAdrien
  then talks about how one can eliminate at least one possible CMB systemat
 ic via using the ratio of power spectra. When doing this there is still a 
 Hubble tension\, and the results are completely consistent with convention
 al CMB analyses (albeit with larger error bars because some info is thrown
  out when taking this ratio). He then covers the same analysis as Colin's 
 ACT analysis\, but this time with the South Pole Telescope (SPT). SPT also
  allows large EDE amplitudes\, but isn't constraining enough to either fav
 our or rule them out.\n\nThe small additional constraining power of SPT do
 es mean though that ACT+SPT+WMAP seems to almost conclusively detect EDE (
 or some equivalent phenomena). It makes me think that *if* Planck didn't e
 xist\, we'd be almost convinced this is *the* answer to where the Hubble t
 ension is coming from. Unfortunately\, Planck does exist and doesn't see a
 ny evidence for this at all - suggesting that this is instead either some 
 systematic in ACT\, or a statistical fluke.\n\nSo\, all bets are off\, but
  this is something to really keep an eye on. ACT will have much more data 
 to say much more about this "within a year" (everything is blind at the mo
 ment though so nobody knows what the data will point at in the end).\n\nFi
 nally\, Evan talks about theory space and how one might tackle this myster
 y of EDE and Hubble tensions and *crucially* large scale structure. He tal
 ks about a "swampland" motivated principle that might allow the mass of da
 rk matter to be influenced by the early dark energy\, meaning that the "S8
  tension" would not be made worse by early dark energy\, but possibly even
  made better. Coupling EDE to dark matter might also help explain why any 
 EDE transition happens to happen close to when the CMB is formed\, maybe..
 . time will tell.\n\nThe talk video: <a href="https://youtu.be/T15WSiHdOFI
 ">https://youtu.be/T15WSiHdOFI</a><br>\n\nAdrien: <a href="https://inspire
 hep.net/authors/1889152">https://inspirehep.net/authors/1889152</a><br>\nA
 drien's paper: <a href="https://arxiv.org/abs/2112.10754">https://arxiv.or
 g/abs/2112.10754</a><br>\n\nColin: <a href="http://user.astro.columbia.edu
 /~jch/">http://user.astro.columbia.edu/~jch/</a><br>\nColin's paper: <a hr
 ef="https://arxiv.org/abs/2109.04451">https://arxiv.org/abs/2109.04451</a>
 <br>\n\nEvan: <a href="https://www.evanmcdonoughphysics.com/">https://www.
 evanmcdonoughphysics.com/</a><br>\nEvan's paper: <a href="https://arxiv.or
 g/abs/2112.09128">https://arxiv.org/abs/2112.09128</a><br>\n\nColin's earl
 ier video on EDE and large scale structure: <a href="https://www.youtube.c
 om/watch?v=5JRHFGuPAV8&t=0s">https://www.youtube.com/watch?v=5JRHFGuPAV8</
 a><br>\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b> \n\n[0:00:00] <a h
 ref="https://youtu.be/T15WSiHdOFIc?t=0s">Shaun's intro</a>\n\n[0:01:05] <a
  href="https://youtu.be/T15WSiHdOFIc?t=65s">Colin's introductory comments<
 /a>\n\n[0:02:13] <a href="https://youtu.be/T15WSiHdOFIc?t=133s">Two things
  for people to remember from this talk</a>\n\n[0:03:24] <a href="https://y
 outu.be/T15WSiHdOFIc?t=204s">The background and context for this work\; th
 e Hubble Situation</a>\n\n[0:06:01] <a href="https://youtu.be/T15WSiHdOFIc
 ?t=361s">ACT Data Release 4</a>: significant improvement upon Planck\, esp
 . on small scales\n\n[0:06:54] <a href="https://youtu.be/T15WSiHdOFIc?t=41
 4s">ACT DR4: foreground-marginalized CMB power spectra</a>\n\n[0:08:16] <a
  href="https://youtu.be/T15WSiHdOFIc?t=496s">ACT DR4 Cosmology</a>\n\n[0:0
 9:46] <a href="https://youtu.be/T15WSiHdOFIc?t=586s">Early Dark Energy</a>
 : motivation - increase CMB-inferred H0\n\n[0:11:28] <a href="https://yout
 u.be/T15WSiHdOFIc?t=688s">Importance of the FIRAS measurement</a>\n\n[0:14
 :09] <a href="https://youtu.be/T15WSiHdOFIc?t=849s">EDE: new component - (
 pseudo)-scalar field</a>\n\n[0:16:09] <a href="https://youtu.be/T15WSiHdOF
 Ic?t=969s">EDE: Parameterization</a>\n\n[0:16:51] <a href="https://youtu.b
 e/T15WSiHdOFIc?t=1011s">EDE model maintains good fit to CMB power spectrum
  data with higher H0</a>\n\n[0:17:29] <a href="https://youtu.be/T15WSiHdOF
 Ic?t=1049s">LSS in EDE Model</a>\n\n[0:18:24] <a href="https://youtu.be/T1
 5WSiHdOFIc?t=1104s">EDE in Planck Primary CMB?</a>\n\n[0:19:21] <a href="h
 ttps://youtu.be/T15WSiHdOFIc?t=1161s">Data set combinations: Planck + BOSS
  (EFT) + DES/HSC/KiDS (S8)</a>\n\n[0:20:32] <a href="https://youtu.be/T15W
 SiHdOFIc?t=1232s">Pre-ACT DR4 Summary</a>\n\n[0:21:22] <a href="https://yo
 utu.be/T15WSiHdOFIc?t=1282s">ACT DR4 EDE Analysis</a>\n\n[0:23:53] <a href
 ="https://youtu.be/T15WSiHdOFIc?t=1433s">ACT DR4 EDE Results</a>: Fig. 1 f
 rom 2109.04451\n\n[0:27:20] <a href="https://youtu.be/T15WSiHdOFIc?t=1640s
 ">Origin of ACT EDE Preference</a>: Figs. 3\, 4 from 2109.04451\n\n[0:29:2
 0] <a href="https://youtu.be/T15WSiHdOFIc?t=1760s">ACT DR4 EDE experimenta
 l and theoretical takeaways</a>\n\n[0:31:53] <a href="https://youtu.be/T15
 WSiHdOFIc?t=1913">Adrien's intro to the 2112.10754 paper (SPT-3G)</a>\n\n[
 0:33:30] <a href="https://youtu.be/T15WSiHdOFIc?t=2010s">Two potential sol
 utions on the CMB side for this tension</a>\n\n[0:34:12] <a href="https://
 youtu.be/T15WSiHdOFIc?t=2052s">Using observables less sensitive to systema
 tics</a>\n\n[0:36:58] <a href="https://youtu.be/T15WSiHdOFIc?t=2218s">SPT-
 3G results vs Planck\, ACT DR4\, and SH0ES</a>\n\n[0:39:08] <a href="https
 ://youtu.be/T15WSiHdOFIc?t=2348s">Summary of EDE results</a>\n\n[0:39:30] 
 <a href="https://youtu.be/T15WSiHdOFIc?t=2370s">New results from SPT-3G pu
 blic data</a>: Figs. 1\, 2 from 2112.10754\n\n[0:41:52] <a href="https://y
 outu.be/T15WSiHdOFIc?t=2512s">Impact of the z_c prior</a>: Fig. 3 from 211
 2.10754\n\n[0:43:55] <a href="https://youtu.be/T15WSiHdOFIc?t=2635s">Combi
 ning with other CMB datasets</a>\n\n[0:45:00] <a href="https://youtu.be/T1
 5WSiHdOFIc?t=2700s">Combining with SH0ES constraint</a>\n\n[0:46:03] <a hr
 ef="https://youtu.be/T15WSiHdOFIc?t=2763s">Adrien's Conclusions</a>\n\n[0:
 49:09] <a href="https://youtu.be/T15WSiHdOFIc?t=2949s">Evan's intro to the
  2112.09128 paper</a>\n\n[0:50:28] <a href="https://youtu.be/T15WSiHdOFIc?
 t=3028s">A recipe for the CMB</a>: CLASS-EDE code on github\n\n[0:51:57] <
 a href="https://youtu.be/T15WSiHdOFIc?t=3117s">Imprint on Large Scale Stru
 cture</a>\n\n[0:53:38] <a href="https://youtu.be/T15WSiHdOFIc?t=3218s">EDE
  and Data</a>\n\n[0:54:36] <a href="https://youtu.be/T15WSiHdOFIc?t=3276s"
 >EDE and Theory</a>\n\n[0:56:28] <a href="https://youtu.be/T15WSiHdOFIc?t=
 3388s">Extending the model: EDE => EDS</a>\n\n[0:58:07] <a href="https://y
 outu.be/T15WSiHdOFIc?t=3487s">Punchline</a>\n\n[1:00:00] <a href="https://
 youtu.be/T15WSiHdOFIc?t=3600s">Into the weeds: What drives the tight const
 raint on c?</a>\n\n[1:02:34] <a href="https://youtu.be/T15WSiHdOFIc?t=3754
 s">The power of ACT</a>: Fig. 10 from 2112.09128\n\n[1:04:01] <a href="htt
 ps://youtu.be/T15WSiHdOFIc?t=3841s">The power of DES-Y3</a>\n\n[1:04:40] <
 a href="https://youtu.be/T15WSiHdOFIc?t=3880s">Evan's wrap-up</a>\n\n[1:05
 :50] <a href="https://youtu.be/T15WSiHdOFIc?t=3950s">Where to next?</a>\n\
 n[1:08:10] <a href="https://youtu.be/T15WSiHdOFIc?t=4090s">What current co
 smology work do you think is particularly under-appreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/56/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Silvia Manconi (RWTH Aachen University)
DTSTART:20220502T060000Z
DTEND:20220502T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/57
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/57/">Planck polarisation beats intensity for dark matter searches at th
 e galactic centre</a>\nby Silvia Manconi (RWTH Aachen University) as part 
 of Cosmology Talks\n\n\nAbstract\nSilvia tells us about her recent use of 
 Planck satellite data to search for dark matter. She doesn't use the CMB t
 hough\, instead she is looking for microwave emission from the galactic ce
 ntre. For her\, the CMB is noise!\n\nIf dark matter decay/annihilation lea
 ds to electron positron emission then those electrons and positrons would 
 emit microwave light through synchrotron radiation as they travel through 
 the magnetic fields at the galactic centre.\n\nShe found that the polarisa
 tion signal is a more sensitive probe of this effect than the intensity. T
 he main theory for why this is is that the observed signal in the polarisa
 tion has more features (coherent hot and cold spots)\, whereas the expecte
 d dark matter signal should be more smooth. Whereas both the intensity mea
 surement and signal should be more smooth. Therefore\, the observed polari
 sation "cold spots" can best constrain the dark matter signal\, especially
  close to the galactic centre\, where the dark matter signal should still 
 be strong.\n\nSilvia: <a href="https://silviamanconi.wordpress.com/">https
 ://silviamanconi.wordpress.com/</a>\n\nPaper: <a href="https://arxiv.org/a
 bs/2204.04232">https://arxiv.org/abs/2204.04232</a>\n\nRecorded Talk: <a h
 ref="https://youtu.be/5lIPLbUyTyw">https://youtu.be/5lIPLbUyTyw</a>\n\n<hr
 >\n\n<b>Index to Key Parts of the Talk</b>\n\n[00:00] <a href="https://you
 tu.be/5lIPLbUyTyw?t=0s">Shaun's intro</a>\n\n[00:42] <a href="https://yout
 u.be/5lIPLbUyTyw?t=42s">Sil‎via's intro comments on this work</a>\n\n[03
 :41] <a href="https://youtu.be/5lIPLbUyTyw?t=221s">Two things for people t
 o remember from this talk</a>\n\n[04:43] <a href="https://youtu.be/5lIPLbU
 yTyw?t=283s">Motivations for this work</a>\n\n[06:55] <a href="https://you
 tu.be/5lIPLbUyTyw?t=415s">Q&A on physics of the DM annihilation and how th
 e synchotron intensity is relevant</a>\n\n[11:28] <a href="https://youtu.b
 e/5lIPLbUyTyw?t=688s">What we need to model</a>\n\n[12:19] <a href="https:
 //youtu.be/5lIPLbUyTyw?t=739s">Q&A involving Fig. S4 from the paper</a>\n\
 n[14:19] <a href="https://youtu.be/5lIPLbUyTyw?t=859s">Q&A involving Fig. 
 S5 top panel</a>\n\n[16:57] <a href="https://youtu.be/5lIPLbUyTyw?t=1017s"
 >Getting into the details: Planck maps processing\, Fig. 1</a>\n\n[21:39] 
 <a href="https://youtu.be/5lIPLbUyTyw?t=1299s">Discussion on the magnetic 
 fields at the galaxy center</a>\n\n[22:59] <a href="https://youtu.be/5lIPL
 bUyTyw?t=1379s">Magnetic field models</a>\n\n[26:16] <a href="https://yout
 u.be/5lIPLbUyTyw?t=1576s">Dark matter signal\, Fig. S3</a>\n\n[27:27] <a h
 ref="https://youtu.be/5lIPLbUyTyw?t=1647s">Dark matter profile\, Fig. S7</
 a>\n\n[29:44] <a href="https://youtu.be/5lIPLbUyTyw?t=1784s">Summary plot\
 , Fig. 3 right panel</a>\n\n[34:03] <a href="https://youtu.be/5lIPLbUyTyw?
 t=2043s">Why is polarisation the most constraining?</a>\n\n[37:32] <a href
 ="https://youtu.be/5lIPLbUyTyw?t=2252s">Magnetic field configuration uncer
 tainty\, Fig. 3 left panel and Fig. 8 left panel</a>\n\n[38:24] <a href="h
 ttps://youtu.be/5lIPLbUyTyw?t=2304s">What comes next?</a>\n\n[39:28] <a hr
 ef="https://youtu.be/5lIPLbUyTyw?t=2368s">Fig. S5 top panel</a>\n\n[42:24]
  <a href="https://youtu.be/5lIPLbUyTyw?t=2544s">Perspectives for follow-up
  work</a>\n\n[44:10] <a href="https://youtu.be/5lIPLbUyTyw?t=2650s">What c
 urrent cosmology work do you think is particularly under-appreciated?</a>\
 n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/57/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Andrej Dvornik and Constance Mahony (Ruhr University Bochum)
DTSTART:20220617T060000Z
DTEND:20220617T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/58
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/58/">The Kilo-Degree Survey goes non-linear. With cosmology constraints
 !</a>\nby Andrej Dvornik and Constance Mahony (Ruhr University Bochum) as 
 part of Cosmology Talks\n\n\nAbstract\nAndrej Dvornik and Constance Mahony
  tell us about the Kilo-Degree Survey (KiDS) and their progress at probing
  the non-linear scales with data from the survey.\n\nConstance talks about
  her recent paper showing that non-linear halo bias is absolutely necessar
 y if you want to avoid errors larger than 5σ on the small\, non-linear sc
 ales.\n\nAndrej takes this and does the analysis on KiDS data to obtain co
 smological constraints.\n\nConstance: <a href="https://inspirehep.net/auth
 ors/1851831">INSPIRE author page</a>\n\nConstance's paper: <a href="https:
 //arxiv.org/abs/2202.01790">arxiv.org/abs/2202.01790</a>\n\nAndrej: <a hre
 f="http://andrej.dvrnk.si/page/">Personal Website</a>\n\nAndrej's paper: <
 a href="https://arxiv.org/abs/2210.03110">arxiv.org/abs/2210.03110</a>\n\n
 <hr>\n\nIndex to Key Parts of the Talk:<br>\n[00:00] <a href="https://yout
 u.be/Lhfsk24GYyU?t=0s">Shaun's intro</a>\n\n[00:56] <a href="https://youtu
 .be/Lhfsk24GYyU?t=56s">Constance's overview comments on this work</a>\n\n[
 01:45] <a href="https://youtu.be/Lhfsk24GYyU?t=105">Andrej's overview comm
 ents</a>\n\n[03:12] <a href="https://youtu.be/Lhfsk24GYyU?t=192s">Two thin
 gs for people to remember from this talk\; start of Constance's portion of
  talk</a>\n\n[03:57] <a href="https://youtu.be/Lhfsk24GYyU?t=237s">Backgro
 und and context\; details on the Halo Model\; revisiting the assumption of
  linear halo bias</a>\n\n[06:05] <a href="https://youtu.be/Lhfsk24GYyU?t=3
 65">Corrections going beyond linear-halo bias</a>\n\n[06:47] <a href="http
 s://youtu.be/Lhfsk24GYyU?t=407">Halo model contributions slide\; eqns (1) 
 in 2202.01790</a>\n\n[07:37] <a href="https://youtu.be/Lhfsk24GYyU?t=457">
 Halo model power spectra\; eqns (2)</a>\n\n[09:07] <a href="https://youtu.
 be/Lhfsk24GYyU?t=547">Beyond-linear halo bias\; eqn (14)</a>\n\n[11:03] <a
  href="https://youtu.be/Lhfsk24GYyU?t=663">Dark Emulator\; Appendix A of p
 aper</a>\n\n[11:45] <a href="https://youtu.be/Lhfsk24GYyU?t=705">Quick int
 ro about KiDS</a>\n\n[12:38] <a href="https://youtu.be/Lhfsk24GYyU?t=758">
 Cosmology Dependence σ8\; Fig. 1 of paper</a>\n\n[13:58] <a href="https:/
 /youtu.be/Lhfsk24GYyU?t=838">Q&A on meaning of excess surface density</a>\
 n\n[15:24] <a href="https://youtu.be/Lhfsk24GYyU?t=924">Cosmology Dependen
 ce Ωm</a>\n\n[16:02] <a href="https://youtu.be/Lhfsk24GYyU?t=962">KiDS ga
 laxy-galaxy lensing and clustering\; Fig. 3\, main takeaway plot from the 
 paper</a>\n\n[17:52] <a href="https://youtu.be/Lhfsk24GYyU?t=1072">Stellar
  Mass Function\; Fig. 4</a>\n\n[18:48] <a href="https://youtu.be/Lhfsk24GY
 yU?t=1128">HSC Y1 results with DarkEmulator+HOD (halo occupation distribut
 ion)</a>\n\n[19:36] <a href="https://youtu.be/Lhfsk24GYyU?t=1176">Comparis
 on to DarkEmulator+HOD\; Fig. 5</a>\n\n[25:25] <a href="https://youtu.be/L
 hfsk24GYyU?t=1225">DarkEmulator+HOD Mock Analysis\; Fig. 6</a>\n\n[21:03] 
 <a href="https://youtu.be/Lhfsk24GYyU?t=1263">DarkEmulator+HOD Results</a>
 \n\n[21:35] <a href="https://youtu.be/Lhfsk24GYyU?t=1295">Constance's Summ
 ary: Beyond-linear halo bias summary</a>\n\n[23:11] <a href="https://youtu
 .be/Lhfsk24GYyU?t=1391">Andrej's portion of talk: Two things for people to
  remember</a>\n\n[24:08] <a href="https://youtu.be/Lhfsk24GYyU?t=1448">2x2
  point cosmology with SMF (stellar mass function)</a>\n\n[25:24] <a href="
 https://youtu.be/Lhfsk24GYyU?t=1524">Halo occupation modelling</a>\n\n[27:
 47] <a href="https://youtu.be/Lhfsk24GYyU?t=1667">Describing the galaxy bi
 as</a>\n\n[29:29] <a href="https://youtu.be/Lhfsk24GYyU?t=1769">Further as
 sumptions in the model</a>\n\n[31:34] <a href="https://youtu.be/Lhfsk24GYy
 U?t=1894">Parameters</a>\n\n[33:09] <a href="https://youtu.be/Lhfsk24GYyU?
 t=1989">Graphic: How stellar mass correlates with the halo mass</a>\n\n[35
 :08] <a href="https://youtu.be/Lhfsk24GYyU?t=2108">Graphic: Stellar mass f
 unction</a>\n\n[35:55] <a href="https://youtu.be/Lhfsk24GYyU?t=2155">KiDS-
 1000/DR4\; The data</a>\n\n[38:21] <a href="https://youtu.be/Lhfsk24GYyU?t
 =2301">Measurements</a>\n\n[40:37] <a href="https://youtu.be/Lhfsk24GYyU?t
 =2437">Results</a>\n\n[42:38] <a href="https://youtu.be/Lhfsk24GYyU?t=2558
 ">Comparison with other literature</a>\n\n[47:07] <a href="https://youtu.b
 e/Lhfsk24GYyU?t=2827">Andrej's Summary</a>\n\n[47:39] <a href="https://you
 tu.be/Lhfsk24GYyU?t=2859">Some Q&As on where to next</a>\n\n[53:26] <a hre
 f="https://youtu.be/Lhfsk24GYyU?t=3206s">What current cosmology work do yo
 u think is particularly under-appreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/58/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Jiamin Hou\, Zachary Slepian and Robert Cahn (U of Florida\, LBNL)
DTSTART:20220819T060000Z
DTEND:20220819T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/59
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/59/">7σ (!?) detection of parity violation in the large scale structur
 e</a>\nby Jiamin Hou\, Zachary Slepian and Robert Cahn (U of Florida\, LBN
 L) as part of Cosmology Talks\n\n\nAbstract\nJiamin Hou\, Zachary (Zack) S
 lepian and Robert (Bob) Cahn talk about their very interesting\, recent pa
 per looking for parity violation in the large scale structure. Cutting to 
 the chase\, they find evidence for it at ~7σ. They also do various system
 atic tests and none reduce the significance below 4σ.\n\nTantalisingly\, 
 parity violation in the LSS could be related to birefringence in the cosmi
 c microwave background\, with many models that would produce one\, also pr
 oducing the other. Avid channel viewers will remember a talk from two year
 s ago with evidence for exactly that. \n\nAre we seeing the beginnings of 
 evidence for genuine parity violation on cosmological scales\, or are the 
 two hints caused by independent errors?\n\nThis is definitely a space to w
 atch...\n\nJiamin: <a href="https://astro.ufl.edu/directory/jiamin-hou/">h
 ttps://astro.ufl.edu/directory/jiamin-hou/</a><br>\nZack: <a href="https:/
 /astro.ufl.edu/directory/zachary-slepian/">https://astro.ufl.edu/directory
 /zachary-slepian/</a><br>\nBob: <a href="http://phyweb.lbl.gov/~rncahn/www
 /cahn.html">http://phyweb.lbl.gov/~rncahn/www/cahn.html</a><br>\n\n<a href
 ="https://youtu.be/4GPx0R4V4-I">Talk recording</a><br>\n\nThe paper (resul
 ts): <a href="https://arxiv.org/abs/2206.03625">https://arxiv.org/abs/2206
 .03625</a><br>\nThe paper (earlier methods): <a href="https://arxiv.org/ab
 s/2110.12004">https://arxiv.org/abs/2110.12004</a><br>\n\n<hr>\n\n<b>Index
  to Key Parts of the Talk</b>\n\n[00:00] <a href="https://youtu.be/4GPx0R4
 V4-I?t=0s">Shaun's intro</a>\n\n[00:58] <a href="https://youtu.be/4GPx0R4V
 4-I?t=58s">Intro comments on this work (Bob)</a>\n\n[01:55] <a href="https
 ://youtu.be/4GPx0R4V4-I?t=115s">Two things for people to remember from thi
 s talk (Zack)</a>\n\n[03:45] <a href="https://youtu.be/4GPx0R4V4-I?t=225s"
 >The background on parity violation and its applications to cosmology</a>\
 n\n[10:31] <a href="https://youtu.be/4GPx0R4V4-I?t=631s">Cosmological pari
 ty violation must be from epoch of inflation</a>\n\n[11:20] <a href="https
 ://youtu.be/4GPx0R4V4-I?t=680s">Parity violation does not conflict with ho
 mogeneity or isotropy</a>\n\n[12:11] <a href="https://youtu.be/4GPx0R4V4-I
 ?t=731s">Parity violation with the 4PCF of LSS (Fig. 1 from 2206.03625)</a
 >\n\n[12:56] <a href="https://youtu.be/4GPx0R4V4-I?t=776s">NPCFs in the Is
 otropic Basis</a>\n\n[16:25] <a href="https://youtu.be/4GPx0R4V4-I?t=985s"
 >Great Find: Yutsis\, Levinson\, & Vanagas (1962)</a>\n\n[17:63] <a href="
 https://youtu.be/4GPx0R4V4-I?t=1073s">Why is this working happening now an
 d not earlier? (Zack)</a>\n\n[22:26] <a href="https://youtu.be/4GPx0R4V4-I
 ?t=1346s">N-Point Functions on the GPU with CADENZA</a>\n\n[23:47] <a href
 ="https://youtu.be/4GPx0R4V4-I?t=1427s">Data analysis: 2 samples used - BO
 SS DR12 LOWZ and CMASS (LRGs)  (Jiamin)</a>\n\n[24:39] <a href="https://yo
 utu.be/4GPx0R4V4-I?t=1479s">Two challenges</a>\n\n[25:14] <a href="https:/
 /youtu.be/4GPx0R4V4-I?t=1514s">3 Ways We Estimate the Covariance Matrix</a
 >\n\n[28:16] <a href="https://youtu.be/4GPx0R4V4-I?t=1696s">Testing the De
 tection Significance's Robustness</a>\n\n[29:42] <a href="https://youtu.be
 /4GPx0R4V4-I?t=1782s">Test of Analytic Covariance Matrix (Fig. 7 from 2206
 .03625)</a>\n\n[34:38] <a href="https://youtu.be/4GPx0R4V4-I?t=2078s">Q&A:
  is it possible this is non-isotropy instead of parity violation?</a>\n\n[
 37:46] <a href="https://youtu.be/4GPx0R4V4-I?t=2266s">Impact of Systematic
 s on Parity-Odd Modes</a>\n\n[41:18] <a href="https://youtu.be/4GPx0R4V4-I
 ?t=2478s">A non-exhaustive list of potential questions</a>\n\n[46:26] <a h
 ref="https://youtu.be/4GPx0R4V4-I?t=2786s">What are the next steps?</a>\n\
 n[55:32] <a href="https://youtu.be/4GPx0R4V4-I?t=3322s">What current work 
 in cosmology is particularly under-appreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/59/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Johannes Røsok Eskilt\, Patricia Diego-Palazuelo (U of Oslo\, U o
 f Cantabria)
DTSTART:20220920T060000Z
DTEND:20220920T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/60
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/60/">2.4σ → 3.6σ\, CMB Birefringence in 2022</a>\nby Johannes Røso
 k Eskilt\, Patricia Diego-Palazuelo (U of Oslo\, U of Cantabria) as part o
 f Cosmology Talks\n\n\nAbstract\nJohannes Røsok Eskilt and Patricia Diego
 -Palazuelo update us on the state of measurements of birefringence in the 
 cosmic microwave background in 2022. The current most popular video on the
  channel was about a tentative hint of CMB birefringence back in 2020 and 
 much can change in two years.\n\nThe tentative hint is very much still pre
 sent. Johannes and Patricia are both members of Planck itself and have spe
 nt the last few years checking for systematics\, taking the effects of EB 
 correlations in the dust into account\, adding WMAP data\, adding addition
 al frequency maps from Planck\, and checking for a frequency dependence of
  the signal.\n\nSo far there are no smoking guns saying "oops\, this is wh
 at is causing the signal"\, so new physics is very much still on the table
 .\n\nWith the additional Planck maps and WMAP data included\, as well as t
 ighter modelling of the dust\, the statistical significance has drifted up
  from 2.4σ two years ago to 3.6σ today\, which is exactly what one would
  expect if this was a real signal.\n\nThe crucial test of this would be a 
 ground based experiment like ACT\, SPT or BICEP calibrating their misalign
 ment angle directly with greater accuracy than Planck/WMAP can indirectly 
 and looking directly for an EB signal in the CMB... if they still see some
 thing that would be extremely interesting!\n\nRecorded talk: <a href="http
 s://youtu.be/k9YZiWoFwzg">https://youtu.be/k9YZiWoFwzg</a>\n\nJohannes: <a
  href="https://www.mn.uio.no/astro/english/people/aca/johanres/">https://w
 ww.mn.uio.no/astro/english/people/aca/johanres/</a><br>\nPatricia: <a href
 ="https://inspirehep.net/authors/1954027">https://inspirehep.net/authors/1
 954027</a>\n\nPaper 1: <a href="https://arxiv.org/abs/2201.07682">https://
 arxiv.org/abs/2201.07682</a><br>\nPaper 2: <a href="https://arxiv.org/abs/
 2205.13962">https://arxiv.org/abs/2205.13962</a>\n\n<hr>\n\n<b>Index to Ke
 y Parts of the Talk</b>\n\n[00:00] <a href="https://youtu.be/k9YZiWoFwzg?t
 =0s">Shaun's intro</a>\n\n[00:49] <a href="https://youtu.be/k9YZiWoFwzg?t=
 49s">Summary comments on this work</a>\n\n[02:43] <a href="https://youtu.b
 e/k9YZiWoFwzg?t=163s">Two things for people to remember from this talk</a>
 \n\n[03:40] <a href="https://youtu.be/k9YZiWoFwzg?t=220s">The potential fo
 r ground-based telescopes in this work</a>\n\n[05:18] <a href="https://you
 tu.be/k9YZiWoFwzg?t=318s">What is the significance of this work?</a>\n\n[0
 5:52] <a href="https://youtu.be/k9YZiWoFwzg?t=352s">Getting into the detai
 ls</a>\n\n[14:00] <a href="https://youtu.be/k9YZiWoFwzg?t=840s">Consistent
  results across 4 independent pipelines</a>\n\n[14:31] <a href="https://yo
 utu.be/k9YZiWoFwzg?t=871s">Results</a>\n\n[15:41] <a href="https://youtu.b
 e/k9YZiWoFwzg?t=941s">Need to correct for dust EB to obtain unbiased measu
 rement of birefringence</a>\n\n[18:36] <a href="https://youtu.be/k9YZiWoFw
 zg?t=1116s">Two independent ways of mitigating the effect of dust EB</a>\n
 \n[19:24] <a href="https://youtu.be/k9YZiWoFwzg?t=1164s">Where does dust E
 B come from?</a>\n\n[21:26] <a href="https://youtu.be/k9YZiWoFwzg?t=1286s"
 >Commander sky model as foreground model</a>\n\n[22:58] <a href="https://y
 outu.be/k9YZiWoFwzg?t=1378s">What did we do next?</a>\n\n[23:36] <a href="
 https://youtu.be/k9YZiWoFwzg?t=1416s">Q&A if there's a dust EB amplitude p
 rediction</a>\n\n[25:25] <a href="https://youtu.be/k9YZiWoFwzg?t=1525s">Wh
 at happens if we include all Planck maps?</a>\n\n[26:24] <a href="https://
 youtu.be/k9YZiWoFwzg?t=1584s">What is the origin of the signal? (if real)<
 /a>\n\n[27:12] <a href="https://youtu.be/k9YZiWoFwzg?t=1632s">Signal is co
 nsistent with being frequency-independent</a>\n\n[28:28] <a href="https://
 youtu.be/k9YZiWoFwzg?t=1708s">Adding LFI increased the significance</a>\n\
 n[29:28] <a href="https://youtu.be/k9YZiWoFwzg?t=1768s">Adding WMAP increa
 ses the significance</a>\n\n[31:21] <a href="https://youtu.be/k9YZiWoFwzg?
 t=1881s">The fitting\; Figs. 4\,5 in 2205.13962</a>\n\n[32:24] <a href="ht
 tps://youtu.be/k9YZiWoFwzg?t=1944s">Miscalibration angles\; Fig. 3 in 2205
 .13962</a>\n\n[33:41] <a href="https://youtu.be/k9YZiWoFwzg?t=2021s">Summa
 ry of Planck plus WMAP analysis</a>\n\n[34:00] <a href="https://youtu.be/k
 9YZiWoFwzg?t=2040s">Quantifying systematics using NPIPE end-to-end simulat
 ions</a>\n\n[39:26] <a href="https://youtu.be/k9YZiWoFwzg?t=2366s">FAQ</a>
 \n\n[42:22] <a href="https://youtu.be/k9YZiWoFwzg?t=2542s">Conclusions</a>
 \n\n[48:28] <a href="https://youtu.be/k9YZiWoFwzg?t=2908s">What current co
 smology work is particularly interesting or underappreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/60/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Richard Easther (University of Auckland)
DTSTART:20221026T050000Z
DTEND:20221026T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/61
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/61/">The earliest gravitational structures (just after inflation)</a>\n
 by Richard Easther (University of Auckland) as part of Cosmology Talks\n\n
 \nAbstract\nRichard Easther talks about the era immediately after inflatio
 n. If reheating is delayed then the small perturbations in the density of 
 the universe grow\, just as they do during matter domination in the late u
 niverse. The growth of non-linear structures during this "early dark age" 
 has not been explored in depth until recently and Richard gives an overvie
 w of recent work on the topic.\n\nIt turns out that the evolution of struc
 tures during this era is described mathematically using essentially the sa
 me equations as a fuzzy dark matter/ultralight dark matter epoch now. This
  means all the tools developed for fuzzy dark matter are re-usable in this
  earlier epoch. In fact\, on large enough scales\, even a Newtonian N-body
  code suffices.\n\nThere are interesting things to explore in models that 
 have existed since inflation became a topic\, one doesn't need to cook up 
 exotic scenarios\, all that is needed is for reheating to not happen insta
 ntly. In fact\, in units of efoldings\, this early matter domination\, gro
 wth of structures period of time could even last much longer than the late
  universe matter dominated phase\, meaning structures have much longer to 
 grow\, and viralise\, and accrete more matter - making them a fascinating 
 thing to study.\n\nTalk recording: <a href="https://youtu.be/kPiCZpi1Px4">
 https://youtu.be/kPiCZpi1Px4</a>\n\nRichard: <a href="https://excursionset
 .com/about-me">https://excursionset.com/about-me</a>\n\nPaper 1: <a href="
 https://arxiv.org/abs/1909.11678">https://arxiv.org/abs/1909.11678</a><br>
 \nPaper 2: <a href="https://arxiv.org/abs/1911.01661">https://arxiv.org/ab
 s/1911.01661</a><br>\nPaper 3: <a href="https://arxiv.org/abs/2011.13333">
 https://arxiv.org/abs/2011.13333</a><br> \nPaper 4: <a href="https://arxiv
 .org/abs/2110.15109">https://arxiv.org/abs/2110.15109</a><br>\n\n<hr>\n<b>
 Index to Key Parts of the Talk</b>\n\n[00:00] <a href="https://youtu.be/kP
 iCZpi1Px4?t=0s">Shaun's intro</a>\n\n[00:43] <a href="https://youtu.be/kPi
 CZpi1Px4?t=43s">Richard's summary comments on this work</a>\n\n[03:28] <a 
 href="https://youtu.be/kPiCZpi1Px4?t=208s">Two things for people to rememb
 er from this talk</a>\n\n[06:50] <a href="https://youtu.be/kPiCZpi1Px4?t=4
 10s">Richard's motivation for studying this early matter-dominated field</
 a>\n\n[15:22] <a href="https://youtu.be/kPiCZpi1Px4?t=922s">Comments on pa
 rallels to ultralight dark matter work</a>\n\n[18:32] <a href="https://you
 tu.be/kPiCZpi1Px4?t=1112s">Getting into the details: Post-Inflationary Uni
 verse</a>\n\n[19:39] <a href="https://youtu.be/kPiCZpi1Px4?t=1179s">Inflat
 ion Condensate</a>\n\n[24:04] <a href="https://youtu.be/kPiCZpi1Px4?t=1444
 s">Paper 1\, 1909.11678</a>\n\n[30:06] <a href="https://youtu.be/kPiCZpi1P
 x4?t=1806s">Self-gravitating quantum matter</a>\n\n[33:24] <a href="https:
 //youtu.be/kPiCZpi1Px4?t=2004s">Schrodinger-Poisson Equation</a>\n\n[35:24
 ] <a href="https://youtu.be/kPiCZpi1Px4?t=2124s">Proof of Concept</a>\n\n[
 38:57] <a href="https://youtu.be/kPiCZpi1Px4?t=2337s">Figure 2 from 1909.1
 1678</a>\n\n[39:18] <a href="https://youtu.be/kPiCZpi1Px4?t=2358s">Structu
 re formation...</a>\n\n[40:27] <a href="https://youtu.be/kPiCZpi1Px4?t=242
 7s">Cosmic web (simulation)</a>\n\n[41:01] <a href="https://youtu.be/kPiCZ
 pi1Px4?t=2461s">A theorist's playground</a>\n\n[43:05] <a href="https://yo
 utu.be/kPiCZpi1Px4?t=2585s">Developing/adapting new numerical tools\; 1911
 .01661\, 2011.1333</a>\n\n[50:44] <a href="https://youtu.be/kPiCZpi1Px4?t=
 3044s">Simulation\, 2011.13333</a>\n\n[51:34] <a href="https://youtu.be/kP
 iCZpi1Px4?t=3094s">Biggest smallest simulation</a>\n\n[52:09] <a href="htt
 ps://youtu.be/kPiCZpi1Px4?t=3129s">cf Press-Schecter\; Zoom-in simulations
 \, 2110.15109</a>\n\n[56:19] <a href="https://youtu.be/kPiCZpi1Px4?t=3379s
 ">Future Work...</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/61/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Keir Rogers (University of Toronto)
DTSTART:20230122T050000Z
DTEND:20230122T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/62
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/62/">Ultralight dark matter and the S8 tension</a>\nby Keir Rogers (Uni
 versity of Toronto) as part of Cosmology Talks\n\n\nAbstract\nKeir tells u
 s about constraints on the fraction of dark matter that could be "ultralig
 ht" at various masses. \n\nIt seems probable now that one single mass of u
 ltralight dark matter (ULDM) can't be responsible for all the dark matter\
 , but this doesn't mean it can't be a sub-component of the dark matter. Th
 e structure suppressing properties of ULDM could also have implications fo
 r the S8 tension\, i.e. maybe a small sub-component of ULDM is what is cau
 sing the low S8 in local measurements?\n\nThe observational data Keir cons
 iders are the Planck CMB data and BOSS clustering data.\n\n<a href="https:
 //youtu.be/xATqST41dGM">Recorded talk</a>\n\nKeir: <a href="https://keirkw
 ame.github.io/">keirkwame.github.io</a>\n\nPaper: <a href="https://arxiv.o
 rg/abs/2301.08361">2301.08361</a>\n<hr>\n\n<b>Index to Key Parts of the Ta
 lk</b>\n\n[00:00] <a href="https://youtu.be/xATqST41dGM?t=0s">Shaun's intr
 o</a>\n\n[00:53] <a href="https://youtu.be/xATqST41dGM?t=53s">Kier's brief
  opening comments about his paper</a>\n\n[02:38] <a href="https://youtu.be
 /xATqST41dGM?t=158">Two things for people to remember from this talk</a>\n
 \n[04:16] <a href="https://youtu.be/xATqST41dGM?t=256">What is the motivat
 ion for this research?</a>\n\n[05:00] <a href="https://youtu.be/xATqST41dG
 M?t=300">Find dark matter by only known interaction - gravity</a> (with ga
 laxies and intergalactic gas as tracers)\n\n[05:45] <a href="https://youtu
 .be/xATqST41dGM?t=345">Beyond the WIMP: dark matter model space</a>\n\n[08
 :12] <a href="https://youtu.be/xATqST41dGM?t=492">ULAs are invoked to reso
 lve so-called CDM "small-scale crisis"</a>\n\n[09:02] <a href="https://you
 tu.be/xATqST41dGM?t=542">"Canonical" 10^-22 to 10^-21 eV ULA DM is ruled o
 ut</a>\n\n[09:37] <a href="https://youtu.be/xATqST41dGM?t=577">Stringy axi
 ons & the string axiverse</a>\n\n[13:08] <a href="https://youtu.be/xATqST4
 1dGM?t=788">Multi-probe approach to detect ULAs</a>\n\n[15:25] <a href="ht
 tps://youtu.be/xATqST41dGM?t=925">Axions are dark matter and dark energy c
 andidates</a>\n\n[17:13] <a href="https://youtu.be/xATqST41dGM?t=1033">Sim
 ulation animations with and without axions</a>\n\n[19:08] <a href="https:/
 /youtu.be/xATqST41dGM?t=1148">S8 tension</a>\n\n[22:46] <a href="https://y
 outu.be/xATqST41dGM?t=1366">ULA DM causes scale-dependent suppression in m
 atter clustering</a>\n\n[26:45] <a href="https://youtu.be/xATqST41dGM?t=14
 85">Axions lower S8</a>\n\n[27:50] <a href="https://youtu.be/xATqST41dGM?t
 =1670">Lightest axions constrained by CMB</a>\n\n[30:01] <a href="https://
 youtu.be/xATqST41dGM?t=1801">Planck 2018 reionisation bump breaks axion de
 generacies</a>\n\n[32:16] <a href="https://youtu.be/xATqST41dGM?t=1936">DM
 -like axions lower S8\; DE-like axions lower h</a>\n\n[33:54] <a href="htt
 ps://youtu.be/xATqST41dGM?t=2034">High-resolution CMB marginally weakens a
 xion constraint</a>\n\n[40:01] <a href="https://youtu.be/xATqST41dGM?t=240
 1">Model galaxy clustering into mildly non-linear regime with EFT of LSS</
 a>\n\n[42:34] <a href="https://youtu.be/xATqST41dGM?t=2454">Galaxy cluster
 ing traces DM clustering - revealing signature of ULAs</a>\n\n[44:05] <a h
 ref="https://youtu.be/xATqST41dGM?t=2645">BOSS DR12 galaxy clustering rule
 s out new parts of axion parameter space</a>\n\n[45:50] <a href="https://y
 outu.be/xATqST41dGM?t=2750">Axions improve consistency between Planck and 
 BOSS</a>\n\n[47:49] <a href="https://youtu.be/xATqST41dGM?t=2869">BOSS has
  mild preference at m_a = 10^-26 eV - excluded by Planck</a>\n\n[53:17] <a
  href="https://youtu.be/xATqST41dGM?t=3197">Strongest axion bounds come fr
 om combining CMB & LSS</a>\n\n[54:29] <a href="https://youtu.be/xATqST41dG
 M?t=3269">Window of DM-like axions with lower S8</a>\n\n[54:56] <a href="h
 ttps://youtu.be/xATqST41dGM?t=3296">Could axions resolve the S8 tension</a
 >\n\n[55:55] <a href="https://youtu.be/xATqST41dGM?t=3355">Multi-probe app
 roach to detect ULAs</a>\n\n[1:00:15] <a href="https://youtu.be/xATqST41dG
 M?t=3615">Where to next?</a>\n\n[1:03:35] <a href="https://youtu.be/xATqST
 41dGM?t=3815">What current work in cosmology is particularly underapprecia
 ted by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/62/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Johannes Lange (Leinweber Center for Theoretical Physics\, Univers
 ity of Michigan)
DTSTART:20230205T050000Z
DTEND:20230205T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/63
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/63/">S8 constraints from (very) non-linear scales in combined DES\, KiD
 S & BOSS</a>\nby Johannes Lange (Leinweber Center for Theoretical Physics\
 , University of Michigan) as part of Cosmology Talks\n\n\nAbstract\nJohann
 es Lange tells us about his recent work with collaborators constraining co
 smological parameters\, in particular S8\, using the non-linear scales in 
 the Dark Energy Survey (DES)\, the Kilo Degree Survey (KiDS) and the Baryo
 n Oscillation Spectroscopic Survey (BOSS).\n\nThey generate predictions fo
 r the non-linear scales via the Aemulus suite of simulations\, which ran w
 ith a variety of cosmological parameters. To connect the simulations' halo
 s with galaxy observations they use a halo occupation distribution (HOD) m
 odel to generate a large number of sets of mock galaxies. The halo model p
 arameters are then marginalised over when comparing the mocks to observati
 ons\, ultimately giving the final cosmology constraints.\n\nAs with more o
 r less all other large scale structure probes nowadays they find a mild te
 nsion between their constraints and predictions for S8 coming from CMB obs
 ervations and the LCDM model.\n\nTalk recording: <a href="https://youtu.be
 /XxCIpFMP_lw">youtu.be/XxCIpFMP_lw</a>\n\nJohannes' web site: <a href="htt
 ps://johannesulf.github.io/">johannesulf.github.io/</a>\n\nPaper: <a href=
 "https://arxiv.org/abs/2301.08692">arxiv.org/abs/2301.08692</a>\n\nhalotoo
 ls code: <a href="https://github.com/astropy/halotools">github.com/astropy
 /halotools</a>\n\ndsigma code: <a href="https://github.com/johannesulf/dsi
 gma">github.com/johannesulf/dsigma</a>\n\n<hr>\n\n<b>Index to Key Parts of
  the Talk</b>\n\n[00:00] <a href="https://youtu.be/XxCIpFMP_lw?t=0s">Shaun
 's intro</a>\n\n[01:16] <a href="https://youtu.be/XxCIpFMP_lw?t=76">Johann
 es' brief opening comments about the paper</a>\n\n[03:45] <a href="https:/
 /youtu.be/XxCIpFMP_lw?t=225">Two things for people to remember from this t
 alk</a>\n\n[05:43] <a href="https://youtu.be/XxCIpFMP_lw?t=343">What are t
 he motivations for this work?</a>\n\n[08:26] <a href="https://youtu.be/XxC
 IpFMP_lw?t=506">Several advancements in recent years made this work possib
 le</a>\n\n[09:12] <a href="https://youtu.be/XxCIpFMP_lw?t=552">Halotools\,
  by Andrew Hearin</a>\n\n[09:26] <a href="https://youtu.be/XxCIpFMP_lw?t=5
 66">Multi-Cosmology Simulations</a>\n\n[10:04] <a href="https://youtu.be/X
 xCIpFMP_lw?t=604">"lensing is low"</a>\n\n[13:36] <a href="https://youtu.b
 e/XxCIpFMP_lw?t=816">Getting into the details: Galaxy Redshift-Space Clust
 ering</a>\n\n[15:12] <a href="https://youtu.be/XxCIpFMP_lw?t=912">Galaxy-G
 alaxy Lensing (dsignma python package\, by Johannes)</a>\n\n[17:54] <a hre
 f="https://youtu.be/XxCIpFMP_lw?t=1074">Comparing galaxy-galaxy lensing me
 asurements in this work vs older measurements</a>\n\n[20:18] <a href="http
 s://youtu.be/XxCIpFMP_lw?t=1218">Projected Clustering + Lensing</a>\n\n[22
 :24] <a href="https://youtu.be/XxCIpFMP_lw?t=1344">Mock Galaxy Catalogs</a
 >\n\n[22:41] <a href="https://youtu.be/XxCIpFMP_lw?t=1361">Multi-Cosmology
  Simulations -> Aemulus</a>\n\n[24:09] <a href="https://youtu.be/XxCIpFMP_
 lw?t=1449">HOD (Halo Occupation Distribution) Model</a>\n\n[25:36] <a href
 ="https://youtu.be/XxCIpFMP_lw?t=1536">Assembly Bias</a>\n\n[26:22] <a hre
 f="https://youtu.be/XxCIpFMP_lw?t=1582">Velocity and Spatial Bias</a>\n\n[
 28:20] <a href="https://youtu.be/XxCIpFMP_lw?t=1700">Cosmological Constrai
 nts\; Cosmology Inference</a>\n\n[32:33] <a href="https://youtu.be/XxCIpFM
 P_lw?t=1953">Mock Test\; Figure 2 from paper</a>\n\n[34:48] <a href="https
 ://youtu.be/XxCIpFMP_lw?t=2088">Blinding\; Figure 5</a>\n\n[35:58] <a href
 ="https://youtu.be/XxCIpFMP_lw?t=2158">Data fits\; Figure 6</a>\n\n[38:54]
  <a href="https://youtu.be/XxCIpFMP_lw?t=2334">S8 Constraints plot\; Figur
 e 12 (key slide)</a>\n\n[41:47] <a href="https://youtu.be/XxCIpFMP_lw?t=25
 07">Where to next? Future Directions</a>\n\n[43:15] <a href="https://youtu
 .be/XxCIpFMP_lw?t=2595">SZ Cross-Correlation</a>\n\n[43:50] <a href="https
 ://youtu.be/XxCIpFMP_lw?t=2630">Baryonic Feedback</a>\n\n[44:58] <a href="
 https://youtu.be/XxCIpFMP_lw?t=2698">DESI\, successor to BOSS (expect much
  better constraints)</a>\n\n[45:42] <a href="https://youtu.be/XxCIpFMP_lw?
 t=2742">More tests on mock catalog</a>\n\n[46:23] <a href="https://youtu.b
 e/XxCIpFMP_lw?t=2783">Speculative question: pretend the S8 tension is syst
 ematics\, what might be the leading reason for it?</a>\n\n[47:59] <a href=
 "https://youtu.be/XxCIpFMP_lw?t=2879">What current work in cosmology is pa
 rticularly underappreciated by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/63/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Stuart Lyall (Swinburne University)
DTSTART:20230302T050000Z
DTEND:20230302T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/64
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/64/">Peculiar velocities will detect or constrain modified gravity (e.g
 . f(R) & DGP)</a>\nby Stuart Lyall (Swinburne University) as part of Cosmo
 logy Talks\n\n\nAbstract\nStuart tells us about his recent work exploring 
 how to use peculiar velocity measurements to constrain modified gravity (s
 pecifically f(R) and DGP models). He finds that even using just linear sca
 les we would be able to detect or rule out model parameter regions that wo
 uld be entirely consist with current measurements of the background expans
 ion.\n\nHe does this by predicting the auto and cross spectra between gala
 xy overdensity and peculiar velocity\, using just linear theory - and then
  analysing those observables in modified gravity simulations to measure th
 e parameters used in the simulations.\n\nAt this point it is just a proof 
 of concept\, as for each modified gravity scenario the method is only cons
 training the linear galaxy bias and one model parameter (other cosmologica
 l parameters are known) and also not taking into account additional observ
 ational uncertainties involved in measuring peculiar velocities in the rea
 l world.\n\nStill\, the method does work\, at least when the effect produc
 es a large enough deviation from LCDM so the proof of concept works. Futur
 e careful work with 6DF and SDSS data (and\, one day soon\, DESI) should a
 llow the method to bring about real constraints on these models.\n\n<a hre
 f="https://youtu.be/7tO1GnB628A">Recorded talk</a>\n\nPaper: <a href="http
 s://arxiv.org/abs/2211.07101">arxiv.org/abs/2211.07101</a>\n\n<hr>\n\n<b>I
 ndex to Key Parts of the Talk</b> \n\n[00:00] <a href="https://youtu.be/7t
 O1GnB628A?t=0s">Introductory comments by Shaun and Stuart</a>\n\n[01:35] <
 a href="https://youtu.be/7tO1GnB628A?t=95">Two things you would like peopl
 e to remember from this talk</a>\n\n[02:20] <a href="https://youtu.be/7tO1
 GnB628A?t=140">What is Dark Energy?</a>\n\n[03:38] <a href="https://youtu.
 be/7tO1GnB628A?t=218">Literature review</a>\n\n[04:15] <a href="https://yo
 utu.be/7tO1GnB628A?t=255">Peculiar Velocity</a>\n\n[07:15] <a href="https:
 //youtu.be/7tO1GnB628A?t=435">Growth of Structure</a>\n\n[09:35] <a href="
 https://youtu.be/7tO1GnB628A?t=575">Pipeline Overview</a>\n\n[11:43] <a hr
 ef="https://youtu.be/7tO1GnB628A?t=703">Modified Gravity Models</a>\n\n[15
 :31] <a href="https://youtu.be/7tO1GnB628A?t=931">Simulation Data</a>\n\n[
 16:05] <a href="https://youtu.be/7tO1GnB628A?t=965">Correlation Functions<
 /a>\n\n[17:16] <a href="https://youtu.be/7tO1GnB628A?t=1036">Theoretical C
 orrelation Functions</a>\n\n[21:52] <a href="https://youtu.be/7tO1GnB628A?
 t=1312">χ² Fitting\; Figure 3 from paper</a>\n\n[22:38] <a href="https:/
 /youtu.be/7tO1GnB628A?t=1358">Results\; Figures 7 and 9</a>\n\n[27:20] <a 
 href="https://youtu.be/7tO1GnB628A?t=1640">Fisher Forecasts\; Figures 11 a
 nd 12</a>\n\n[29:52] <a href="https://youtu.be/7tO1GnB628A?t=1792">Apply t
 o Real Surveys\; comments on main purpose of this work</a>\n\n[31:51] <a h
 ref="https://youtu.be/7tO1GnB628A?t=1911">Preliminary Real Results</a>\n\n
 [34:29] <a href="https://youtu.be/7tO1GnB628A?t=2069">Where to next? and I
 nvestigating Environmental Dependence</a>\n\n[36:48] <a href="https://yout
 u.be/7tO1GnB628A?t=2208">What current work in cosmology is particularly un
 derappreciated by the community?</a>\n<br>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/64/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Minh Nguyen (University of Michigan)
DTSTART:20230311T050000Z
DTEND:20230311T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/65
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/65/">3.7 sigma evidence for suppression of growth of structure! (and S_
 8 resolved?)</a>\nby Minh Nguyen (University of Michigan) as part of Cosmo
 logy Talks\n\n\nAbstract\nMinh Nguyen tells us about his recent work looki
 ng for evidence of modified gravity in cosmological observations. Rather t
 han look at a specific model\, Minh and his collaborators look for evidenc
 e of a deviation in the "growth index" γ.\n\nIn general relativity and Λ
 CDM γ≃0.55 but in a more general theory of gravity it could deviate. Mi
 nh looks at measurements of peculiar velocity\, clustering and Planck CMB 
 data (temperature\, polarisation and lensing) and finds 3.7σ evidence for
  γ greater than 0.55.\n\nThis is not perhaps surprising\, as it ties in w
 ith the  S₈ tension. γ quantifies how fast structure grows in the unive
 rse and where we already know there is a deficit of structure in the late 
 universe. Moreover γ greater than 0.55 would cause a deficit. \n\nHowever
 \, it is still impressive that this one parameter is able to provide a goo
 d fit to the various data sets simultaneously. This doesn't look like a "r
 esolution" that takes CMB and late universe probes into bad fitting region
 s of parameter space. In fact\, Planck CMB alone even has weak evidence fo
 r γ greater than 0.55 because it appears to also help with the A_lens ten
 sion.\n\nA fascinating development to keep an eye on...\n\n<a href="https:
 //youtu.be/Tov5KahGEVQ">Talk recording</a>\n\nPaper: <a href="https://arxi
 v.org/abs/2302.01331">arxiv.org/abs/2302.01331</a>\n\nMinh: <a href="https
 ://minhmpa.github.io/">minhmpa.github.io</a>\n\nCode: <a href="https://git
 hub.com/MinhMPA/CAMB_GammaPrime_Growth">github.com/MinhMPA/CAMB_GammaPrime
 _Growth</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/65/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Giovanni Arico (University of Zurich)
DTSTART:20230410T060000Z
DTEND:20230410T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/66
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/66/">Cosmology Without Scale Cuts! (DES Cosmic Shear Baryonified)</a>\n
 by Giovanni Arico (University of Zurich) as part of Cosmology Talks\n\n\nA
 bstract\nGiovanni Arico tells us about his recent work adding baryons to t
 he modelling of Dark Energy Survey cosmic shear analysis. By adding baryon
 ic modelling he and collaborators are able to use all of the DES data. \n\
 nThe cosmological constraints don't tighten a lot\, because although a lot
  of data is added\, the baryonic effects are largely degenerate with cosmo
 logy. However\, they are able to obtain a clear lower bound on one of the 
 baryonic parameters\, which parameterises the typical halo mass that has e
 jected 50% of its gas.\n\nTheir results are 1.4σ different the DES' own c
 osmic shear analysis\, and therefore their S₈ measurement is not in tens
 ion with Planck. This isn't mainly due top the baryons though\, so there i
 s no clear story that "baryons are responsible for the S₈ tension". Inst
 ead the difference comes roughly half from the methods to include non-line
 ar clustering and half from intrinsic alignment modelling.\n\nThis isn't a
  death knell for the S₈ tension in any case because DES cosmic shear alo
 ne wasn't in very large tension with Planck\, and many other measurements 
 are - however it does highlight how a number of assumptions\, each on thei
 r own small enough to perhaps not worry about\, can ultimately add up to s
 omething more substantial.\n\nThe future is bright as\, with appropriate m
 odelling\, the "baryonification" methods used here can be used for all the
  other large scale structure measurements out there. Also\, if the baryon 
 parameters are constrained with additional data sets (tSZ\, kSZ\, X-ray te
 mperature\, stellar mass function\, etc) then the degeneracies with cosmol
 ogical parameters can be broken\, allowing full constraining power from th
 ese small scales.\n\n<a href="https://youtu.be/023dBECojxM">Talk recording
 </a>\n\nGiovanni: <a href="https://www.linkedin.com/in/giovanni-aricò-883
 2684a/">linkedin.com/in/giovanni-aricò-8832684a</a>\n\nPaper: <a href="ht
 tps://arxiv.org/abs/2303.05537">arxiv.org/abs/2303.05537</a>\n\nBACCOemu: 
 <a href="https://bitbucket.org/rangulo/baccoemu/src/master/">bitbucket.org
 /rangulo/baccoemu/src/master/</a>\n\n<hr>\n\n<b>Index to Key Parts of the 
 Talk</b>\n\n[00:00] <a href="https://youtu.be/023dBECojxM?t=0s">Introducto
 ry comments by Shaun</a>\n\n[01:38] <a href="https://youtu.be/023dBECojxM?
 t=98">Giovanni's opening comments on the paper</a>\n\n[02:32] <a href="htt
 ps://youtu.be/023dBECojxM?t=152">Two things for people to remember from th
 is talk</a>\n\n[03:58] <a href="https://youtu.be/023dBECojxM?t=238">What m
 otivated this work?</a>\n\n[05:14] <a href="https://youtu.be/023dBECojxM?t
 =314">Discussion about the scale cuts\, baryonification process\, etc</a>\
 n\n[08:46] <a href="https://youtu.be/023dBECojxM?t=526">Getting into the d
 etails</a>\n\n[11:11] <a href="https://youtu.be/023dBECojxM?t=671">Model: 
 BACCO framework</a>\n\n[16:16] <a href="https://youtu.be/023dBECojxM?t=976
 ">BACCOemu</a>\n\n[18:57] <a href="https://youtu.be/023dBECojxM?t=1137">Pi
 peline: Bayesian inference (Table I in paper\, free parameters)</a>\n\n[22
 :48] <a href="https://youtu.be/023dBECojxM?t=1368">Results: Cosmology (Fig
 ure 3)</a>\n\n[26:21] <a href="https://youtu.be/023dBECojxM?t=1581">Result
 s: Baryons (Figure 4)</a>\n\n[29:53] <a href="https://youtu.be/023dBECojxM
 ?t=1793">Results: Intrinsic Alignment</a>\n\n[31:30] <a href="https://yout
 u.be/023dBECojxM?t=1890">Intrinsic alignment of galaxies: NLA preferred ov
 er TATT</a>\n\n[32:28] <a href="https://youtu.be/023dBECojxM?t=1948">S8 te
 nsion (Figs. 6\, 7)</a>\n\n[36:00] <a href="https://youtu.be/023dBECojxM?t
 =2160">S8 tension (Figure 8)</a>\n\n[40:49] <a href="https://youtu.be/023d
 BECojxM?t=2449">Difference with DES Collaboration (Figure 10)</a>\n\n[49:0
 7] <a href="https://youtu.be/023dBECojxM?t=2947">Q&A on this work in relat
 ion to KiDS</a>\n\n[54:16] <a href="https://youtu.be/023dBECojxM?t=3256">W
 here to next?</a>\n\n[56:32] <a href="https://youtu.be/023dBECojxM?t=3392"
 >What current work in cosmology is particularly underappreciated by the co
 mmunity?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/66/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Jeongin Moon\, David Valcin\, Christoph Saulder (Sejong U\, Ohio U
 \, Max Planck Inst)
DTSTART:20230513T060000Z
DTEND:20230513T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/67
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/67/">Actual DESI Results! - BAO with BOSS Precision after just two mont
 hs</a>\nby Jeongin Moon\, David Valcin\, Christoph Saulder (Sejong U\, Ohi
 o U\, Max Planck Inst) as part of Cosmology Talks\n\n\nAbstract\nJeongin M
 oon\, David Valcin and Christoph Saulder tell us about the first cosmologi
 cally relevant results from DESI (The Dark Energy Spectroscopic Instrument
 ). Specifically\, they are presenting the first detection of the BAO (Bary
 on Acoustic Oscillations) from DESI.\n\nWith a "first detection" one would
  expect something mediocre\, but even this result\, using only two months 
 of DESI data\, has similar precision to the final BOSS data after years of
  operation. This is a very exciting time for cosmology as we wait for the 
 full one year DESI results and cosmological constraints.\n\nJeongin\, Davi
 d and Christoph talk us through the galaxy subsets DESI will use (and whic
 h they have used in this analysis) as well as the statistical significance
  of the BAO detection and modelling required to quantify this.\n\nWith thi
 s detection they are able to also provide a forecast for the one year and 
 five year results that is actually data driven\, based on what they've act
 ually seen so far (rather than just optimistic modelling). The forecast fo
 r the five year measurement looks exquisite.\n\nJeongin: <a href="https://
 arxiv.org/search/astro-ph?query=Moon%2C+Jeongin&searchtype=author">arxiv.o
 rg/search/astro-ph?q...</a>\n\nDavid: <a href="https://inspirehep.net/auth
 ors/1887016">inspirehep.net/authors/1887016</a>\n\nChristoph: <a href="htt
 ps://cosmology.kasi.re.kr/members.php?member=saulder">cosmology.kasi.re.kr
 /members.php?member=saulder</a>\n\nPaper: <a href="https://arxiv.org/abs/2
 304.08427">2304.08427</a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/SHm
 KO5wRlko?t=0s">Intro comments</a>\n\n[01:01] <a href="https://youtu.be/SHm
 KO5wRlko?t=61">When can we expect the year 1 data analysis?</a>\n\n[01:28]
  <a href="https://youtu.be/SHmKO5wRlko?t=88">Two things for people to reme
 mber from this talk</a>\n\n[02:19] <a href="https://youtu.be/SHmKO5wRlko?t
 =139">What are Baryon Acoustic Oscillations?</a>\n\n[04:16] <a href="https
 ://youtu.be/SHmKO5wRlko?t=256">Why are Baryon Acoustic Oscillations Useful
 ?</a>\n\n[05:45] <a href="https://youtu.be/SHmKO5wRlko?t=345">BAO Reconstr
 uction</a>\n\n[09:24] <a href="https://youtu.be/SHmKO5wRlko?t=564">Plan fo
 r DESI</a>\n\n[10:42] <a href="https://youtu.be/SHmKO5wRlko?t=642">The Ins
 trument (and comparison with SDSS)</a>\n\n[12:55] <a href="https://youtu.b
 e/SHmKO5wRlko?t=775">Main tracers of DESI</a>\n\n[16:50] <a href="https://
 youtu.be/SHmKO5wRlko?t=1010">DESI will explore a x30 larger map over a x10
  larger volume than SDSS</a>\n\n[18:17] <a href="https://youtu.be/SHmKO5wR
 lko?t=1097">Our work with early DESI data</a>\n\n[18:52] <a href="https://
 youtu.be/SHmKO5wRlko?t=1132">First two months of observations</a>\n\n[19:3
 4] <a href="https://youtu.be/SHmKO5wRlko?t=1174">Correlation function meas
 urements</a>\n\n[21:40] <a href="https://youtu.be/SHmKO5wRlko?t=1360">Simu
 lations and the covariance matrix</a>\n\n[27:10] <a href="https://youtu.be
 /SHmKO5wRlko?t=1630">Detection in simulations</a>\n\n[30:11] <a href="http
 s://youtu.be/SHmKO5wRlko?t=1811">BAO reconstruction efficiency</a>\n\n[31:
 20] <a href="https://youtu.be/SHmKO5wRlko?t=1880">BAO detection using LRG 
 and BGS</a>\n\n[33:23] <a href="https://youtu.be/SHmKO5wRlko?t=2003">Corre
 lation function measurements</a>\n\n[34:18] <a href="https://youtu.be/SHmK
 O5wRlko?t=2058">Fisher forecast</a>\n\n[35:28] <a href="https://youtu.be/S
 HmKO5wRlko?t=2128">Summary</a>\n\n[37:03] <a href="https://youtu.be/SHmKO5
 wRlko?t=2223">Outlook</a>\n\n[38:21] <a href="https://youtu.be/SHmKO5wRlko
 ?t=2301">What current work in cosmology is particularly underappreciated b
 y the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/67/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Dongwon Han\,  Niall MacCrann\, Mathew Madhavacheril\, Frank Qu\, 
 Blake Sherwin (U of Cambridge\, U of Pennsylvania)
DTSTART:20230525T060000Z
DTEND:20230525T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/68
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/68/">Advanced ACT Lensing Cosmology (the best high redshift\, large sca
 le take on the S8 tension)</a>\nby Dongwon Han\,  Niall MacCrann\, Mathew 
 Madhavacheril\, Frank Qu\, Blake Sherwin (U of Cambridge\, U of Pennsylvan
 ia) as part of Cosmology Talks\n\n\nAbstract\nDongwon Han\,  Niall MacCran
 n\, Mathew Madhavacheril\, Frank Qu\, and Blake Sherwin tell us about the 
 Atacama Cosmology Telescope's latest measurement of CMB weak lensing ("Adv
 anced ACT" to be precise).\n\nIt is quite the measurement. Despite ACT bei
 ng on the ground\, the measurement now rivals the best Planck lensing meas
 urement. This means the additional complications of the atmosphere have be
 en overcome\, and the better technology of telescope possible from not hav
 ing to put something in space are starting to win.\n\nThe results are fasc
 inating in the era of S₈ tensions. They match both Planck CMB and Planck
  lensing (and ACT primary CMB). The CMB lensing measurements are sensitive
  to larger scales and higher redshifts than other large scale structure pr
 obes (because the CMB is further away\, so is lensed by stuff further away
 ). This means that if the S₈ tension is new physics their result seems t
 o be suggesting it must happen at late times and/or on small scales. Perha
 ps this is consistent with what other probes are suggesting too?\n\nIn thi
 s video we hear about the hard work done to eliminate systematic effects a
 nd make sure noise isn't being mistaken for signal\, and then we hear abou
 t the cosmology results and their implications for the future.\n\nPaper 1:
  <a href="https://arxiv.org/abs/2304.05203">arxiv.org/abs/2304.05203</a><b
 r>\nPaper 2: <a href="https://arxiv.org/abs/2304.05202">arxiv.org/abs/2304
 .05202</a><br>\nPaper 3: <a href="https://arxiv.org/abs/2304.05196">arxiv.
 org/abs/2304.05196</a><br>\n\nDongwon: <a href="https://dwhan89.github.io/
 ">dwhan89.github.io</a><br>\nNiall: <a href="https://www.maths.cam.ac.uk/p
 erson/nm746">maths.cam.ac.uk/person/nm746</a><br>\nMathew: <a href="https:
 //live-sas-physics.pantheon.sas.upenn.edu/people/mathew-madhavacheril">upe
 nn.edu/people/mathew-madhavacheril</a><br>\nFrank: <a href="https://www.li
 nkedin.com/in/frankqu7/">linkedin.com/in/frankqu7</a><br>\nBlake: <a href=
 "http://www.damtp.cam.ac.uk/person/bds30">damtp.cam.ac.uk/person/bds30</a>
 \n\n<a href="https://www.youtube.com/watch?v=pB6mwj_V37c&amp\;t=0s">[00:00
 ] Intro bits</a><br>\n<a href="https://www.youtube.com/watch?v=pB6mwj_V37c
 &amp\;t=170s">[02:50]  Why is this important now?</a><br>\n<a href="https:
 //www.youtube.com/watch?v=pB6mwj_V37c&amp\;t=872s">[14:32]  ACT and its ma
 ps</a><br>\n<a href="https://www.youtube.com/watch?v=pB6mwj_V37c&amp\;t=11
 15s">[18:35]  ACT lensing maps</a><br>\n<a href="https://www.youtube.com/w
 atch?v=pB6mwj_V37c&amp\;t=1676s">[27:56]  The power spectrum from the map 
 (and challenges!)</a><br>\n<a href="https://www.youtube.com/watch?v=pB6mwj
 _V37c&amp\;t=2454s">[40:54]  Cosmology Results! (and implications)</a><br>
 \n<a href="https://www.youtube.com/watch?v=pB6mwj_V37c&amp\;t=3689s">[1:01
 :39]  What comes next (and discussion)</a><br>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/68/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Alexandra Amon\, Ami Choi\, Anna Porredon\, Catherine Heymans\, Ma
 rika Asgari\, Simon Samuroff (DES\, KiDS)
DTSTART:20230529T060000Z
DTEND:20230529T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/69
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/69/">DES & KiDS Combined Cosmology Constraints (No Tension with Planck?
 !)</a>\nby Alexandra Amon\, Ami Choi\, Anna Porredon\, Catherine Heymans\,
  Marika Asgari\, Simon Samuroff (DES\, KiDS) as part of Cosmology Talks\n\
 n\nAbstract\nMembers from the Dark Energy Survey and Kilo Degree Survey ha
 ve teamed up to do a joint cosmic shear analysis\, complete with final cos
 mology results. They tell us the final cosmology results\, and go into det
 ails explaining what the technical difficulties were to combine the data s
 ets.\n\nTalk Recording: <a href="https://youtu.be/T8hkgJ-hFoo">youtu.be/T8
 hkgJ-hFoo</a>\n\nTalk Slides: <a href="https://docs.google.com/presentatio
 n/d/1jgR4z9Hb3OVHxcpgWr4VgRXPjWfMTBcqf8rjS3hHjxw">https://docs.google.com/
 presentation...</a>\n\nPaper: <a href="https://arxiv.org/abs/2305.17173">a
 rxiv.org/abs/2305.17173</a>\n\nAlexandra Amon: <a href="https://alexandraa
 mon.com/">alexandraamon.com</a>\n\nAmi Choi: <a href="https://amichoi.gith
 ub.io/">amichoi.github.io</a>\n\nAnna Porredon: <a href="https://www.ph.ed
 .ac.uk/people/anna-porredon">ph.ed.ac.uk/...</a>\n\nCatherine Heymans: <a 
 href="https://www.roe.ac.uk/~heymans/">roe.ac.uk/~heymans</a>\n\nMarika As
 gari: <a href="https://www.hull.ac.uk/staff-directory/marika-asgari">hull.
 ac.uk/...</a>\n\nSimon Samuroff: <a href="https://inspirehep.net/authors/1
 597747?ui-citation-summary=true">inspirehep.net/...</a>\n\nDES: <a href="h
 ttps://www.darkenergysurvey.org/des-year-3-cosmology-results-papers/">dark
 energysurvey.org/...</a>\n\nKiDS: <a href="https://kids.strw.leidenuniv.nl
 /KiDS-1000.php">kids.strw.leidenuniv.nl/......</a>\n\nHSC: <a href="https:
 //hsc-release.mtk.nao.ac.jp/doc/index.php/wly3/">hsc-release.mtk.nao.ac.jp
 /...</a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/T8hkgJ-hFoo?t=0s">Sh
 aun's intro</a>\n\n[01:13] <a href="https://youtu.be/T8hkgJ-hFoo?t=73s">Op
 ening comments on the work\; Fig. 7 from the paper</a>\n\n[05:28] <a href=
 "https://youtu.be/T8hkgJ-hFoo?t=328s">The results: KiDS + DES cosmic shear
 \; Fig. 1</a>\n\n[09:51] <a href="https://youtu.be/T8hkgJ-hFoo?t=591s">Whe
 n can we expect KiDS + DES 3x2pt analysis?</a>\n\n[11:19] <a href="https:/
 /youtu.be/T8hkgJ-hFoo?t=679s">Two takeways for people to remember from thi
 s talk</a>\n\n[12:06] <a href="https://youtu.be/T8hkgJ-hFoo?t=726s">Backgr
 ound on the cosmic shear surveys</a>\n\n[13:52] <a href="https://youtu.be/
 T8hkgJ-hFoo?t=832s">Cosmology from cosmic shear in 2023</a>\n\n[16:20] <a 
 href="https://youtu.be/T8hkgJ-hFoo?t=980s">Overview of the process going f
 rom input images to output cosmological parameters</a>\n\n[21:15] <a href=
 "https://youtu.be/T8hkgJ-hFoo?t=1275s">Analysis choices matter!</a>\n\n[30
 :04] <a href="https://youtu.be/T8hkgJ-hFoo?t=1894s">Choices made between v
 arious possible analysis methods\; Mock analysis\; Hybrid pipeline</a>\n\n
 [36:53] <a href="https://youtu.be/T8hkgJ-hFoo?t=2213s">Re-analysis of KiDS
 -1000 and DES Y3</a>\n\n[42:07] <a href="https://youtu.be/T8hkgJ-hFoo?t=25
 27s">Re-analysis of HSC Y3</a>\n\n[43:52] <a href="https://youtu.be/T8hkgJ
 -hFoo?t=2632s">The combination of the two surveys</a>\n\n[46:27] <a href="
 https://youtu.be/T8hkgJ-hFoo?t=2787s">The S8 tension</a>\n\n[49:40] <a hre
 f="https://youtu.be/T8hkgJ-hFoo?t=2980s">Analysis variants</a>\n\n[52:14:]
  <a href="https://youtu.be/T8hkgJ-hFoo?t=3134s">Accounting for nonlinear g
 rowth and baryonic feedback</a>\n\n[56:05] <a href="https://youtu.be/T8hkg
 J-hFoo?t=3365s">Looking ahead</a>\n\n[59:58] <a href="https://youtu.be/T8h
 kgJ-hFoo?t=3598">What current work in cosmology is particularly underappre
 ciated by the community?</a>\n\n[1:00:56] <a href="https://youtu.be/T8hkgJ
 -hFoo?t=3656s">Comments from Catherine Heymans</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/69/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Jenny Wagner
DTSTART:20230625T060000Z
DTEND:20230625T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/70
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/70/">The Case Against the Cosmological Principle (and/or FLRW)</a>\nby 
 Jenny Wagner as part of Cosmology Talks\n\n\nAbstract\nJenny Wagner gives 
 us the observational case for and against the Cosmological Principle\, bas
 ed on a paper she and 22 co-authors wrote summarising this case. \n\nShe s
 tarts by clearly defining what the Cosmological Principle is and then talk
 s us through the observations that she and her coauthors find to be the mo
 st compelling evidence against the assumptions of full statistical isotrop
 y and homogeneity. In each case she gives us the story either "side" would
  need to tell to reconcile the observation (the standard\, FLRW side and t
 he inhomogeneous cosmology side).\n\nJenny: <a href="https://thegravitygri
 nch.blogspot.com/">thegravitygrinch.blogspot.com</a>\n\nRecording: <a href
 ="https://youtu.be/nASUsWQyemc">https://youtu.be/nASUsWQyemc</a>\n\nPaper:
  <a href="https://arxiv.org/abs/2207.05765">arXiv: 2207.05765</a>\n\n<hr>\
 n\n[00:00] <a href="https://www.youtube.com/watch?v=nASUsWQyemc&t=0s">Intr
 o and take home messages</a>\n\n[07:27] <a href="https://www.youtube.com/w
 atch?v=nASUsWQyemc&t=447s">Background and motivation</a>\n\n[12:40] <a hre
 f="https://www.youtube.com/watch?v=nASUsWQyemc&t=760s">What is the Cosmolo
 gical Principle?</a>\n\n[20:50] <a href="https://www.youtube.com/watch?v=n
 ASUsWQyemc&t=1250s">Half sky analyses of the CMB</a>\n\n[30:19] <a href="h
 ttps://www.youtube.com/watch?v=nASUsWQyemc&t=1819s">'Scale of homogeneity'
 </a>\n\n[38:09] <a href="https://www.youtube.com/watch?v=nASUsWQyemc&t=228
 9s">Variations in time and space of cosmological parameters</a>\n\n[51:05]
  <a href="https://www.youtube.com/watch?v=nASUsWQyemc&t=3065s">Ellis-Baldw
 in and anomalous dipoles</a>\n\n[1:01:47] <a href="https://www.youtube.com
 /watch?v=nASUsWQyemc&t=3707s">What comes next?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/70/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Lilan Yang\, Mike Boylan-Kolchin (Kavli IPMU\, U of Texas)
DTSTART:20230716T060000Z
DTEND:20230716T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/71
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/71/">Too Big\, Too Early? (High Redshift JWST Galaxies)</a>\nby Lilan Y
 ang\, Mike Boylan-Kolchin (Kavli IPMU\, U of Texas) as part of Cosmology T
 alks\n\n\nAbstract\nLilan Yang and Mike Boylan-Kolchin tell us about high 
 redshift JWST galaxies. Lilan is one of the astronomers using JWST to look
  at high redshifts and find new galaxies. Mike is a cosmologist who has pi
 oneered looking at these high redshift galaxies to think about cosmology.\
 n\nRecording: <a href="https://youtu.be/ApB4Jv3P9Gs">https://youtu.be/ApB4
 Jv3P9Gs</a>\n\nPapers: <a href="https://arxiv.org/abs/2207.13101">2207.131
 01</a>\, <a href="https://arxiv.org/abs/2207.13527">2207.13527</a>\, <a hr
 ef="https://arxiv.org/abs/2208.01611">2208.01611</a>\, <a href="https://ar
 xiv.org/abs/2212.06666">2212.06666</a>\n\n00:00 <a href="https://www.youtu
 be.com/watch?v=ApB4Jv3P9Gs&t=0s">Shaun's Intro</a>\n\n01:19 <a href="https
 ://www.youtube.com/watch?v=ApB4Jv3P9Gs&t=79s">Lilan intro to JWST</a>\n\n0
 5:40 <a href="https://www.youtube.com/watch?v=ApB4Jv3P9Gs&t=340s">Lilan: W
 hat are the first stars and galaxies?</a>\n\n13:02 <a href="https://www.yo
 utube.com/watch?v=ApB4Jv3P9Gs&t=782s">Lilan: How did reionization occur?</
 a>\n\n28:03 <a href="https://www.youtube.com/watch?v=ApB4Jv3P9Gs&t=1683s">
 Mike: Are observed structures consistent with initial conditions?</a>\n\n4
 7:01 <a href="https://www.youtube.com/watch?v=ApB4Jv3P9Gs&t=2821s">Mike: P
 hysics beyond ΛCDM</a>\n\n1:00:03 <a href="https://www.youtube.com/watch?
 v=ApB4Jv3P9Gs&t=3603s">Lilan and Mike: Summary and what's next?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/71/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Cyril Creque-Sarbinowski (Center for Computational Astrophysics\, 
 Flatiron Institute)
DTSTART:20230827T060000Z
DTEND:20230827T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/72
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/72/">Parity Violation from Inflation (via Chern-Simons Gravity)</a>\nby
  Cyril Creque-Sarbinowski (Center for Computational Astrophysics\, Flatiro
 n Institute) as part of Cosmology Talks\n\n\nAbstract\nCyril Creque-Sarbin
 owski tells us about recent work on Chern-Simons gravity and how if it is 
 the correct general model of gravity then parity violation can be generate
 d during inflation in such a way that correlation functions of galaxies me
 asured today could see that parity violation. Given the recent evidence fo
 r parity violation in galaxy correlation functions\, that is intriguing.\n
 \nThe model also requires parameter values that could produce baryogenesis
 \, so the same physics would end up producing the (observed?) parity viola
 tion and the baryon asymmetry in the universe.\n\nEven if the current hint
 s of parity violation turn out to be wrong\, future experiments would be s
 ensitive to smaller magnitudes of this effect\, meaning the model will be 
 well constrained by the next wave of large scale structure measurements\n\
 nCyril: <a href="https://cyril-creque.github.io/">cyril-creque.github.io</
 a>\n\nPaper: <a href="https://arxiv.org/abs/2303.04815">arxiv.org/abs/2303
 .04815</a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/IxhbpfblhQQ?t=0">S
 ean's intro</a>\n\n[00:47] <a href="https://youtu.be/IxhbpfblhQQ?t=47">Cyr
 il's brief intro on the paper</a>\n\n[01:46] <a href="https://youtu.be/Ixh
 bpfblhQQ?t=106">Two things to remember from this talk</a>\n\n[02:17] <a hr
 ef="https://youtu.be/IxhbpfblhQQ?t=137">The motivation for this work</a>\n
 \n[03:15] <a href="https://youtu.be/IxhbpfblhQQ?t=195">What is Parity? How
  can Gravity violate it?</a>\n\n[05:25] <a href="https://youtu.be/Ixhbpfbl
 hQQ?t=325">What is [dynamical] Chern-Simons (dCS) Gravity?</a>\n\n[07:33] 
 <a href="https://youtu.be/IxhbpfblhQQ?t=453">How can Parity be Observed? (
 Galaxy N-Point Functions)</a>\n\n[09:02] <a href="https://youtu.be/Ixhbpfb
 lhQQ?t=542">The Galaxy Four Point Function / Trispectrum</a>\n\n[11:53] <a
  href="https://youtu.be/IxhbpfblhQQ?t=713">Inflation: A Lightning Review</
 a>\n\n[14:43] <a href="https://youtu.be/IxhbpfblhQQ?t=883">dCS Inflation: 
 Full Action</a>\n\n[18:58] <a href="https://youtu.be/IxhbpfblhQQ?t=1138">P
 rimordial Scalar Trispectrum from dCS</a>\n\n[23:55] <a href="https://yout
 u.be/IxhbpfblhQQ?t=1435">The Collapsed Limit</a>\n\n[24:24] <a href="https
 ://youtu.be/IxhbpfblhQQ?t=1464">The Collapsed Limit Scalar Trispectra</a>\
 n\n[31:21] <a href="https://youtu.be/IxhbpfblhQQ?t=1881">Two Examples Beyo
 nd Vanilla dCS Inflation</a>\n\n[35:37] <a href="https://youtu.be/Ixhbpfbl
 hQQ?t=2137">How Sensitive are we to Collapsed Trispectra?</a>\n\n[44:05] <
 a href="https://youtu.be/IxhbpfblhQQ?t=2645">What about Experiments?</a>\n
 \n[46:17] <a href="https://youtu.be/IxhbpfblhQQ?t=2777">dCS Inflation: Lep
 to/Baryogenesis</a>\n\n[53:35] <a href="https://youtu.be/IxhbpfblhQQ?t=321
 5">Conclusions / Future Extensions</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/72/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Gerrit Farren\, Alex Krolewski (Cambridge\, Perimeter Institute)
DTSTART:20230911T060000Z
DTEND:20230911T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/73
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/73/">S8 at low redshift and large scales - ACT lensing X unWISE galaxie
 s</a>\nby Gerrit Farren\, Alex Krolewski (Cambridge\, Perimeter Institute)
  as part of Cosmology Talks\n\n\nAbstract\nGerrit Farren and Alex Krolewsk
 i tell us about their work cross correlating the ACT lensing maps with unW
 ISE galaxies. Their method is an update of earlier analyses using Planck l
 ensing. Those earlier analyses were in tension with Planck primary CMB mea
 surements\, which was similar to e.g. cosmic shear\, and other clustering 
 measurements\, at smaller scales.\n\nCuriously\, this new analysis reveals
  no tension with primary CMB. A re-analysis of Planck lensing cross unWISE
 \, with updated assumptions and modelling\, shows that Planck lensing is a
 ctually also not in tension with primary CMB (a combination of effects wer
 e responsible for removing the tension).\n\nThis analysis covers the large
 (ish) scale low(ish) redshift quadrant of the (k\,z) space\, suggesting th
 at the origin of the S8 tension is likely to either be a very low redshift
  phenomenon\, or scale dependent.\n\nHowever Alex and Gerrit do note that 
 a recent cross-correlation of Planck with DESI LRGs does seem to still ind
 icate some tension at the same redshift and scales\, so the dust hasn't 10
 0% settled on the large scale\, low redshift quadrant.\n\nVideo recording:
  <a href="https://youtu.be/Y_QMPWDi95s">youtu.be/Y_QMPWDi95s</a>\n\nGerrit
 : <a href="https://www.maths.cam.ac.uk/person/gsf29">maths.cam.ac.uk/perso
 n/gsf29</a>\n\nAlex: <a href="https://perimeterinstitute.ca/people/alex-kr
 olewski">perimeterinstitute.ca/people/alex-krolewski</a>\n\nPaper: <a href
 ="https://arxiv.org/abs/2309.05659">arXiv: 2309.05659</a>\n\n<hr>\n[00:00]
  <a href="https://youtu.be/Y_QMPWDi95s?t=0s">Shaun's intro</a>\n\n[01:06] 
 <a href="https://youtu.be/Y_QMPWDi95s?t=66">Overview comments by Gerrit an
 d Alex</a>\n\n[03:31] <a href="https://youtu.be/Y_QMPWDi95s?t=211">Two thi
 ngs to remember from this talk</a>\n\n[04:40] <a href="https://youtu.be/Y_
 QMPWDi95s?t=280">Motivations for this work</a>\n\n[07:41] <a href="https:/
 /youtu.be/Y_QMPWDi95s?t=461">Measuring S8 with galaxy-CMB lensing cross-co
 rrelations</a>\n\n[09:16] <a href="https://youtu.be/Y_QMPWDi95s?t=556">New
  ACT DR6 X unWISE spectra (Fig. 3 from paper)</a>\n\n[12:03] <a href="http
 s://youtu.be/Y_QMPWDi95s?t=723">Q&A: Advantages of using UnWISE vs eBOSS i
 n this work</a>\n\n[13:13] <a href="https://youtu.be/Y_QMPWDi95s?t=793">Ba
 ckground: defining the unWISE sample</a>\n\n[18:21] <a href="https://youtu
 .be/Y_QMPWDi95s?t=1101">Background: previous unWISE-Planck results</a>\n\n
 [19:08] <a href="https://youtu.be/Y_QMPWDi95s?t=1148">Clustering redshifts
  for unWISE</a>\n\n[21:00] <a href="https://youtu.be/Y_QMPWDi95s?t=1260">I
 mproving the galaxy sample: updated redshift distribution</a>\n\n[22:24] <
 a href="https://youtu.be/Y_QMPWDi95s?t=1344">Mitigating systematic density
  fluctuations</a>\n\n[25:59] <a href="https://youtu.be/Y_QMPWDi95s?t=1559"
 >Modelling improvements: Redshift marginalisation (Fig. 17)</a>\n\n[27:45]
  <a href="https://youtu.be/Y_QMPWDi95s?t=1665">Modelling improvements: The
  power spectrum model</a>\n\n[29:36] <a href="https://youtu.be/Y_QMPWDi95s
 ?t=1776">Series of systematics tests: Data null-tests</a>\n\n[31:06] <a hr
 ef="https://youtu.be/Y_QMPWDi95s?t=1866">Series of systematics tests: Simu
 lation driven tests (Fig. 12)</a>\n\n[31:58] <a href="https://youtu.be/Y_Q
 MPWDi95s?t=1918">Series of systematics tests: Parameter consistency tests 
 (Fig. 21)</a>\n\n[32:28] <a href="https://youtu.be/Y_QMPWDi95s?t=1948">Cos
 mology from ACT DR6 Lensing X unWISE (Fig. 19)</a>\n\n[35:33] <a href="htt
 ps://youtu.be/Y_QMPWDi95s?t=2133">Reanalysing Planck Lensing X unWISE: MC 
 norm correction</a>\n\n[36:47] <a href="https://youtu.be/Y_QMPWDi95s?t=220
 7">Reanalysing Planck Lensing X unWISE: Planck PR4 lensing</a>\n\n[37:16] 
 <a href="https://youtu.be/Y_QMPWDi95s?t=2236">Reanalysing Planck Lensing X
  unWISE: summary of changes</a>\n\n[38:12] <a href="https://youtu.be/Y_QMP
 WDi95s?t=2292">Reanalysing Planck Lensing X unWISE: Cosmology</a>\n\n[40:2
 2] <a href="https://youtu.be/Y_QMPWDi95s?t=2422">Joint constraints from AC
 T DR6 and Planck PR4 X unWISE (Fig. 23)</a>\n\n[41:12] <a href="https://yo
 utu.be/Y_QMPWDi95s?t=2472">Comparing to other analyses (Fig. 23)</a>\n\n[4
 5:09] <a href="https://youtu.be/Y_QMPWDi95s?t=2709">Future CMB lensing cro
 ss-correlations</a>\n\n[50:51] <a href="https://youtu.be/Y_QMPWDi95s?t=305
 1">What current work in cosmology is particularly underappreciated by the 
 community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/73/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Melissa Diamond\, Chris Cappiello (Queens U.)
DTSTART:20231003T050000Z
DTEND:20231003T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/74
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/74/">If Dark Matter Interacts with Protons We Could See It Scatter Elec
 trons</a>\nby Melissa Diamond\, Chris Cappiello (Queens U.) as part of Cos
 mology Talks\n\n\nAbstract\nMelissa Diamond\, joined by Chris Cappiello\, 
 tells us how dark matter interactions with one set of standard model parti
 cles might be first constrained via experiments looking for interactions w
 ith other particles.\n\nAs a first example they explore how loop diagrams 
 that arise when dark matter interacts with quarks (and thus pions\, neutro
 ns and protons)\, necessarily introduce an interaction with electrons too.
  For light enough dark matter\, this would mean that the first direct dete
 ction of these dark matter models would come via electron scattering exper
 iments\, not nucleon scattering experiments.\n\nAt the moment this just ad
 ds to constraints in somewhat less-interesting parameter space\, but futur
 e experiments will push the constraints into well motivated parameter rang
 es for dark matter production mechanisms.\n\nThis loop interaction would a
 lso generate a dark matter "millicharge"\, which could be combined with as
 trophysical observations to make even tighter constraints.\n\nTalk recordi
 ng: <a href="https://youtu.be/gixAFpnVhAw">youtu.be/gixAFpnVhAw</a>\n\nPap
 er: <a href="https://arxiv.org/abs/2307.13727">arXiv: 2307.13727</a>\n\nMe
 lissa: <a href="https://inspirehep.net/authors/1945406">inspirehep.net/aut
 hors/1945406</a>\n\nChris: <a href="https://mcdonaldinstitute.ca/chris-cap
 piello/">mcdonaldinstitute.ca/chris-cappiello</a>\n\n<hr>\n\n<strong>Index
  to Key Parts of the Talk</strong>\n\n[00:00] <a href="https://youtu.be/gi
 xAFpnVhAw?t=0s">Shaun's intro</a>\n\n[00:56] <a href="https://youtu.be/gix
 AFpnVhAw?t=56">Overview comments by Melissa</a>\n\n[01:39] <a href="https:
 //youtu.be/gixAFpnVhAw?t=99">Two things to remember from this talk</a>\n\n
 [02:31] <a href="https://youtu.be/gixAFpnVhAw?t=151">Motivations for this 
 work</a>\n\n[04:48] <a href="https://youtu.be/gixAFpnVhAw?t=288">Explanati
 on of Figure 1 from paper</a>\n\n[06:20] <a href="https://youtu.be/gixAFpn
 VhAw?t=380">Why should there be an interaction of DM with the SM?</a>\n\n[
 08:04] <a href="https://youtu.be/gixAFpnVhAw?t=484">More specific motivati
 on</a>\n\n[09:35] <a href="https://youtu.be/gixAFpnVhAw?t=575">Chris on SE
 NSEI and DAMIC</a>\n\n[12:24] <a href="https://youtu.be/gixAFpnVhAw?t=744"
 >Explanation of the blue Cosmology line on the plot</a>\n\n[13:20] <a href
 ="https://youtu.be/gixAFpnVhAw?t=800">Getting into the details (Figs. 2\, 
 7)</a>\n\n[20:41] <a href="https://youtu.be/gixAFpnVhAw?t=1241">Chiral Eff
 ective Interaction</a>\n\n[26:44] <a href="https://youtu.be/gixAFpnVhAw?t=
 1604">Calculating the Cross Sections</a>\n\n[30:50] <a href="https://youtu
 .be/gixAFpnVhAw?t=1850">Effective Electron Cross Section</a>\n\n[32:25] <a
  href="https://youtu.be/gixAFpnVhAw?t=1945">Probe Hadrophilic DM with a He
 avy Mediator using Electron Coil Detectors</a>\n\n[35:15] <a href="https:/
 /youtu.be/gixAFpnVhAw?t=2115">Bounds from Effective Millicharge</a>\n\n[44
 :48] <a href="https://youtu.be/gixAFpnVhAw?t=2688">Where to next?</a>\n\n[
 52:12] <a href="https://youtu.be/gixAFpnVhAw?t=3132">What current work in 
 cosmology is particularly underappreciated by the community?\n</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/74/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Kate Clements (University of Nottingham)
DTSTART:20231103T050000Z
DTEND:20231103T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/75
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/75/">A Lab Experiment to Detect Dark Sector Domain Wall</a>\nby Kate Cl
 ements (University of Nottingham) as part of Cosmology Talks\n\n\nAbstract
 \nKate tells us about her recent work showing how domain walls in the dark
  sector could be trapped in a laboratory. \n\nIn many well motivated model
 s\, a scalar field in the dark sector can have a double well potential. In
  this case\, the scalar field can form "domain walls" if in some region of
  space the field occupies one side of the well\, and in other regions of s
 pace the field occupies the other side of the well. The wall occurs at the
  transition point between the two regions.\n\nNormally such domain walls w
 ill not stick around\, either evaporating\, or simply moving away from an 
 observer. However\, by putting a density spike in a vacuum chamber one can
  trap a domain wall in place. Once trapped\, one could observe the domain 
 wall's effects on standard model particles\, e.g. cold atoms\, via a chang
 e in a fifth force.\n\nOf all the ways we're looking for new fundamental p
 hysics\, this sort of experiment would be the coolest if it worked\, as it
  would be reproducible in labs around the world\, making experimental fund
 amental physics cheap (ish) again.\n\nPaper: <a href="https://arxiv.org/ab
 s/2308.01179">arXiv:2308.01179</a>\n\nTalk Video: <a href="https://youtu.b
 e/U6arawZnxHQ">youtu.be/U6arawZnxHQ</a>\n\nKate: <a href="https://www.link
 edin.com/in/kate-clements-499770b8/">linkedin.com: Kate Clements</a>\n\n<h
 r>\n\n<strong>Index to Key Parts of the Talk</strong><br>\n[00:00] <a href
 ="https://youtu.be/U6arawZnxHQ?t=0s">Shaun's intro</a>\n\n[00:39] <a href=
 "https://youtu.be/U6arawZnxHQ?t=39s">Overview comments by Kate</a>\n\n[01:
 21] <a href="https://youtu.be/U6arawZnxHQ?t=81s">Two things to remember fr
 om this talk</a>\n\n[02:07] <a href="https://youtu.be/U6arawZnxHQ?t=127s">
 Motivations for this work (Fig. 1 from the paper)</a>\n\n[04:42] <a href="
 https://youtu.be/U6arawZnxHQ?t=282s">Detecting Dark Domain Walls</a>\n\n[0
 5:57] <a href="https://youtu.be/U6arawZnxHQ?t=357s">What is a Domain Wall?
 </a>\n\n[08:45] <a href="https://youtu.be/U6arawZnxHQ?t=525s">Infinite Dom
 ain Walls</a>\n\n[09:37] <a href="https://youtu.be/U6arawZnxHQ?t=577s">Vac
 uum Chamber Experiment</a>\n\n[12:49] <a href="https://youtu.be/U6arawZnxH
 Q?t=769s">Thin Domain Walls (Fig. 2)</a>\n\n[14:41] <a href="https://youtu
 .be/U6arawZnxHQ?t=881s">Thick Domain Walls (Fig. 3)</a>\n\n[16:00] <a href
 ="https://youtu.be/U6arawZnxHQ?t=960s">What Next?</a>\n\n[24:48] <a href="
 https://youtu.be/U6arawZnxHQ?t=1488s">What current work in cosmology is pa
 rticularly underappreciated by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/75/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Keir Rogers\, Vivian Poulin (U Toronto\, U Montpellier)
DTSTART:20231201T050000Z
DTEND:20231201T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/76
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/76/">4.9σ evidence for axions & warm dark matter - eBOSS Lyα vs Planc
 k CMB</a>\nby Keir Rogers\, Vivian Poulin (U Toronto\, U Montpellier) as p
 art of Cosmology Talks\n\n\nAbstract\nKeir and Vivian tell us about their 
 recent work looking at the Lyman-α power spectrum from eBOSS quasars. Spe
 cifically\, they look at how consistent this power spectrum is with the po
 wer spectrum one would expect from the relevant scales given Planck CMB ob
 servations within the ΛCDM model and find a whopping 4.9σ tension.\n\nTh
 ere have been hints of a tension between Lyman-α and CMB for a while\, bu
 t not with this magnitude. Keir and Vivian focus their analysis on the sca
 les and observables that the eBOSS Lyman-α are most sensitive to and see 
 that the slope of the power spectrum of this range of scales is very diffe
 rent to what is seen on CMB scales. Within ΛCDM the slope of the power sp
 ectrum should be constant\, hence the whopping tension.\n\nMost excitingly
 \, they also find three simple models that more or less completely solve t
 he tension\, without harming any other observations! These are a one-param
 eter power-law running of the "spectral index" (i.e. the slope of the powe
 r spectrum)\, and a small fraction of axion "ultralight" dark matter\, or 
 warm dark matter. For the axion and warm dark matter models there are two 
 free parameters (the mass and the fraction of the total dark matter). The 
 running and axion models in particular completely remove the tension\, and
  the warm dark matter reduces the "tension" to 1.5σ. Very exciting!\n\nVi
 deo Recording: <a href="https://youtu.be/_cueUDEf6n4">youtu.be/_cueUDEf6n4
 </a>\n\nKeir: <a href="https://keirkwame.github.io/">keirkwame.github.io/<
 /a>\n\nVivian: <a href="https://inspirehep.net/authors/1341720">inspire.ne
 t/authors/1341720</a>\n\nPaper: <a href="https://arxiv.org/abs/2311.16377"
 >arXiv: 2311.16377</a>\n\n<hr>\n\n<strong>Index to Key Parts of the Talk</
 strong>\n[00:00] <a href="https://youtu.be/_cueUDEf6n4?t=0s">Shaun's intro
 </a>\n\n[01:04] <a href="https://youtu.be/_cueUDEf6n4?t=64s">Overview comm
 ents by Keir and Viv</a>\n\n[03:25] <a href="https://youtu.be/_cueUDEf6n4?
 t=205s">Two things to remember from this talk</a>\n\n[06:45] <a href="http
 s://youtu.be/_cueUDEf6n4?t=405s">Motivations for this work</a>\n\n[11:35] 
 <a href="https://youtu.be/_cueUDEf6n4?t=695s">Getting into the Details</a>
 \n\n[15:57] <a href="https://youtu.be/_cueUDEf6n4?t=957s">All the cosmolog
 ical info in the eBOSS Lyα forest compressed to two parameters</a>\n\n[17
 :20] <a href="https://youtu.be/_cueUDEf6n4?t=1040s">This compression is va
 lid for all the models we consider (Fig. 4 from paper)</a>\n\n[18:26] <a h
 ref="https://youtu.be/_cueUDEf6n4?t=1106s">4.9σ tension between eBOSS Ly-
 αf & Planck CMB (Fig. 1)</a>\n\n[20:11] <a href="https://youtu.be/_cueUDE
 f6n4?t=1211s">Clarifying comments by Shaun (editing insert)</a>\n\n[23:27]
  <a href="https://youtu.be/_cueUDEf6n4?t=1407s">CMB+BAO+SNe vs Lyα\; powe
 r spectrum running\, ULA\, WDM (Fig. 2 top)</a>\n\n[34:40] <a href="https:
 //youtu.be/_cueUDEf6n4?t=2080s">Tension missed when looking at omega_8\, n
 _s (Fig. 2 bottom</a>\n\n[36:35] <a href="https://youtu.be/_cueUDEf6n4?t=2
 195s">Planck CMB+BAO+SNe+eBOSS Ly-αf constraints on primordial power spec
 trum (Fig. 3)</a>\n\n[37:39] <a href="https://youtu.be/_cueUDEf6n4?t=2259s
 ">Planck CMB+BAO+SNe+eBOSS Ly-αf constraints on nature of dark matter (Fi
 g. 3)</a>\n\n[39:25] <a href="https://youtu.be/_cueUDEf6n4?t=2365s">What e
 lse may be causing this discrepancy?</a>\n\n[41:35] <a href="https://youtu
 .be/_cueUDEf6n4?t=2495s">Where to next?</a>\n\n[51:29] <a href="https://yo
 utu.be/_cueUDEf6n4?t=3089s">Vivian's supplemental comment on neutrino mass
  constraints</a>\n\n[52:38] <a href="https://youtu.be/_cueUDEf6n4?t=3158s"
 >Keir - follow-up coming from DESI</a>\n\n[52:59] <a href="https://youtu.b
 e/_cueUDEf6n4?t=3179s">What current work in cosmology is particularly unde
 rappreciated by the community?</a>\n\n[55:23] <a href="https://youtu.be/_c
 ueUDEf6n4?t=3323s">Final question to Keir about how these findings relate 
 to work discussed in an earlier Cosmology Talk</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/76/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Lamman\, Legnani\, Shi\, Sarcevic\, Pyne\, and Ferreira
DTSTART:20240221T050000Z
DTEND:20240221T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/77
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/77/">Intrinsic Alignments: A Guide for Everyone</a>\nby Lamman\, Legnan
 i\, Shi\, Sarcevic\, Pyne\, and Ferreira as part of Cosmology Talks\n\n\nA
 bstract\nClaire Lamman\, Jingjing Shi\, Niko Šarčević\, Susan Pyne\, El
 isa Legnani and Tassia Ferreira tell us about the intrinsic alignments gui
 de they wrote (along with Eleni Tsaprazi\, who couldn’t make the video r
 ecording).\n\nThey wanted to write something that wasn’t quite a review\
 , but also wasn’t quite a set of lecture notes. Instead they aimed for w
 hat might be best framed as a “cheat sheet” for intrinsic alignments. 
 Everything you need to know about the topic\, compressed into one article.
  However\, there’s still a lot about the topic\, so the compression is s
 till 33 pages and 10 figures big.\n\nTo construct the guide they broke the
  topic of intrinsic alignments into sub-fields and then asked questions li
 ke “what are the key equations for this sub-field?”\, “what are the 
 different notations people use?”\, “what might be confusing to a newco
 mer?” They then wrote the guide to answer those questions\, even includi
 ng subsections with quick definitions of each common term\, and short list
 s of common alternative notations.\n\nIn this video they go over both the 
 guide and the topic of intrinsic alignments.\n\nVideo: <a href="https://yo
 utu.be/BlibRW4XpR8">youtu.be/BlibRW4XpR8</a>\n\nPaper: <a href="https://ar
 xiv.org/abs/2309.08605">arXiv:2309.08605 </a>\n\n\nClaire: <a href="https:
 //cmlamman.github.io/">cmlamman.github.io/</a>\n\nJingjing: <a href="https
 ://www.jshiastro.com/home">jshiastro.com</a>\n\nNiko: <a href="https://nik
 osarcevic.com/">nikosarcevic.com</a>\n\nSusan: <a href="https://www.ucl.ac
 .uk/astrophysics/susan-pyne-honorary-research-fellow">www.ucl.ac.uk/astrop
 hysics/susan-pyne-honorary-research-fellow</a>\n\nElisa: <a href="https://
 elisalegnani.github.io/">elisalegnani.github.io</a>\n\nTassia: <a href="ht
 tps://www.physics.ox.ac.uk/our-people/ferreirat">physics.ox.ac.uk/our-peop
 le/ferreirat</a>\n\nEleni: <a href="https://tsaprazi.eu/">https://tsaprazi
 .eu</a>\n\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b>\n\n[0:00:00] <a
  href="https://youtu.be/BlibRW4XpR8?t=0s">Shaun's intro</a>\n\n[0:01:13] <
 a href="https://youtu.be/BlibRW4XpR8?t=73s">What are intrinsic alignments?
  plus IA cheat sheet</a>\n\n[0:02:54] <a href="https://youtu.be/BlibRW4XpR
 8?t=174s">Two things to remember from this talk</a>\n\n[0:03:17] <a href="
 https://youtu.be/BlibRW4XpR8?t=197s">Getting into the background and detai
 ls</a>\n\n[0:10:04] <a href="https://youtu.be/BlibRW4XpR8?t=604s">Elliptic
 ity (section 2 of paper*)</a>\n\n[0:12:38] <a href="https://youtu.be/BlibR
 W4XpR8?t=758s">Galaxy types and shapes</a>\n\n[0:16:31] <a href="https://y
 outu.be/BlibRW4XpR8?t=991s">IA Correlation Function Notation (section 4*)<
 /a>\n\n[0:19:02] <a href="https://youtu.be/BlibRW4XpR8?t=1142s">IA Correla
 tion Functions (section 5*)</a>\n\n[0:23:01] <a href="https://youtu.be/Bli
 bRW4XpR8?t=1381s">Correlations</a>\n\n[0:23:34] <a href="https://youtu.be/
 BlibRW4XpR8?t=1414s">Shear (section 3*)</a>\n\n[0:30:54] <a href="https://
 youtu.be/BlibRW4XpR8?t=1854s">3D IA Power Spectrum (section 6*)</a>\n\n[0:
 38:33] <a href="https://youtu.be/BlibRW4XpR8?t=2313">2D IA Power Spectrum 
 (section 7*)</a>\n\n[0:46:01] <a href="https://youtu.be/BlibRW4XpR8?t=2761
 s">Modeling (section 8*)</a>\n\n[1:00:41] <a href="https://youtu.be/BlibRW
 4XpR8?t=3641s">Where to next?</a>\n\n[1:06:44] <a href="https://youtu.be/B
 libRW4XpR8?t=4004s">What current work in cosmology is particularly underap
 preciated by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/77/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Pritha Paul\, Chris Clarkson (QMUL)
DTSTART:20240308T050000Z
DTEND:20240308T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/78
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/78/">There is Parity Violation in Standard Observational Cosmology</a>\
 nby Pritha Paul\, Chris Clarkson (QMUL) as part of Cosmology Talks\n\n\nAb
 stract\nThere is Parity Violation in Standard Observational Cosmology (Pri
 tha Paul and Chris Clarkson)\n\nPritha Paul and Chris Clarkson tell us abo
 ut their work\, along with Roy Maartens\, delving very deeply into standar
 d observational cosmology. Specifically\, they have looked at relativistic
  effects in the four point function/trispectrum of galaxy positions.\n\nTh
 is might sound crazy and masochistic\, but there are big rewards. On large
  enough scales\, the relativistic effects start to grow\, and tantalisingl
 y\, once one takes into account both relativistic effects and the observat
 ional effects of observing in redshift space\, a parity violating signal e
 merges in both the bispectrum and trispectrum on large scales. This is ver
 y interesting given the possible observations of parity violation in the f
 our point function of galaxy positions (i.e. Fourier transform of the tris
 pectrum).\n\nThere are reasons to suspect the effect Pritha\, Chris and Ro
 y have uncovered within standard cosmology couldn't be the thing potential
 ly observed in the four point function\, however it is possible to at leas
 t tell a story about how the one effect might show up in the other observa
 tion. Time will tell whether they are indeed related.\n\nIrrespective of t
 hat\, the result is still interesting as it is likely that Euclid and/or S
 KA will be able to spot this signal\, thus detecting the effects of relati
 vity within the large scale structure.\n\n<a href="https://youtu.be/WPlrF9
 GvDHM">Talk recording on the Cosmology Talks youtube channel</a>\n\n<a hre
 f="https://www.qmul.ac.uk/spcs/staff/research-students/profiles/ppaul.html
 ">Pritha's QMUL profile page</a>\n\n<a href="https://www.qmul.ac.uk/spcs/s
 taff/academics/profiles/chrisclarkson.html">Chris' QMUL profile page</a>\n
 \nPaper: <a href="https://arxiv.org/abs/2402.16478">arXiv: 2402.16478</a>\
 n\n<hr>\n\n<b>Index to Key Parts of the Talk</b>\n\n[00:00] <a href="https
 ://youtu.be/WPlrF9GvDHM?t=0s">Shaun's intro</a>\n\n[01:26] <a href="https:
 //youtu.be/WPlrF9GvDHM?t=86s">Overview by Pritha and Chris and 2 takeaways
  from the talk</a>\n\n[02:34] <a href="https://youtu.be/WPlrF9GvDHM?t=154s
 ">What is the motivation for this work?</a>\n\n[05:03] <a href="https://yo
 utu.be/WPlrF9GvDHM?t=303s">Why the 4-pt correlation function is needed</a>
 \n\n[05:58] <a href="https://youtu.be/WPlrF9GvDHM?t=358s">Recent work by o
 thers</a>\n\n[09:37] <a href="https://youtu.be/WPlrF9GvDHM?t=577s">Large S
 cale Surveys</a>\n\n[11:35] <a href="https://youtu.be/WPlrF9GvDHM?t=695s">
 Real Space to Redshift Space - Power Spectrum</a>\n\n[15:36] <a href="http
 s://youtu.be/WPlrF9GvDHM?t=936s">Real Space to Redshift Space - Bipectrum<
 /a>\n\n[19:38] <a href="https://youtu.be/WPlrF9GvDHM?t=1178s">Tree Level T
 rispectrum</a>\n\n[20:59] <a href="https://youtu.be/WPlrF9GvDHM?t=1259s">T
 rispectrum Geometry</a>\n\n[21:43] <a href="https://youtu.be/WPlrF9GvDHM?t
 =1303s">Third order number counts</a>\n\n[26:30] <a href="https://youtu.be
 /WPlrF9GvDHM?t=1590s">Trispectrum</a>\n\n[26:55] <a href="https://youtu.be
 /WPlrF9GvDHM?t=1615s">Calculating the Trispectrum</a>\n\n[30:50] <a href="
 https://youtu.be/WPlrF9GvDHM?t=1850s">15-min Q & A segment</a>\n\n[46:10] 
 <a href="https://youtu.be/WPlrF9GvDHM?t=s1770">What current work in cosmol
 ogy is particularly underappreciated by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/78/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Sylvia Wenmachers (Institute of Philosophy\, KU Leuven)
DTSTART:20240316T050000Z
DTEND:20240316T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/79
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/79/">New Probability Axioms Could Fix Cosmology's Multiverse (Partially
 )</a>\nby Sylvia Wenmachers (Institute of Philosophy\, KU Leuven) as part 
 of Cosmology Talks\n\n\nAbstract\nSylvia is a philosopher of science. Her 
 focus is probability and she has worked on a few theories that aim to exte
 nd and modify the standard axioms of probability in order to tackle parado
 xes related to infinite spaces. In particular there is a paradox of the "i
 nfinite fair lottery" where within standard probability it seems impossibl
 e to write down a "fair" probability function on the integers. If you give
  the integers any non-zero probability\, the total probability of all inte
 gers is unbounded\, so the function is not normalisable. If you give the i
 ntegers zero probability\, the total probability of all integers is also z
 ero. No other option seems viable for a fair distribution.\n\nThis paradox
  arises in a number of places within cosmology\, especially in the context
  of eternal inflation and a possible multiverse of big bangs bubbling off.
  If every bubble is to be treated fairly\, and there will ultimately be an
  unbounded number of them\, how do we assign probability?\n\nThe proposed 
 solutions involve hyper-real numbers\, such as infinitesimals and infiniti
 es with different relative sizes\, (reflecting how quickly things converge
  or diverge respectively).\n\nThe multiverse has other problems\, and othe
 r areas of cosmology where this issue arises also have their own problems 
 (e.g. the initial conditions of inflation)\; however this could very well 
 be part of the way towards fixing the cosmological multiverse.\n\nTalk rec
 ording: <a href="https://youtu.be/MBeSoig4DPY">youtu.be/MBeSoig4DPY</a>\n\
 nSylvia: <a href="https://www.sylviawenmackers.be/">sylviawenmackers.be</a
 >\n\nPaper: <a href="https://arxiv.org/abs/2308.12229">arXiv: 2308.12229</
 a>\n\n<hr>\n\n[0:00:00] <a href="https://youtu.be/MBeSoig4DPY?t=0s">Shaun'
 s intro</a>\n\n[0:02:17] <a href="https://youtu.be/MBeSoig4DPY?t=137s">Syl
 via's overview</a>\n\n[0:03:49] <a href="https://youtu.be/MBeSoig4DPY?t=22
 9s">Two takeaways from this talk</a>\n\n[0:06:36] <a href="https://youtu.b
 e/MBeSoig4DPY?t=396s">The motivation and reason for timing of this work</a
 >\n\n[0:09:54] <a href="https://youtu.be/MBeSoig4DPY?t=594s">Two probabili
 stic questions</a>\n\n[0:10:22] <a href="https://youtu.be/MBeSoig4DPY?t=62
 2s">1. Probability of inflation</a>\n\n[0:11:03] <a href="https://youtu.be
 /MBeSoig4DPY?t=663s">2. Predictability problem</a>\n\n[0:14:27] <a href="h
 ttps://youtu.be/MBeSoig4DPY?t=867s">Infinite phase space</a>\n\n[0:16:01] 
 <a href="https://youtu.be/MBeSoig4DPY?t=961s">Probability formalisms</a>\n
 \n[0:19:20] <a href="https://youtu.be/MBeSoig4DPY?t=1160s">Paradox: fair i
 nfinite lottery</a>\n\n[0:20:56] <a href="https://youtu.be/MBeSoig4DPY?t=1
 256s">Standard probability theory</a>\n\n[0:23:07] <a href="https://youtu.
 be/MBeSoig4DPY?t=1387s">Paradox: fair lottery on N</a>\n\n[0:26:40] <a hre
 f="https://youtu.be/MBeSoig4DPY?t=1600s">Finitely additive probability</a>
 \n\n[0:33:00] <a href="https://youtu.be/MBeSoig4DPY?t=1980s">Non-Archimede
 an probability</a>\n\n[0:41:10] <a href="https://youtu.be/MBeSoig4DPY?t=24
 70s">Non-normal quasi-probability</a>\n\n[0:45:27] <a href="https://youtu.
 be/MBeSoig4DPY?t=2727s">Infinite lottery logic (ILL)</a>\n\n[0:47:53] <a h
 ref="https://youtu.be/MBeSoig4DPY?t=2873s">Implications for inflation theo
 ry?</a>\n\n[1:02:05] <a href="https://youtu.be/MBeSoig4DPY?t=3725s">Where 
 to next?</a>\n\n[1:08:27] <a href="https://youtu.be/MBeSoig4DPY?t=4107s">W
 hat current work in cosmology is particularly underappreciated by the comm
 unity?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/79/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Andreu Font-Ribera\, Seshadri Nadathur (IFAE\, U of Portsmouth)
DTSTART:20240404T050000Z
DTEND:20240404T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/80
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/80/">DESI 2024 - Cosmological Constraints from BAO (Font-Ribera and Nad
 athur)</a>\nby Andreu Font-Ribera\, Seshadri Nadathur (IFAE\, U of Portsmo
 uth) as part of Cosmology Talks\n\n\nAbstract\nThe Dark Energy Spectroscop
 ic Instrument (DESI) has produced cosmological constraints! And it is livi
 ng up to its name.\n\nTwo researchers from DESI\, Seshadri Nadathur and An
 dreu Font-Ribera\, tell us about DESI's measurements of the Baryon Acousti
 c Oscillations (BAO) released today. These results use one full year of DE
 SI data and are the first cosmological constraints from the telescope that
  have been released.\n\nMostly\, it is what you might expect: tighter cons
 traints. However\, in the realm of the equation of state of dark energy\, 
 they find\, even with BAO alone\, that there is a hint of evidence for evo
 lving dark energy. When they combine their data with CMB and Supernovae\, 
 who both also find small hints of evolving dark energy on their own\, the 
 evidence for dark energy not being a cosmological constant jumps as high a
 s 3.9σ with one combination of the datasets.\n\nIt seems there still is "
 concordance cosmology"\, it's just not ΛCDM for these datasets.\n\nThe fa
 ct that all three probes are tentatively favouring this is intriguing\, as
  it makes it unlikely to be due to systematic errors in one measurement pi
 peline.\n\nWatch this space for updates!\n\nVideo recording: <a href="http
 s://youtu.be/9DsMphPfrjI">youtu.be/9DsMphPfrjI</a>\n\nThe papers: <a href=
 "https://data.desi.lbl.gov/doc/papers/">data.desi.lbl.gov/doc/papers/</a>\
 n\narXiv:  <a href="https://arxiv.org/abs/2404.03000">2404.03000</a>\, <a 
 href="https://arxiv.org/abs/2404.03001">2404.03001</a>\, <a href="https://
 arxiv.org/abs/2404.03002">2404.03002</a>\n\nDESI: <a href="https://www.des
 i.lbl.gov/">desi.lbl.gov/</a>\n\nAndreu: <a href="https://andreufont.githu
 b.io/">andreufont.github.io/</a>\n\nSesh: <a href="https://seshnadathur.gi
 thub.io/">seshnadathur.github.io/</a>\n\n<hr>\n\n<b>Index to Key Parts of 
 the Talk</b>\n\n[0:00:00] <a href="https://youtu.be/9DsMphPfrjI?t=0s">Shau
 n's intro</a>\n\n[0:00:36] <a href="https://youtu.be/9DsMphPfrjI?t=36s">Op
 ening overview and quick peak of results by Andreu and Sesh</a>\n\n[0:01:3
 7] <a href="https://youtu.be/9DsMphPfrjI?t=97s">BAO results from DESI DR1<
 /a>\n\n[0:02:14] <a href="https://youtu.be/9DsMphPfrjI?t=134s">DESI BAO an
 d Dark Energy</a>\n\n[0:04:54] <a href="https://youtu.be/9DsMphPfrjI?t=294
 s">DESI BAO and neutrino masses</a>\n\n[0:05:18] <a href="https://youtu.be
 /9DsMphPfrjI?t=318s">DESI BAO and the Hubble Tension</a>\n\n[0:06:31] <a h
 ref="https://youtu.be/9DsMphPfrjI?t=391s">Main talk: background\, details\
 , results (starting with BAO)</a>\n\n[0:09:43] <a href="https://youtu.be/9
 DsMphPfrjI?t=583s">DESI: the instrument</a>\n\n[0:11:05] <a href="https://
 youtu.be/9DsMphPfrjI?t=665s">DESI: the survey</a>\n\n[0:12:04] <a href="ht
 tps://youtu.be/9DsMphPfrjI?t=724s">DESI Data Release 1 (DR1)</a>\n\n[0:18:
 11] <a href="https://youtu.be/9DsMphPfrjI?t=1091s">BAO measurements with g
 alaxies & quasars at z<2</a>\n\n[0:21:32] <a href="https://youtu.be/9DsMph
 PfrjI?t=1292s">Non-linear evolution and Density field reconstruction</a>\n
 \n[0:23:41] <a href="https://youtu.be/9DsMphPfrjI?t=1421s">How is the DESI
  BAO analysis different?</a>\n\n[0:30:08] <a href="https://youtu.be/9DsMph
 PfrjI?t=1808s">Tests of systematic errors</a>\n\n[0:34:02] <a href="https:
 //youtu.be/9DsMphPfrjI?t=2042s">Unblinded data results!</a>\n\n[0:39:16] <
 a href="https://youtu.be/9DsMphPfrjI?t=2356s">BAO measurements from the Ly
 man-α forest at z>2</a>\n\n[0:45:16] <a href="https://youtu.be/9DsMphPfrj
 I?t=2716s">Lyα BAO: Analysis Validation</a>\n\n[0:48:41] <a href="https:/
 /youtu.be/9DsMphPfrjI?t=2921s">Lyα BAO: Unblinding!</a>\n\n[0:51:10] <a h
 ref="https://youtu.be/9DsMphPfrjI?t=3070s">DESI DR1 Lyα BAO: Publications
 </a>\n\n[0:53:42] <a href="https://youtu.be/9DsMphPfrjI?t=3222s">Cosmologi
 cal Constraints: Flat ΛCDM from DESI BAO</a>\n\n[0:58:02] <a href="https:
 //youtu.be/9DsMphPfrjI?t=3482s">Breaking the H_0-r_d degeneracy</a>\n\n[1:
 01:35] <a href="https://youtu.be/9DsMphPfrjI?t=3695s">DESI BAO and the Hub
 ble Tension</a>\n\n[1:03:54] <a href="https://youtu.be/9DsMphPfrjI?t=3834s
 ">DESI BAO and neutrino masses</a>\n\n[1:10:52] <a href="https://youtu.be/
 9DsMphPfrjI?t=4252s">DESI BAO and Dark Energy</a>\n\n[1:23:06] <a href="ht
 tps://youtu.be/9DsMphPfrjI?t=4986s">Summary</a>\n\n[1:24:00] <a href="http
 s://youtu.be/9DsMphPfrjI?t=5040s">What's next?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/80/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Russell Boey\, Richard Easther\, Yourong Frank Wang (University of
  Auckland)
DTSTART:20240411T060000Z
DTEND:20240411T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/81
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/81/">Black Holes in Ultralight Dark Matter - Slowed Down and Sped Up?</
 a>\nby Russell Boey\, Richard Easther\, Yourong Frank Wang (University of 
 Auckland) as part of Cosmology Talks\n\n\nAbstract\nRussell Boey\, along w
 ith his coauthors Richard Easther and Yourong Wang\, tells us about his si
 mulations of a supermassive blackhole travelling through an ultralight dar
 k matter soliton. In particular\, he has studied the dynamical friction ef
 fect on the blackhole within the soliton. \n\nThis is especially interesti
 ng in the context of the "final parsec" problem\, where the orbits of supe
 rmassive blackhole binary systems stall in their decay as they reach one p
 arsec separation. Maybe a different background\, in the form of ULDM inste
 ad of WIMP DM\, could help?\n\nAn ultralight dark matter soliton is much m
 ore dense than expectations from "ordinary" WIMP-like dark matter\, so it 
 is also expected that the dynamical friction in such a soliton should be l
 arge. This is indeed what Russell\, Richard and Yourong found (and other c
 oauthor Emily Kendall who isn't present in the video). However\, curiously
 \, they also found a secondary effect where the blackhole perturbs the sol
 iton\, which in turn causes the soliton to backreact on the blackhole and 
 sometimes speed it back up.\n\nThere is definitely interesting physics to 
 explore inside galaxies in ultralight dark matter systems\, but no verdict
  just yet on whether the final parsec has been overcome or not.\n\nTalk re
 cording: https://www.youtube.com/watch?v=hyf6VtbZ6-c\n\nRussell: https://p
 rofiles.auckland.ac.nz/russell-boey\n\nRichard: https://profiles.auckland.
 ac.nz/r-easther/about\n\nYourong: https://fwphys.com/\n\nThe paper: https:
 //arxiv.org/abs/2403.09038\n\nThe earlier paper: https://arxiv.org/abs/211
 0.03428\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b>\n\n[00:00] <a hre
 f="https://youtu.be/hyf6VtbZ6-c?t=0s">Shaun's intro</a>\n\n[01:14] <a href
 ="https://youtu.be/hyf6VtbZ6-c?t=74s">Opening remarks by Russell</a>\n\n[0
 2:02] <a href="https://youtu.be/hyf6VtbZ6-c?t=122s">Two things to remember
  about this talk</a>\n\n[04:08] <a href="https://youtu.be/hyf6VtbZ6-c?t=24
 8s">Motivation for this work (The Final Parsec Problem)</a>\n\n[06:49] <a 
 href="https://youtu.be/hyf6VtbZ6-c?t=409s">Ultralight Dark Matter</a>\n\n[
 09:07] <a href="https://youtu.be/hyf6VtbZ6-c?t=547s">Objective</a>\n\n[12:
 10] <a href="https://youtu.be/hyf6VtbZ6-c?t=730s">Explaining use of the Sc
 hrodinger-Poisson equations</a>\n\n[13:44] <a href="https://youtu.be/hyf6V
 tbZ6-c?t=824s">Getting into the details - Setup</a>\n\n[17:14] <a href="ht
 tps://youtu.be/hyf6VtbZ6-c?t=1034s">Dynamical Friction Theory</a>\n\n[22:2
 4] <a href="https://youtu.be/hyf6VtbZ6-c?t=1344s">Semi-Analytic Model</a>\
 n\n[25:28] <a href="https://youtu.be/hyf6VtbZ6-c?t=1528s">Simulation Behav
 ior</a>\n\n[30:01] <a href="https://youtu.be/hyf6VtbZ6-c?t=1801s">Numerica
 l Dependencies</a>\n\n[33:19] <a href="https://youtu.be/hyf6VtbZ6-c?t=1999
 s">Black Hole Mass Dependence</a>\n\n[34:46] <a href="https://youtu.be/hyf
 6VtbZ6-c?t=2086s">ULDM Mass Dependence</a>\n\n[36:38] <a href="https://you
 tu.be/hyf6VtbZ6-c?t=2198s">Soliton Mass Dependence</a>\n\n[38:22] <a href=
 "https://youtu.be/hyf6VtbZ6-c?t=2302s">Semi Analytic Model Comparison</a>\
 n\n[40:51] <a href="https://youtu.be/hyf6VtbZ6-c?t=2451s">Overdensities</a
 >\n\n[43:12] <a href="https://youtu.be/hyf6VtbZ6-c?t=2592s">Force Comparis
 on</a>\n\n[45:40] <a href="https://youtu.be/hyf6VtbZ6-c?t=2740s">Conclusio
 n</a>\n\n[51:48] <a href="https://youtu.be/hyf6VtbZ6-c?t=3108s">What next?
 </a>\n\n[56:34] <a href="https://youtu.be/hyf6VtbZ6-c?t=3394s">What curren
 t work in cosmology is interesting but underappreciated by the community?<
 /a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/81/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Minh Nguyen\, Beatriz Tucci (University of Michigan\, Max-Planck-I
 nstitut für Astrophysik)
DTSTART:20240503T060000Z
DTEND:20240503T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/82
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/82/">Field Level Inference - Up to 5 sigma Better than Power and Bispec
 trum!</a>\nby Minh Nguyen\, Beatriz Tucci (University of Michigan\, Max-Pl
 anck-Institut für Astrophysik) as part of Cosmology Talks\n\n\nAbstract\n
 Nhat-Minh Nguyen and Beatrice Tucci tell us about their recent work compar
 ing the performance of field inference (FLI) and simulation based inferenc
 e (SBI). In an apples to apples comparison\, they find that FLI comfortabl
 y outperforms SBI\, even in what is essentially the "best case scenario" f
 or SBI.\n\nField level inference gives up on using "summary statistics" to
  construct a cosmological likelihood (e.g. the power spectrum\, the bispec
 trum\, the location of the BAO peak\, voids\, etc) and instead constructs 
 the cosmological likelihood at the level of the field itself. In other wor
 ds the likelihood step of a statistical analysis is done comparing the mea
 sured density field at each point in Fourier space to a model's actual den
 sity field. This means the set of model "parameters" necessarily also incl
 udes the entire set of Fourier modes of the initial conditions. Then\, for
  example\, when one would then talk about the "maximum likelihood" paramet
 ers in a FLI inference\, one is talking also about the maximum likelihood 
 set of initial conditions.\n\nOne then does the rest of the statistical an
 alysis more or less the same as if one is analysing a measured power spect
 rum\, e.g. one has priors on the inferred parameters\, one has the likelih
 ood function\, and one produces posterior probability distributions for al
 l of the model parameters.\n\nIn this analysis they fixed all cosmological
  parameters except the overall amplitude of the initial density fluctuatio
 ns\, via σ8. This means they also restricted the set of initial density f
 luctuations to those with a certain spectral index\, but varied over all s
 ets of initial density fluctuations that do produce this spectral index. T
 hey then evolve the initial conditions forward in time using the LEFTfield
  framework and do the FLI analysis on the evolved field.<!--more-->\n\nSBI
  however still uses summary statistics\, in this case the power spectrum a
 nd bispectrum\, but uses simulations to construct the likelihood\, rather 
 than making model based assumptions for what these statistics should look 
 like.\n\nIn this analysis they are only comparing the performance of FLI a
 nd SBI at reconstructing the parameters of simulations\, because the obser
 ved data in e.g. BOSS or DESI is only well-calibrated at the level of the 
 power spectrum (and maybe the bispectrum?)\, but not the full non-linear d
 ensity field that FLI can probe - and where its true improvements lie.\n\n
 However\, they find FLI outperforms SBI with error bars substantially smal
 ler (by factors of 2-5 depending on the scales and simulations considered)
 . This shows that if we could perform field level inference on current or 
 future data sets\, the level of constraints we could obtain would also be 
 substantially improved (e.g\, maybe even a 1σ deviation would become a 5
 σ detection!?)\n\nRecorded Talk Video: <a href="https://www.youtube.com/w
 atch?v=Pxfsf89jZwI">youtu.be/Pxfsf89jZwI</a>\n\nMinh: <a href="https://min
 hmpa.github.io/">minhmpa.github.io/</a>\n\nBeatriz: <a href="https://wwwmp
 a.mpa-garching.mpg.de/~tucci/">wwwmpa.mpa-garching.mpg.de/~tucci/</a>\n\nP
 aper: <a href="https://arxiv.org/abs/2403.03220">arXiv:2403.03220</a>\n\n<
 hr>\n\n<b>Index to Key Parts of the Talk</b>\n\n[00:00] <a href="https://y
 outu.be/Pxfsf89jZwI?t=0s">Shaun's intro</a>\n\n[01:20] <a href="https://yo
 utu.be/Pxfsf89jZwI?t=80s">Opening remarks by Minh and Beatriz</a>\n\n[02:3
 9] <a href="https://youtu.be/Pxfsf89jZwI?t=159s">Takeaways to remember abo
 ut this talk</a>\n\n[05:48] <a href="https://youtu.be/Pxfsf89jZwI?t=348s">
 Motivation for this work</a>\n\n[08:45] <a href="https://youtu.be/Pxfsf89j
 ZwI?t=525s">Getting into the details: Amplitude of Structure Growth</a>\n\
 n[09:52] <a href="https://youtu.be/Pxfsf89jZwI?t=591s">Galaxy clustering c
 an distinguish scenarios of new physics</a>\n\n[10:49] <a href="https://yo
 utu.be/Pxfsf89jZwI?t=649s">Galaxy bias - response of galaxy formation to f
 luctuations</a>\n\n[11:47] <a href="https://youtu.be/Pxfsf89jZwI?t=707s">G
 alaxy bias spoils constraint from galaxy clustering</a>\n\n[12:30] <a href
 ="https://youtu.be/Pxfsf89jZwI?t=750s">Effective Field Theory of galaxy bi
 as</a>\n\n[15:45] <a href="https://youtu.be/Pxfsf89jZwI?t=945s">FBI (field
 -level Bayesian inference) and SBI (simulation-based inference) posteriors
 </a>\n\n[18:46] <a href="https://youtu.be/Pxfsf89jZwI?t=1126s">Extended di
 scussion at the Field-Level Inference slide</a>\n\n[29:17] <a href="https:
 //youtu.be/Pxfsf89jZwI?t=1757s">Apple-to-apple comparison of FBI and SBI P
 +B</a>\n\n[31:12] <a href="https://youtu.be/Pxfsf89jZwI?t=1872s">Simulatio
 n-based inference</a>\n\n[33:06] <a href="https://youtu.be/Pxfsf89jZwI?t=1
 986s">Neural Posterior Estimation (NPE)</a>\n\n[34:35] <a href="https://yo
 utu.be/Pxfsf89jZwI?t=2065s">Normalizing flows</a>\n\n[35:37] <a href="http
 s://youtu.be/Pxfsf89jZwI?t=2137s">SBI wrap-up putting it all together</a>\
 n\n[40:37] <a href="https://youtu.be/Pxfsf89jZwI?t=2437s">Improvement incr
 eases with scale cuts</a>\n\n[43:02] <a href="https://youtu.be/Pxfsf89jZwI
 ?t=2582s">Robust improvement across samples</a>\n\n[44:50] <a href="https:
 //youtu.be/Pxfsf89jZwI?t=2690s">Where to next?</a>\n\n[49:30] <a href="htt
 ps://youtu.be/Pxfsf89jZwI?t=2970s">What current work in cosmology is inter
 esting but underappreciated by the community?</a>\n\n[50:24] <a href="http
 s://youtu.be/Pxfsf89jZwI?t=3024s">Beyond 2-point mock data challenge</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/82/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Mark Fromhold\, Lucia Hackermuller (University of Nottingham)
DTSTART:20240523T060000Z
DTEND:20240523T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/83
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/83/">Fundamental Cosmology from the Lab</a>\nby Mark Fromhold\, Lucia H
 ackermuller (University of Nottingham) as part of Cosmology Talks\n\n\nAbs
 tract\nMark Fromhold and Lucia Hackermuller tell us about how they are 3D 
 printing atom traps that allow them to cool atoms to a few micro Kelvin. T
 his is super interesting for cosmology because it would allow them\, among
  many other things\, to potentially trap dark domain walls. We learned in 
 another recent cosmology talk about the physics behind these dark domain w
 alls\, now here is the physics behind the cold atom trap.\n\nIn principle 
 these traps may one day measure the gravitational effects of quantum objec
 ts\, ultimately testing whether space-time curvature can be in a quantum s
 uperposition or not.\n\nTalk video: https://youtu.be/1XAbMkoQeXg\n\nLucia:
  https://www.nottingham.ac.uk/physics/people/lucia.hackermuller\n\nMark: h
 ttps://www.nottingham.ac.uk/physics/people/mark.fromhold\n\nDark Domain Wa
 lls: https://arxiv.org/abs/2308.01179\n\n<hr>\n<b>Index to Key Parts of th
 e Talk</b>\n\n[00:00] <a href="https://youtu.be/1XAbMkoQeXg?t=0s">Shaun's 
 intro</a>\n\n[01:04] <a href="https://youtu.be/1XAbMkoQeXg?t=64s">Opening 
 remarks by Lucia and Mark</a>\n\n[04:47] <a href="https://youtu.be/1XAbMko
 QeXg?t=287s">Timing & enabling investments in Quantum 2.0 technologies</a>
 \n\n[09:18] <a href="https://youtu.be/1XAbMkoQeXg?t=558s">How are atoms co
 oled to <1 millionth degree above absolute zero?</a>\n\n[15:50] <a href="h
 ttps://youtu.be/1XAbMkoQeXg?t=950s">Ultracold atoms\, setup in the lab\, l
 aser system</a>\n\n[20:12] <a href="https://youtu.be/1XAbMkoQeXg?t=1212s">
 Movie - Lithium MOT</a>\n\n[21:05] <a href="https://youtu.be/1XAbMkoQeXg?t
 =1265s">Evaporative cooling - Lithium</a>\n\n[26:02] <a href="https://yout
 u.be/1XAbMkoQeXg?t=1562s">Li_2 Bose-Einstein Condensate</a>\n\n[27:47] <a 
 href="https://youtu.be/1XAbMkoQeXg?t=1667s">Quantum 2.0 sensors</a>\n\n[32
 :15] <a href="https://youtu.be/1XAbMkoQeXg?t=1935s">3D printed chambers</a
 >\n\n[34:23] <a href="https://youtu.be/1XAbMkoQeXg?t=2063s">Printed surfac
 es</a>\n\n[35:17] <a href="https://youtu.be/1XAbMkoQeXg?t=2117s">Parts for
  Quantum 2.0 technologies\; New manufacturing techniques</a>\n\n[37:53] <a
  href="https://youtu.be/1XAbMkoQeXg?t=2273s">New hybrid shielding/magnetic
  bias product</a>\n\n[39:34] <a href="https://youtu.be/1XAbMkoQeXg?t=2374s
 ">Printed vapour cells</a>\n\n[41:34] <a href="https://youtu.be/1XAbMkoQeX
 g?t=2494s">Spectroscopy and magnetic sensors</a>\n\n[42:36] <a href="https
 ://youtu.be/1XAbMkoQeXg?t=2556s">Compact\, printed Laser system</a>\n\n[44
 :22] <a href="https://youtu.be/1XAbMkoQeXg?t=2662s">A printed gravimeter f
 or space</a>\n\n[46:16] <a href="https://youtu.be/1XAbMkoQeXg?t=2776s">Pri
 nted cold atom system</a>\n\n[49:35] <a href="https://youtu.be/1XAbMkoQeXg
 ?t=2975s">Where to next?</a>\n\n[53:42] <a href="https://youtu.be/1XAbMkoQ
 eXg?t=3222s">Other ideas on the horizon?</a>\n\n[58:02] <a href="https://y
 outu.be/1XAbMkoQeXg?t=3482s">What current work in cold atoms is interestin
 g but underappreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/83/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Elisabeth Krause++ (University of Arizona)
DTSTART:20240606T060000Z
DTEND:20240606T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/84
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/84/">The Parameter Masked Mock Data Challenge for Beyond 2-Pt Statistic
 s - Results\, Lessons & Reflections</a>\nby Elisabeth Krause++ (University
  of Arizona) as part of Cosmology Talks\n\n\nAbstract\n1-1/2 hour discussi
 on with Shaun Hotchkiss and 9 members of The Beyond-2pt Collaboration: Eli
 sabeth Krause\, Marcos Pellejero-Ibanez\, Andres Salcedo\, Minh Nguyen\, M
 ikhail Ivanov\, Enrique Paillas\, Carolina Cuesta-Lazaro\, Chirag Modi\, G
 iovanni Verza\n\nOne-sentence summary of the work by Minh Nguyen: "how cos
 mology and galaxy survey analyses can move beyond the canonical 2-point co
 rrelation function"\n\nRecorded video: <a href="https://youtu.be/LPykO2206
 OY">youtu.be/LPykO2206OY</a>\n\nPaper: <a href="https://arxiv.org/abs/2405
 .02252">arXiv:2405.02252</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk<
 /b>\n\n[0:00:00] <a href="https://youtu.be/LPykO2206OY?t=0s">Shaun's intro
 </a>\n\n[0:02:05] <a href="https://youtu.be/LPykO2206OY?t=125s">Opening co
 mments by Elisabeth Krause</a>\n\n[0:03:13] <a href="https://youtu.be/LPyk
 O2206OY?t=193s">Two things to remember about this talk</a>\n\n[0:04:56] <a
  href="https://youtu.be/LPykO2206OY?t=296s">The history of this idea</a>\n
 \n[0:06:19] <a href="https://youtu.be/LPykO2206OY?t=379s">Why the team use
 d this approach</a>\n\n[0:08:43] <a href="https://youtu.be/LPykO2206OY?t=5
 23s">Getting into the details</a>\n\n[0:13:31] <a href="https://youtu.be/L
 PykO2206OY?t=811s">Redshift-space results in σ8 and Ωm (Figs. 21\, 1 in 
 paper)</a>\n\n[0:18:10] <a href="https://youtu.be/LPykO2206OY?t=1090s">Lig
 ht-cone and Real-space Results (Figs 3\, 4)</a>\n\n[0:19:28] <a href="http
 s://youtu.be/LPykO2206OY?t=1168s">Takeaways</a>\n\n[0:22:53] <a href="http
 s://youtu.be/LPykO2206OY?t=1373s">The Methods and How They Work: Participa
 ting Analyses (Table 1)</a>\n\n[0:24:14] <a href="https://youtu.be/LPykO22
 06OY?t=1454s">Importance of k_max</a>\n\n[0:27:18] <a href="https://youtu.
 be/LPykO2206OY?t=1638s">Overview of EFT Methods</a>\n\n[0:35:47] <a href="
 https://youtu.be/LPykO2206OY?t=2147s">Overview of HOD Methods</a>\n\n[0:41
 :43] <a href="https://youtu.be/LPykO2206OY?t=2503s">2-min overviews of eac
 h specific method</a>\n\n[0:55:50] <a href="https://youtu.be/LPykO2206OY?t
 =3350s">Post unmasking insights and updated results</a>\n\n[1:04:49] <a hr
 ef="https://youtu.be/LPykO2206OY?t=3889s">Lessons learned and future refle
 ctions</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/84/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Tamara Davis\, Maria Vincenzi\, Dillon Brout (DES Collaboration)
DTSTART:20240610T060000Z
DTEND:20240610T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/85
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/85/">The Dark Energy Survey Supernova Program - Data and Cosmology</a>\
 nby Tamara Davis\, Maria Vincenzi\, Dillon Brout (DES Collaboration) as pa
 rt of Cosmology Talks\n\n\nAbstract\nTamara Davis\, Maria Vincenzi and Dil
 lon Brout tell us about the Dark Energy Survey's (DES) new supernova catal
 ogue. The catalogue has more than 1500 new supernovae\, and will allow a v
 ast range of new cosmology constraints. It is a factor of around five larg
 er than the next largest high redshift supernovae catalogue.\n\nVery curio
 usly\, DES' supernovae see hints of evolving dark energy. This is especial
 ly curious given that a few months after DES released this data\, the Dark
  Energy Spectroscopic Instrument (DESI) also released data with similar hi
 nts.\n\nTamara: <a href="https://smp.uq.edu.au/profile/186/tamara-davis">s
 mp.uq.edu.au - tamara-davis</a>\n\nMaria: <a href="https://www.linkedin.co
 m/in/maria-vincenzi-45a739150/">linkedin - maria-vincenzi</a>\n\nDillon: <
 a href="https://djbrout.github.io/">djbrout.github.io</a>\n\nKey cosmology
  paper: <a href="https://arxiv.org/abs/2401.02929">arXiv: 2401.02929</a>\n
 \nCosmological Analysis and Systematic Uncertainties: <a href="https://arx
 iv.org/abs/2401.02945">arXiv: 2401.02945</a>\n\nLight curves and 5-Year da
 ta release: <a href="https://arxiv.org/abs/2406.05046">arXiv: 2406.05046</
 a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b>\n\n[0:00:00] <a href="
 https://youtu.be/y9ocwGJnGwk?t=0s">Shaun's intro</a>\n\n[0:01:11] <a href=
 "https://youtu.be/y9ocwGJnGwk?t=71">Intro by the 3 speakers to this work</
 a>\n\n[0:02:43] <a href="https://youtu.be/y9ocwGJnGwk?t=163">Two takeaways
  to remember</a>\n\n[0:05:54] <a href="https://www.youtube.com/watch?v=y9o
 cwGJnGwk&t=354s">Supernova cosmology basics</a>\n\n[0:29:47] <a href="http
 s://youtu.be/y9ocwGJnGwk?t=1787">DES Analysis Details</a>\n\n[0:48:10] <a 
 href="https://youtu.be/y9ocwGJnGwk?t=2890">DES SN Cosmology Results</a>\n\
 n[1:00:09] <a href="https://youtu.be/y9ocwGJnGwk?t=3609">Is dark energy a 
 cosmological constant?</a> \n\n[1:01:22] <a href="https://youtu.be/y9ocwGJ
 nGwk?t=3682">A few months later...DESI supports DES\, finding similar resu
 lt for w<sub>a</sub></a>\n\n[1:02:39] <a href="https://youtu.be/y9ocwGJnGw
 k?t=3759">Big Questions: Is the expansion of the Universe accelerating? Ye
 s!</a> \n\n[1:03:35] <a href="https://youtu.be/y9ocwGJnGwk?t=3815">Big Que
 stions: Is dark energy a cosmological constant? Maybe? Union 3 also prefer
  w > -1</a>\n\n[1:10:23] <a href="https://youtu.be/y9ocwGJnGwk?t=4223">Big
  Questions: How old is the Universe?  Slightly younger than we thought?</a
 >\n\n[1:11:12] <a href="https://youtu.be/y9ocwGJnGwk?t=4272">Big Questions
 : Does DES best fit resolve Hubble tension? No\, DES doesn't constrain H<s
 ub>0</sub></a>\n\n[1:12:04] <a href="https://youtu.be/y9ocwGJnGwk?t=4324">
 Bonus Science!!!</a>\n\n[1:16:08] <a href="https://youtu.be/y9ocwGJnGwk?t=
 4568">Cosmology work interesting but underappreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/85/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Ryan Camilleri\, Tamara Davis (DES Collaboration\, University of Q
 ueensland)
DTSTART:20240611T060000Z
DTEND:20240611T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/86
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/86/">DES Supernovae - H0 From the Inverse Distance Ladder Without ΛCDM
 </a>\nby Ryan Camilleri\, Tamara Davis (DES Collaboration\, University of 
 Queensland) as part of Cosmology Talks\n\n\nAbstract\nRyan Camilleri and T
 amara Davis tell us about how they have used the Dark Energy Survey's Year
  5 supernovae catalogue\, anchored to the Dark Energy Spectroscopic Instru
 ment's Baryon Acoustic Oscillations\, to create an "inverse distance ladde
 r".\n\nWith this they are able to determine the Hubble Parameter\, at reds
 hift zero with a high accuracy\, without needing to assume ΛCDM. The resu
 lts still match Planck\, meaning that the high redshift to low redshift ma
 tching appears to still not work out\, even outside of ΛCDM.\n\nThe impli
 cations are large for any attempts to go beyond ΛCDM to solve the Hubble 
 tension as it appears the z=2 to z=0.05 window is not the right window for
  finding the solution.\n\nVideo recording: <a href="https://youtu.be/kzT0t
 WWggRo">youtu.be/kzT0tWWggRo</a>\n\nPaper: <a href="https://arxiv.org/abs/
 2406.05049">arXiv: 2406.05049</a>\n\nRyan: <a href="https://smp.uq.edu.au/
 profile/13102/ryan-camilleri">smp.uq.edu.au/profile/13102/ryan-camilleri</
 a>\n\nTamara: <a href="https://smp.uq.edu.au/profile/186/tamara-davis">smp
 .uq.edu.au/profile/186/tamara-davis</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/86/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Ryan Camilleri\, Tamara Davis (DES Collaboration\, University of Q
 ueensland)
DTSTART:20240612T060000Z
DTEND:20240612T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/87
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/87/">DES Supernovae - Beyond ΛCDM</a>\nby Ryan Camilleri\, Tamara Davi
 s (DES Collaboration\, University of Queensland) as part of Cosmology Talk
 s\n\n\nAbstract\nRyan Camilleri and Tamara Davis tell us about how they ha
 ve examined models beyond ΛCDM using the Dark Energy Survey's wonderful s
 upernova catalogue. Tantalisingly\, they find that a number of models are 
 "moderately preferred" over ΛCDM (in model comparison speak).\n\nThey als
 o\, very admirably\, check whether crucial aspects of the DES pipeline are
  model dependent or not. They find that\, so long as the reference model i
 s close-ish to the true model then the pipeline is accurate. "Close-ish" i
 s very generous here as well\, as they even found in simulations that when
  one processed the data with models 10σ from the truth\, the subsequent p
 arameter constraints were still within 1σ of the truth. The moral of this
  is that\, even though the supernovae were processed assuming ΛCDM\, so l
 ong as the true cosmology isn't too far from ΛCDM then this doesn't matte
 r.\n\nThis means\, if you have your own model that they haven't tested\, y
 ou don't need to simulate the entire DES analysis pipeline to analysis you
 r model\, you can do your model comparison at the level of the Hubble diag
 ram. Nice!\n\nTalk video: <a href="https://youtu.be/NLXxX-Z2OfM">youtu.be/
 NLXxX-Z2OfM</a>\n\nPaper: <a href="https://arxiv.org/abs/2406.05048">arXiv
 : 2406.05048</a>\n\nRyan: <a href="https://smp.uq.edu.au/profile/13102/rya
 n-camilleri">smp.uq.edu.au/profile/13102/ryan-camilleri</a>\n\nTamara: <a 
 href="https://smp.uq.edu.au/profile/186/tamara-davis">smp.uq.edu.au/profil
 e/186/tamara-davis</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b>\n\
 n[00:00] <a href="https://youtu.be/NLXxX-Z2OfM?t=0s">Shaun's intro</a>\n\n
 [01:41] <a href="https://youtu.be/NLXxX-Z2OfM?t=101s">Opening comments by 
 Ryan</a>\n\n[02:20] <a href="https://youtu.be/NLXxX-Z2OfM?t=140s">Two take
 aways to remember</a>\n\n[03:06] <a href="https://youtu.be/NLXxX-Z2OfM?t=1
 86s">Motivation for this work\, starting with ΛCDM overview</a>\n\n[05:01
 ] <a href="https://youtu.be/NLXxX-Z2OfM?t=301s">So why go beyond ΛCDM?</a
 >\n\n[06:13] <a href="https://youtu.be/NLXxX-Z2OfM?t=373s">What is beyond 
 ΛCDM? Testing different models</a>\n\n[07:18] <a href="https://youtu.be/N
 LXxX-Z2OfM?t=438s">Parametric forms of Λ</a>\n\n[09:28] <a href="https://
 youtu.be/NLXxX-Z2OfM?t=568s">Dvali-Gabadadze-Porrati (DBP) models</a>\n\n[
 10:04] <a href="https://youtu.be/NLXxX-Z2OfM?t=604s">Chaplygin Gas models<
 /a>\n\n[11:13] <a href="https://youtu.be/NLXxX-Z2OfM?t=673s">Timescape cos
 mology</a>\n\n[14:12] <a href="https://youtu.be/NLXxX-Z2OfM?t=852s">Why th
 ese models were tested vs other options?</a>\n\n[15:31] <a href="https://y
 outu.be/NLXxX-Z2OfM?t=931s">Observations -> Hubble Diagram</a>\n\n[16:08] 
 <a href="https://youtu.be/NLXxX-Z2OfM?t=968s">DES-SN5YR Pipeline</a>\n\n[2
 3:10] <a href="https://youtu.be/NLXxX-Z2OfM?t=1390s">The Omega\\_m - w deg
 eneracy\; intro of Q_H parameter</a>\n\n[25:21] <a href="https://youtu.be/
 NLXxX-Z2OfM?t=1521s">Model constraints</a>\n\n[29:43] <a href="https://you
 tu.be/NLXxX-Z2OfM?t=1783s">Model comparisons</a>\n\n[35:37] <a href="https
 ://youtu.be/NLXxX-Z2OfM?t=2137s">What's next?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/87/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Paul Shah\, Tamara Davis (DES Collaboration\, University College L
 ondon\, University of Queensland)
DTSTART:20240617T060000Z
DTEND:20240617T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/88
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/88/">DES Supernovae - Weak Lensing Magnification Detected at 6σ!</a>\n
 by Paul Shah\, Tamara Davis (DES Collaboration\, University College London
 \, University of Queensland) as part of Cosmology Talks\n\n\nAbstract\nPau
 l Shah and Tamara Davis tell us about how they have used this wonderful su
 pernova catalogue from the Dark Energy Survey to detect the weak lensing m
 agnification signal for the first time. There has been evidence of this si
 gnal in earlier catalogues\, but at no bigger than 1.4σ. They've got it a
 t 6σ!\n\nThey do this by correlating the scatter in the magnitude of the 
 supernovae with the over-under density in galaxy catalogues along the same
  lines of sight of the supernovae. Where there is more matter\, the light 
 from the supernova should be magnified\, and where there is less matter it
  should be de-maginified. And they do indeed see that along overdense line
 s of sight the supernovae are\, on average\, ever so slightly brighter\, a
 nd on underdense lines of sight the are ever so slightly dimmer.\n\nI can'
 t wait to see how this observable is used in the future to constrain all s
 orts of bits of cosmology. Nice work everyone!\n\nTalk Video: <a href="htt
 ps://youtu.be/YljnmVZKukc">youtu.be/YljnmVZKukc</a>\n\nPaper: <a href="htt
 ps://arxiv.org/abs/2406.05047">arXiv: 2406.05047</a>\n\nPaul: <a href="htt
 ps://paulshah.github.io/">paulshah.github.io</a>\n\nTamara: <a href="https
 ://smp.uq.edu.au/profile/186/tamara-davis">smp.uq.edu.au/profile/186/tamar
 a-davis</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b>\n\n[00:00] <a
  href="https://youtu.be/YljnmVZKukc?t=0s">Shaun's intro</a>\n\n[01:20] <a 
 href="https://youtu.be/YljnmVZKukc?t=80s">Searching for gravitational lens
 ing of SNe</a>\n\n[04:24] <a href="https://youtu.be/YljnmVZKukc?t=264s">Tw
 o takeaways to remember</a>\n\n[05:43] <a href="https://youtu.be/YljnmVZKu
 kc?t=343s">Motivation for this work and why it could be done now</a>\n\n[1
 0:22] <a href="https://youtu.be/YljnmVZKukc?t=622s">The Hubble diagram of 
 SN Ia</a>\n\n[11:16] <a href="https://youtu.be/YljnmVZKukc?t=676s">What do
 es a clumpy universe do to SN Ia?</a>\n\n[13:37] <a href="https://youtu.be
 /YljnmVZKukc?t=817s">But can we detect it?</a>\n\n[14:46] <a href="https:/
 /youtu.be/YljnmVZKukc?t=886s">Our data</a>\n\n[16:37] <a href="https://you
 tu.be/YljnmVZKukc?t=997s">Our lensing estimator</a>\n\n[20:52] <a href="ht
 tps://youtu.be/YljnmVZKukc?t=1252s">Correlate lensing estimate with Hubble
  diagram residuals</a>\n\n[27:01] <a href="https://youtu.be/YljnmVZKukc?t=
 1621s">The shape of dark matter haloes</a>\n\n[27:43] <a href="https://you
 tu.be/YljnmVZKukc?t=1663s">'Adaptive optics' for dark matter</a>\n\n[30:49
 ] <a href="https://youtu.be/YljnmVZKukc?t=1849s">What's next?</a>\n\n[34:2
 3] <a href="https://youtu.be/YljnmVZKukc?t=2063s">Key results from DES-SN5
 YR weak lensing</a>\n\n[45:05] <a href="https://youtu.be/YljnmVZKukc?t=270
 5s">Further work anticipated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/88/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Ryan White\, Tamara Davis (DES Collaboration\, University of Queen
 sland)
DTSTART:20240619T060000Z
DTEND:20240619T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/89
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/89/">DES Supernovae - Precisely Measured Time Dilation from Universe's 
 Expansion</a>\nby Ryan White\, Tamara Davis (DES Collaboration\, Universit
 y of Queensland) as part of Cosmology Talks\n\n\nAbstract\nRyan White and 
 Tamara Davis from the Dark Energy Survey tell us about how they have measu
 red time dilation in distant supernovae. This time dilation is precisely w
 hat one would expect in an expanding universe. "Precisely" is the right wo
 rd too\, as they have measured this effect to 0.5% precision and they get 
 exactly the number predicted by an expanding universe.\n\nThere may be all
  sorts of tensions popping up for the standard cosmological model ΛCDM\, 
 but it seems the expanding universe itself is doing just fine.\n\nTalk vid
 eo: <a href="https://youtu.be/1vfo-JFc-Io">youtu.be/1vfo-JFc-Io</a>\n\nRya
 n: <a href="https://ryanwhite1.github.io/">ryanwhite1.github.io</a>\n\nTam
 ara: <a href="https://smp.uq.edu.au/profile/186/tamara-davis">smp.uq.edu.a
 u/profile/186/tamara-davis</a>\n\nThe paper: <a href="https://arxiv.org/ab
 s/2406.05050">arXiv: 2406.05050</a>\n\nThe paper with the \\Delta t = (1+z
 ) proof (in appendix A): <a href="https://arxiv.org/abs/0804.3595">arXiv: 
 0804.3595</a>\n\n<hr>\n\n<b>Index to Key Parts of the Talk</b>\n\n[00:00] 
 <a href="https://youtu.be/1vfo-JFc-Io?t=0s">Shaun's intro</a>\n\n[02:46] <
 a href="https://youtu.be/1vfo-JFc-Io?t=166s">Overview of this work by Ryan
  and Tamara</a>\n\n[06:08] <a href="https://youtu.be/1vfo-JFc-Io?t=368s">S
 upernova light curves in different bands across redshifts</a>\n\n[10:55] <
 a href="https://youtu.be/1vfo-JFc-Io?t=655s">Picking similar light curves 
 out of different bands</a>\n\n[11:23] <a href="https://youtu.be/1vfo-JFc-I
 o?t=683s">Stacked light curves</a>\n\n[13:55] <a href="https://youtu.be/1v
 fo-JFc-Io?t=835s">Scale light curves in time by function of source z</a>\n
 \n[18:02] <a href="https://youtu.be/1vfo-JFc-Io?t=1082s">The 'width' of ea
 ch individual light curve</a>\n\n[18:43] <a href="https://youtu.be/1vfo-JF
 c-Io?t=1123s">Quantifying time dilation</a>\n\n[21:44] <a href="https://yo
 utu.be/1vfo-JFc-Io?t=1304s">Why do we expect time dilation?</a>\n\n[27:58]
  <a href="https://youtu.be/1vfo-JFc-Io?t=1678s">Scatter in widths from noi
 se & intrinsic SN light curve variation</a>\n\n[38:00] <a href="https://yo
 utu.be/1vfo-JFc-Io?t=2280s">Where to next?</a>\n\n[40:56] <a href="https:/
 /youtu.be/1vfo-JFc-Io?t=2456s">What current cosmology work is interesting 
 but underappreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/89/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Wendy Freedman\, Barry Madore (Chicago Carnegie Hubble Program (CC
 HP))
DTSTART:20240816T060000Z
DTEND:20240816T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/90
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/90/">The Status of the Chicago-Carnegie Hubble Program (with JWST data)
 </a>\nby Wendy Freedman\, Barry Madore (Chicago Carnegie Hubble Program (C
 CHP)) as part of Cosmology Talks\n\n\nAbstract\nWendy Freedman and Barry M
 adore give a status update on the Chicago-Carnegie Hubble Program (CCHP). 
 There has been much progress!\n\nIn this status update there are three ind
 ependent distance ladder measurements of the expansion rate (i.e. the Hubb
 le parameter) all using JWST data. There is the very well-known Cepheid me
 thod\, the now also well known Tip of the Red Giant (TRGB) method\, and ma
 king its debut\, the J-Region Asymptotic Giant Branch (JAGB) method. \n\nT
 he TRGB and JAGB methods agree strikingly well and appear to be consistent
  with the CMB + ΛCDM value for the expansion rate. The Cepheid method als
 o agrees to within less than 5%\, which is still striking\, but there is s
 ome deviation.\n\nThe deviation pushes the Cepheid value for H0 up\, makin
 g it consistent with the SH0ES value\, although the error bars on this CCH
 P result are large enough that their Cepheid value is also consistent with
  the lower TRGB and JAGB methods. Most curiously (to this relative outside
 r) the JAGB value does not appear to be consistent with SH0ES\, even when 
 considering statistical and systematic errors at once. The striking consis
 tency between TRGB and JAGB\, means that one's naive guess might be that t
 here is some unknown systematic in the Cepheid method (in both the CCHP an
 d SH0ES measurements). However\, naive guesses are naive so\, time will te
 ll.<!--more-->\n\nTime really will tell as the ongoing JWST measurements w
 ill shrink both statistical and systematic errors in all methods\, so it w
 on't be long before the CCHP Cepheids are forced to take a side.\n\nVideo 
 recording: <a href="https://youtu.be/OkGUoKukwk8">youtu.be/OkGUoKukwk8</a>
 \n\nWendy: <a href="https://astro.uchicago.edu/people/wendy-l-freedman.php
 ">astro.uchicago.edu/people/wendy-l-freedman.php</a>\n\nBarry: <a href="ht
 tps://carnegiescience.edu/bio/dr-barry-madore-emeritus">carnegiescience.ed
 u/bio/dr-barry-madore-emeritus</a>\n\nPaper: <a href="https://arxiv.org/ab
 s/2408.06153">arXiv: 2408.06153</a>\n\n<hr>\n\n[0:00:00] <a href="https://
 youtu.be/OkGUoKukwk8?t=0s">Intro comments by Shaun and Wendy</a>\n\n[0:01:
 22] <a href="https://youtu.be/OkGUoKukwk8?t=82s">Two takeaways to remember
 </a>\n\n[0:01:47] <a href="https://youtu.be/OkGUoKukwk8?t=107s">Not seeing
  now *extraordinary evidence* for Hubble tension\; unknown systematics</a>
 \n\n[0:03:18] <a href="https://youtu.be/OkGUoKukwk8?t=198s">Background on 
 gold standard methods for measuring H0</a>\n\n[0:09:05] <a href="https://y
 outu.be/OkGUoKukwk8?t=545s">2 methods agree in their zero point\, low scat
 ter against each other</a>\n\n[0:09:35] <a href="https://youtu.be/OkGUoKuk
 wk8?t=575s">2 new papers on arXiv and recent CCHP group papers\; more comi
 ng</a>\n\n[0:11:58] <a href="https://youtu.be/OkGUoKukwk8?t=718s">First ta
 rget galaxies\; TRGB and JAGB advantages\; HST cf JWST</a>\n\n[0:20:54] <a
  href="https://youtu.be/OkGUoKukwk8?t=1254s">3 distances indicators - TRGB
 \, Cepheids\, JAGB</a>\n\n[0:29:14] <a href="https://youtu.be/OkGUoKukwk8?
 t=1754s">JAGB details</a>\n\n[0:31:29] <a href="https://youtu.be/OkGUoKukw
 k8?t=1889s">Data Analysis</a>\n\n[0:32:31] <a href="https://youtu.be/OkGUo
 Kukwk8?t=1951s">Comparison of distances (pre a determination of H0)</a>\n\
 n[0:36:09] <a href="https://youtu.be/OkGUoKukwk8?t=2169s">TRGB vs JAGB com
 parison</a>\n\n[0:38:22] <a href="https://youtu.be/OkGUoKukwk8?t=2302s">SN
  Calibrator M_B with Distance Modulus (potential systematic needs understa
 nding)</a>\n\n[0:42:02] <a href="https://youtu.be/OkGUoKukwk8?t=2522s">Car
 negie Supernova Project</a>\n\n[0:44:12] <a href="https://youtu.be/OkGUoKu
 kwk8?t=2652s">Summary of H0 Values and Statistical Uncertainties (Table 4 
 in paper)</a>\n\n[0:51:09] <a href="https://youtu.be/OkGUoKukwk8?t=3069s">
 Distribution of H0 Values for 3 JWST Methods( Fig. 11)</a>\n\n[0:52:45] <a
  href="https://youtu.be/OkGUoKukwk8?t=3165s">Distribution of H0 Values Wit
 h Total Errors (Fig. 12)</a>\n\n[0:53:21] <a href="https://youtu.be/OkGUoK
 ukwk8?t=3201s">CCHP JWST H0 Values (Fig. 20)</a>\n\n[0:58:38] <a href="htt
 ps://youtu.be/OkGUoKukwk8?t=3518s">Conclusions (TRGB\, JAGB agree at 1% le
 vel\; results consistent with Planck\, LCDM</a>\n\n[1:02:27] <a href="http
 s://youtu.be/OkGUoKukwk8?t=3747s">What might be cause of high H0 with Ceph
 eids?</a>\n\n[1:06:28] <a href="https://youtu.be/OkGUoKukwk8?t=3988s">What
  about the possibility of new physics?</a>\n\n[1:09:06] <a href="https://y
 outu.be/OkGUoKukwk8?t=4146s">What current work in cosmology is interesting
  but underappreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/90/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Abigail J. Lee (University of Chicago)
DTSTART:20240822T060000Z
DTEND:20240822T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/91
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/91/">Extragalactic Distances from the J-region Asymptotic Giant Branch<
 /a>\nby Abigail J. Lee (University of Chicago) as part of Cosmology Talks\
 n\n\nAbstract\nAbigail Lee tells us about how she has used the J-region As
 ymptotic Giant Branch (JAGB) to measure extragalactic distances\, ultimate
 ly using them as a rung on the distance ladder to measure the expansion ra
 te of the universe.\n\nThe JAGB method is new\, at least compared to cephe
 ids and "tip of the red giant" (TRGB) methods\, but is also very promising
 . The stars it uses are bright\, so they can be seen at large distances\, 
 and they're numerous\, which means they can be observed far from the centr
 es of galaxies (minimising "crowding" from other stars in the same pixels)
 . So\, even ignoring Hubble tensions\,  this is a very exciting time to be
  involved in extragalactic distance measurements.\n\nAbby used data from J
 WST to detect the JAGB mode brightness\, which is then the distance indica
 tor of the method. With more telescope time\, and more local calibrators\,
  JAGB will only go from strength to strength.\n\nWhen the measured distanc
 es are compared to JWST measurements of TRGB and cepheids it has very litt
 le scatter with TRGB\, but a little more from cepheids. The ultimate Hubbl
 e parameter is also on the smaller side\, consistent with CMB + ΛCDM and 
 on the border of being inconsistent with SH0ES cepheid+HST based measureme
 nts.\n\nTalk video: <a href="https://youtu.be/mpSsmyInrEA">youtu.be/mpSsmy
 InrEA</a>\n\nAbby: <a href="https://abiglee7.github.io/">abiglee7.github.i
 o</a>\n\nThe paper: <a href="https://arxiv.org/abs/2408.03474">arXiv: 2408
 .03474</a>\n\nAlso see recent\, related Cosmology Talk with Wendy Freedman
  and Barry Madore at <a href="https://youtu.be/OkGUoKukwk8">youtu.be/OkGUo
 Kukwk8</a>\n\n<hr>\n\n[00:00] <a href="https://youtu.be/mpSsmyInrEA?t=0s">
 Intro comments by Shaun</a>\n\n[01:06] <a href="https://youtu.be/mpSsmyInr
 EA?t=66s">Abby's opening comments on paper and CCHP</a>\n\n[01:37] <a href
 ="https://youtu.be/mpSsmyInrEA?t=97s">Two takeaways to remember</a>\n\n[02
 :36] <a href="https://youtu.be/mpSsmyInrEA?t=156s">Background and motivati
 on for this work</a>\n\n[04:50] <a href="https://youtu.be/mpSsmyInrEA?t=29
 0s">Asymptotic Giant Branch Stars \, HR diagram\, carbon stars as standard
  candles</a>\n\n[06:38] <a href="https://youtu.be/mpSsmyInrEA?t=398s">The 
 J-Region Asymptotic Giant Branch (JAGB) Method</a>\n\n[08:30] <a href="htt
 ps://youtu.be/mpSsmyInrEA?t=510s">History of the JAGB Method</a>\n\n[17:08
 ] <a href="https://youtu.be/mpSsmyInrEA?t=1028s">Comparison of brightnesse
 s between distance indicators</a>\n\n[18:58] <a href="https://youtu.be/mpS
 smyInrEA?t=1138s">The JAGB Method Advantages</a>\n\n[20:25] <a href="https
 ://youtu.be/mpSsmyInrEA?t=1245s">TRGB\, Cepheids\, and JAGB are independen
 t methods</a>\n\n[22:45] <a href="https://youtu.be/mpSsmyInrEA?t=1365s">Ho
 w accurate/precise are JAGB distances vs TRGB and Cepheids?</a>\n\n[25:38]
  <a href="https://youtu.be/mpSsmyInrEA?t=1538s">Comments on the paper</a>\
 n\n[30:32] <a href="https://youtu.be/mpSsmyInrEA?t=1832s">How do you know 
 where the outer disk is?</a>\n\n[33:32] <a href="https://youtu.be/mpSsmyIn
 rEA?t=2012s">Final H0 and Distance Comparisons</a>\n\n[37:21] <a href="htt
 ps://youtu.be/mpSsmyInrEA?t=2241s">Summary</a>\n\n[37:57] <a href="https:/
 /youtu.be/mpSsmyInrEA?t=2277s">Is JAGB the gold standard method of the fut
 ure?</a>\n\n[43:36] <a href="https://youtu.be/mpSsmyInrEA?t=2616s">What cu
 rrent work in cosmology is interesting but underappreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/91/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Ana Alexandre\, Valentin Thoss (Max Planck Institute for Physics)
DTSTART:20240921T060000Z
DTEND:20240921T070000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/92
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/92/">A New Window for PBH Dark Matter (Due to Delayed Hawking Radiation
 )?</a>\nby Ana Alexandre\, Valentin Thoss (Max Planck Institute for Physic
 s) as part of Cosmology Talks\n\n\nAbstract\nAna Alexandre and Valentin Th
 oss tell us about their recent papers examining the consequences of a pote
 ntial "memory burden" effect on decaying primordial blackholes (PBHs). \n\
 nThis memory burden effect would be a consequence of quantum gravity and w
 ould substantially slow down the Hawking evaporation of blackholes. The co
 nsequences for primordial blackholes would be very important because it wo
 uld open a whole window of PBH masses as dark matter candidates. (Masses t
 hat are normally ignored because PBHs of these masses are presumed to have
  decayed by today.)\n\nAll fundamental physicists would agree that Hawking
  radiation must breakdown at some point at/before a blackhole reaches the 
 Planck mass. This proposed memory burden effect goes a step further and cl
 aims that the breakdown must happen no later than when a blackhole has dec
 ayed to half of its original mass. This is not universally agreed upon\, b
 ut it's still worth examining the consequences if it is true.\n\nRecorded 
 video: <a href="https://youtu.be/p8UhnWri4II">youtu.be/p8UhnWri4II</a>\n\n
 Ana: <a href="https://www.linkedin.com/in/ana-alexandre-a13548197">at link
 edin</a><br>\nValentin: <a href="https://www.mpe.mpg.de/personnel/122518">
 at Max Planck Inst</a>\n\nAna's paper: <a href="https://arxiv.org/abs/2402
 .14069">arXiv: 2402.14069</a><br>\nValentin's paper: <a href="https://arxi
 v.org/abs/2402.17823">arXiv: 2402.17823</a>\n\n<hr>\n\n[00:00] <a href="ht
 tps://youtu.be/p8UhnWri4II?t=0s">Intro comments by Shaun</a>\n\n[01:30] <a
  href="https://youtu.be/p8UhnWri4II?t=90">Brief opening comments by Valent
 in</a>\n\n[02:18] <a href="https://youtu.be/p8UhnWri4II?t=138">Two takeawa
 ys to remember by Ana</a>\n\n[02:50] <a href="https://youtu.be/p8UhnWri4II
 ?t=170">Getting into the background</a>\n\n[07:45] <a href="https://youtu.
 be/p8UhnWri4II?t=465">Black hole evaporation\; "memory burden" effect</a>\
 n\n[14:32] <a href="https://youtu.be/p8UhnWri4II?t=872">How well accepted 
 is the memory burden effect by experts in its field?</a>\n\n[17:34] <a hre
 f="https://youtu.be/p8UhnWri4II?t=1054">New parameter space for PBH DM</a>
 \n\n[21:06] <a href="https://youtu.be/p8UhnWri4II?t=1266">Big Bang Nucleos
 ynthesis</a>\n\n[22:24] <a href="https://youtu.be/p8UhnWri4II?t=1344">Rela
 xing constraints with memory burden</a>\n\n[26:51] <a href="https://youtu.
 be/p8UhnWri4II?t=1611">4 Constraints (sections 2.5-2.8 in 2402.17823)</a>\
 n\n[27:41] <a href="https://youtu.be/p8UhnWri4II?t=1661">Constraints from 
 galactic gamma ray emission</a>\n\n[32:22] <a href="https://youtu.be/p8Uhn
 Wri4II?t=1942">The other 3 constraints</a>\n\n[37:42] <a href="https://you
 tu.be/p8UhnWri4II?t=2262">The landscape of constraints</a>\n\n[38:53] <a h
 ref="https://youtu.be/p8UhnWri4II?t=2333">Combined constraints plot (Fig. 
 1 in 2402.17823)</a>\n\n[42:18] <a href="https://youtu.be/p8UhnWri4II?t=25
 38">Discussion re lower bound on the mass</a>\n\n[43:40] <a href="https://
 youtu.be/p8UhnWri4II?t=2620">Where to next?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/92/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Daniele Sorini (Durham University)
DTSTART:20241113T050000Z
DTEND:20241113T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/93
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/93/">How Dark Energy Affects Past and Future Star Formation</a>\nby Dan
 iele Sorini (Durham University) as part of Cosmology Talks\n\n\nAbstract\n
 Daniele Sorini tells us about his research looking into how the value of d
 ark energy affects star formation in the universe. He builds an analytic m
 odel of star formation in the universe\, which allows him to follow the un
 iverse to very late times and ask "if Λ was different\, how many total st
 ars could form over the entire history of the universe?"\n\nThis is the cr
 ucial question one wants to ask when examining anthropic explanations of 
 Λ scientifically. Previous studies have asked this question using simulat
 ions\, forcing them to stop after a finite amount of time.\n\nFascinatingl
 y\, Daniele finds that there is a value of Λ where star formation peaks\,
  which is about 0.1 times the value in our universe. Previous simulation-b
 ased studies maybe didn't spot this because they simply didn't do simulati
 ons with Λ less than our observed value\, except for Λ=0\, but also they
  didn't go to late enough times.\n\nWhen combined with a uniform prior for
  Λ he finds that our value\, or a value smaller than it still only has a 
 0.5% chance\, but with other priors one gets other results.\n\nTalk video:
  <a href="https://youtu.be/cgfV2vwtEgs">youtu.be/cgfV2vwtEgs</a>\n\nThe pa
 per: <a href="https://arxiv.org/abs/2411.07301">arXiv: 2411.07301</a>\n\nD
 aniele: <a href="https://www.danielesorini.com/">danielesorini.com</a>\n\n
 <hr>\n\n<strong>Index to Key Parts of the Talk</strong>\n\n[0:00:00] <a hr
 ef="https://youtu.be/cgfV2vwtEgs?t=0s">Intro comments by Shaun</a>\n\n[0:0
 1:13] <a href="https://youtu.be/cgfV2vwtEgs?t=73s">Brief opening comments 
 by Daniele</a>\n\n[0:02:09] <a href="https://youtu.be/cgfV2vwtEgs?t=129s">
 Sneak preview of the results</a>\n\n[0:05:07] <a href="https://youtu.be/cg
 fV2vwtEgs?t=307s">What was surprising about the results?</a>\n\n[0:07:24] 
 <a href="https://youtu.be/cgfV2vwtEgs?t=444s">Motivation and current relev
 ance for this work</a>\n\n[0:15:59] <a href="https://youtu.be/cgfV2vwtEgs?
 t=959s">Can ΛCDM explain observations?</a>\n\n[0:27:03] <a href="https://
 youtu.be/cgfV2vwtEgs?t=1623s">Diff models reach diff conclusions but all p
 osteriors peak at Λ>>Λobs</a>\n\n[0:29:53] <a href="https://youtu.be/cgf
 V2vwtEgs?t=1793s">Details</a>\n\n[0:36:48] <a href="https://youtu.be/cgfV2
 vwtEgs?t=2208s">Improved match with observations of cosmic SFR density vs 
 time</a>\n\n[0:39:25] <a href="https://youtu.be/cgfV2vwtEgs?t=2365s">Stell
 ar mass density converges as time tends to infinity</a>\n\n[0:41:18] <a hr
 ef="https://youtu.be/cgfV2vwtEgs?t=2478s">Star formation saturates at t>>1
 00 Gyr (Fig 9 in paper)</a>\n\n[0:49:31] <a href="https://youtu.be/cgfV2vw
 tEgs?t=2971s">Larger Λ -> Fewer massive haloes (Fig 4)</a>\n\n[0:50:20] <
 a href="https://youtu.be/cgfV2vwtEgs?t=3020s">Larger Λ -> More efficient 
 haloes (Fig 8)</a>\n\n[0:55:56] <a href="https://youtu.be/cgfV2vwtEgs?t=33
 56s">Does Λ=Λobs promote the generation of observers? (Fig 11)</a>\n\n[0
 :58:14] <a href="https://youtu.be/cgfV2vwtEgs?t=3494s">Conclusions very se
 nsitive to prior on Λ (Fig 12)</a>\n\n[1:01:27] <a href="https://youtu.be
 /cgfV2vwtEgs?t=3687s">Conclusions</a>\n\n[1:09:25] <a href="https://youtu.
 be/cgfV2vwtEgs?t=4164s">Where to next?</a>\n\n[1:17:20] <a href="https://y
 outu.be/cgfV2vwtEgs?t=4640s">What current cosmology work is interesting bu
 t underappreciated by the community?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/93/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Arnaud de Mattia\, Héctor Gil-Marín\, Pauline Zarrouk (DESI Coll
 aboration)
DTSTART:20241120T050000Z
DTEND:20241120T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/94
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/94/">DESI 2024: Cosmology Results from the Power Spectrum's Full Shape<
 /a>\nby Arnaud de Mattia\, Héctor Gil-Marín\, Pauline Zarrouk (DESI Coll
 aboration) as part of Cosmology Talks\n\n\nAbstract\nArnaud de Mattia\, He
 ctor Gil-Marín and Pauline Zarrouk tell us about the latest DESI key pape
 rs. These ones are covering the "full shape" of the galaxy power spectrum.
  This is in contrast to their results from April\, which were centred arou
 nd the Baryon Acoustic Oscillation (BAO) feature.\n\nThe analysis is an ab
 solute tour de force\, explaining why the video is so long. DESI have done
  a lot of analysis and it takes a while to unpack. (The raw recording of t
 his video was more than 200 minutes long!)\n\nThe results aren't quite so 
 eye-opening as the BAO ones were in April. The evidence for evolving dark 
 energy is still there\, but the significance of this evidence hasn't chang
 ed much. They are however able to do a bunch of tests of modified gravity 
 and find that\, unlike ΛCDM\, General Relativity appears to be in great s
 hape (at least as far as DESI observations are concerned).\n\nWe're proper
 ly in the era of Stage 4 cosmology now! Thanks DESI for the wonderful anal
 yses and results.\n\nTalk video recording: <a href="https://www.youtube.co
 m/watch?v=-2mlU-YzEbw">youtu.be/2mlU-YzEbw</a>\n\nRelevant papers on the a
 rXiv:<br>\n<a href="https://arxiv.org/abs/2411.12026">2411.12026</a> - Mod
 ified Gravity Constraints from the Full Shape Modeling of Clustering Measu
 rements from DESI 2024<br>\n<a href="https://arxiv.org/abs/2411.12025">241
 1.12025</a> - Characterization of DESI fiber assignment incompleteness eff
 ect on 2-point clustering and mitigation methods for DR1 analysis<br>\n<a 
 href="https://arxiv.org/abs/2411.12024">2411.12024</a> - Mitigating Imagin
 g Systematics for DESI 2024 Emission Line Galaxies and Beyond<br>\n<a href
 ="https://arxiv.org/abs/2411.12023">2411.12023</a> - Exploring HOD-depende
 nt systematics for the DESI 2024 Full-Shape galaxy clustering analysis<br>
 \n<a href="https://arxiv.org/abs/2411.12022">2411.12022</a> - DESI 2024 VI
 I: Cosmological Constraints from the Full-Shape Modeling of Clustering Mea
 surements<br>\n<a href="https://arxiv.org/abs/2411.12021">2411.12021</a> -
  DESI 2024 V: Full-Shape Galaxy Clustering from Galaxies and Quasars<br>\n
 <a href="https://arxiv.org/abs/2411.12020">2411.12020</a> - DESI 2024 II: 
 Sample Definitions\, Characteristics\, and Two-point Clustering Statistics
 <br>\n\nArnaud: <a href="https://inspirehep.net/authors/1881382">inspirehe
 p.net/authors/1881382</a><br>\nHector: <a href="https://www.ub.edu/bispect
 rum/">www.ub.edu/bispectrum</a><br>\nPauline: <a href="https://inspirehep.
 net/authors/1884383">inspirehep.net/authors/1884383</a><br>\n\nDESI itself
 : <a href="https://www.desi.lbl.gov/">desi.lbl.gov</a><br>\n\nTimestamp li
 nks to key parts of the talk:<br> \n<a href="https://www.youtube.com/watch
 ?v=-2mlU-YzEbw&amp\;t=0s">00:00</a> Intro and brief overview of new result
 s<br>\n<a href="https://www.youtube.com/watch?v=-2mlU-YzEbw&amp\;t=372s">0
 6:12</a> The background and motivation<br>\n<a href="https://www.youtube.c
 om/watch?v=-2mlU-YzEbw&amp\;t=1445s">24:05</a> Full shape galaxy clusterin
 g analysis<br>\n<a href="https://www.youtube.com/watch?v=-2mlU-YzEbw&amp\;
 t=3346s">55:46</a> Systematic effects<br>\n<a href="https://www.youtube.co
 m/watch?v=-2mlU-YzEbw&amp\;t=4210s">1:10:10</a> Cosmology results!<br>\n<a
  href="https://www.youtube.com/watch?v=-2mlU-YzEbw&amp\;t=4768s">1:19:28</
 a> Beyond ΛCDM and GR constraints<br>\n<a href="https://www.youtube.com/w
 atch?v=-2mlU-YzEbw&amp\;t=5822s">1:37:02</a> Conclusions and additional di
 scussion<br>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/94/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Guadalupe Cañas Herrera\, Hervé Aussel (Euclid Consortium)
DTSTART:20250319T050000Z
DTEND:20250319T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/95
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/95/">Euclid 2025: Science Goals and Q1 Data Summary</a>\nby Guadalupe C
 añas Herrera\, Hervé Aussel (Euclid Consortium) as part of Cosmology Tal
 ks\n\n\nAbstract\nThe day has arrived. The space observatory Euclid is pro
 ducing and sharing results. In this video Guadalupe Cañas-Herrera and Her
 vé Aussel tell us about Euclid\, its science goals and the Q1 data set th
 ey have released today.\n\n<a href="https://www.youtube.com/watch?v=DVlKqF
 rvhRY">Talk video recording</a>\n\n<a href="https://www.euclid-ec.org/scie
 nce/publications/">Euclid Papers</a>\n\n<a href="https://www.euclid-ec.org
 /public/press-releases/euclid-quick-data-release-1/">Euclid Consortium det
 ails on the Q1 release</a>\n\n<a href="https://www.cosmos.esa.int/web/eucl
 id/euclid-q1-data-release">ESA details on the Euclid Q1 release</a>\n\n<hr
 >\n\n<b>Index to Key Parts of the Talk</b>\n\n[01:18] <a href="https://you
 tu.be/DVlKqFrvhRY&t=78s">Euclid overview</a>\n\n[02:21] <a href="https://y
 outu.be/DVlKqFrvhRY&t=141s">Euclid: intro and goals\; dark energy\, accele
 rated expansion\, dark matter</a>\n\n[04:38] <a href="https://youtu.be/DVl
 KqFrvhRY&t=278s">Why the name Euclid?</a>\n\n[06:28] <a href="https://yout
 u.be/DVlKqFrvhRY&t=388s">Universe timeline\; Euclid targets 0 < z < 3 to s
 tudy LSS and create 3D map</a>\n\n[08:58] <a href="https://youtu.be/DVlKqF
 rvhRY&t=538s">Two probes: cosmic shear and galaxy clustering</a>\n\n[12:35
 ] <a href="https://youtu.be/DVlKqFrvhRY&t=755s">Mapping the Universe in 3D
 </a>\n\n[13:05] <a href="https://youtu.be/DVlKqFrvhRY&t=785s">Euclid space
 craft and instrument details</a>\n\n[18:46] <a href="https://youtu.be/DVlK
 qFrvhRY&t=1126s">Scope of the Euclid Wide Survey</a>\n\n[19:59] <a href="h
 ttps://youtu.be/DVlKqFrvhRY&t=1199s">What to Expect</a>\n\n[20:50] <a href
 ="https://youtu.be/DVlKqFrvhRY&t=1250s">Advantages of Euclid as a space mi
 ssion</a>\n\n[22:06] <a href="https://youtu.be/DVlKqFrvhRY&t=1326s">Outloo
 k for constraints on w\\_0 and w\\_a</a>\n\n[23:40] <a href="https://youtu
 .be/DVlKqFrvhRY&t=1420s">Q1 Data Release Contents</a>\n\n[26:06] <a href="
 https://youtu.be/DVlKqFrvhRY&t=1566s">The Euclid Deep Fields</a>\n\n[30:16
 ] <a href="https://youtu.be/DVlKqFrvhRY&t=1816s">Q1 Processing</a>\n\n[33:
 32] <a href="https://youtu.be/DVlKqFrvhRY&t=2012s">Photometric Redshifts a
 nd Photometric Classification</a>\n\n[34:55] <a href="https://youtu.be/DVl
 KqFrvhRY&t=2095s">Physical Parameters</a>\n\n[36:31] <a href="https://yout
 u.be/DVlKqFrvhRY&t=2191s">NISP Spectroscopy</a>\n\n[40:16] <a href="https:
 //youtu.be/DVlKqFrvhRY&t=2416s">SPE Redshifts Measurements</a>\n\n[47:13] 
 <a href="https://youtu.be/DVlKqFrvhRY&t=2833s">Important Caveats</a>\n\n[5
 0:54] <a href="https://youtu.be/DVlKqFrvhRY&t=3054s">Conclusion</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/95/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Teresa Matamoro\, Mike Walmsley\, Phil Holloway (Euclid Consortium
 )
DTSTART:20250319T050000Z
DTEND:20250319T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/96
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/96/">Euclid 2025: AGN\, Galaxy Morphology & Strong Lensing</a>\nby Tere
 sa Matamoro\, Mike Walmsley\, Phil Holloway (Euclid Consortium) as part of
  Cosmology Talks\n\n\nAbstract\nTeresa Matamoro\, Mike Walmsley and Phil H
 olloway tell us about three key areas Euclid has shed a scientific light o
 n in their Q1 data release today. These are active galactic nuclei\, galax
 y morphology and strong lensing.\n\n<a href="https://www.youtube.com/watch
 ?v=YGqaxDH00Yw">Talk video recording</a>\n\n<a href="https://www.euclid-ec
 .org/science/publications/">Euclid Papers</a>\n\n<a href="https://www.eucl
 id-ec.org/public/press-releases/euclid-quick-data-release-1/">Euclid Conso
 rtium details on the Q1 release</a>\n\n<a href="https://www.cosmos.esa.int
 /web/euclid/euclid-q1-data-release">ESA details on the Euclid Q1 release</
 a>\n\n<strong>Papers:</strong>\n\n<a href="https://arxiv.org/abs/2503.1532
 6">[2503.15326] Euclid Quick Data Release (Q1). The Strong Lensing Discove
 ry Engine C - Finding lenses with machine learning</a>\n\n<a href="https:/
 /arxiv.org/abs/2503.15324">[2503.15324] Euclid Quick Data Release (Q1): Th
 e Strong Lensing Discovery Engine A -- System overview and lens catalogue<
 /a>\n\n<a href="https://arxiv.org/abs/2503.15320">[2503.15320] Euclid Quic
 k Data Release (Q1). The active galaxies of Euclid</a>\n\n<a href="https:/
 /arxiv.org/abs/2502.06505">[2502.06505] Euclid: A complete Einstein ring i
 n NGC 6505</a>\n\n<a href="https://arxiv.org/abs/2404.02973">[2404.02973] 
 Scaling Laws for Galaxy Images</a>\n\n<hr>\n\n<b>Timestamp Index to Key Pa
 rts of the Talk</b>\n\n[00:00:00] <a href="https://youtu.be/YGqaxDH00Yw?t=
 0s">Shaun's intro</a>\n\n[00:01:03] <a href="https://youtu.be/YGqaxDH00Yw?
 t=63s">AGN overview (Teresa)</a>\n\n[00:05:47] <a href="https://youtu.be/Y
 GqaxDH00Yw?t=347s">New results and main takeaways</a>\n\n[00:09:43] <a hre
 f="https://youtu.be/YGqaxDH00Yw?t=583s">Building a multi-wavelength catalo
 gue</a>\n\n[00:13:54] <a href="https://youtu.be/YGqaxDH00Yw?t=834s">Colour
 -colour selections</a>\n\n[00:17:31] <a href="https://youtu.be/YGqaxDH00Yw
 ?t=1051s">Spectroscopy</a>\n\n[00:18:51] <a href="https://youtu.be/YGqaxDH
 00Yw?t=1131s">SED fitting</a>\n\n[00:20:32] <a href="https://youtu.be/YGqa
 xDH00Yw?t=1232s">Other AGN works</a>\n\n[00:21:22] <a href="https://youtu.
 be/YGqaxDH00Yw?t=1282s">What next?</a>\n\n[00:22:38] <a href="https://yout
 u.be/YGqaxDH00Yw?t=1358s">Application to cosmology (Mike)</a>\n\n[00:23:44
 ] <a href="https://youtu.be/YGqaxDH00Yw?t=1424s">Galaxy morphology</a>\n\n
 [00:31:34] <a href="https://youtu.be/YGqaxDH00Yw?t=1894s">What are foundat
 ion models?</a>\n\n[00:38:08] <a href="https://youtu.be/YGqaxDH00Yw?t=2288
 s">Strong lensing (Phil)</a>\n\n[00:42:01] <a href="https://youtu.be/YGqax
 DH00Yw?t=2521s">497 strong lenses found in Euclid Q1</a>\n\n[00:44:29] <a 
 href="https://youtu.be/YGqaxDH00Yw?t=2669s">Euclid will revolutionise stro
 ng lensing</a>\n\n[00:47:33] <a href="https://youtu.be/YGqaxDH00Yw?t=2853s
 ">The Euclid Strong Lensing Discovery Engine</a>\n\n[00:54:43:] <a href="h
 ttps://youtu.be/YGqaxDH00Yw?t=3283s">Which lenses did we find?</a>\n\n[00:
 57:28] <a href="https://youtu.be/YGqaxDH00Yw?t=3448s">Notable lens candida
 tes</a>\n\n[01:02:49] <a href="https://youtu.be/YGqaxDH00Yw?t=3769s">With 
 100k future strong lenses\, any possibility of GR tests?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/96/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Cristhian Garcia Quintero\, Paul Martini (DESI Collaboration)
DTSTART:20250319T050000Z
DTEND:20250319T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/97
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/97/">Cosmology Results from DESI DR2 BAO</a>\nby Cristhian Garcia Quint
 ero\, Paul Martini (DESI Collaboration) as part of Cosmology Talks\n\n\nAb
 stract\nCristhian Garcia Quintero and Paul Martini tell us about the baryo
 n acoustic oscillation measurements in data release two (DR2) of the Dark 
 Energy Spectroscopic Instrument (three years of data). As with the first d
 ata release they are seeing evidence for evolving dark energy. They now se
 e it when combining with just CMB\, or with "just" Dark Energy Survey supe
 rnovae and clustering data.\n\nTalk Recording: <a href="https://www.youtub
 e.com/watch?v=YiRaDtslycE">youtube.com/watch?v=YiRaDtslycE</a>\n\nCristhia
 n Garcia Quintero: <a href="https://gqcristhian.github.io/">gqcristhian.gi
 thub.io</a>\n\nPaul Martini: <a href="https://astronomy.osu.edu/people/mar
 tini.10">OSU.edu</a>\n\n<a href="https://www.desi.lbl.gov/2025/03/19/desi-
 dr2-results-march-19-guide/">Guide to DESI DR2 Results\, dated 19-Mar-2025
 </a>\n\nRelevant papers on the arXiv:\n\n<a href="https://arxiv.org/abs/25
 03.14738">[2503.14738] DESI DR2 Results II: Measurements of Baryon Acousti
 c Oscillations and Cosmological Constraints</a>\n\n<a href="https://arxiv.
 org/abs/2503.14739">[2503.14739] DESI DR2 Results I: Baryon Acoustic Oscil
 lations from the Lyman Alpha Forest</a>\n\n<a href="https://arxiv.org/abs/
 2503.14741">[2503.14741] Validation of the DESI DR2 Ly$α$ BAO analysis us
 ing synthetic datasets</a>\n\n<a href="https://arxiv.org/abs/2503.14742">[
 2503.14742] Validation of the DESI DR2 Measurements of Baryon Acoustic Osc
 illations from Galaxies and Quasars</a>\n\n<a href="https://arxiv.org/abs/
 2503.14743">[2503.14743] Extended Dark Energy analysis using DESI DR2 BAO 
 measurements</a>\n\n<a href="https://arxiv.org/abs/2503.14744">[2503.14744
 ] Constraints on Neutrino Physics from DESI DR2 BAO and DR1 Full Shape</a>
 \n\n<hr>\n\n<b>Timestamp Index to Key Parts of the Talk</b>\n\n[00:00:00] 
 <a href="https://youtu.be/YiRaDtslycE?t=0s">Shaun's intro</a>\n\n[00:00:54
 ] <a href="https://youtu.be/YiRaDtslycE?t=54s">Overview of findings</a>\n\
 n[00:02:53] <a href="https://youtu.be/YiRaDtslycE?t=173s">Main plot of res
 ults with and w/o supernova datasets</a>\n\n[00:03:46] <a href="https://yo
 utu.be/YiRaDtslycE?t=226s">The highest significance plot and the role of D
 ES Y5 data</a>\n\n[00:04:40] <a href="https://youtu.be/YiRaDtslycE?t=280s"
 >w0wa parameterization vs physical models beyond LCDM</a>\n\n[00:07:55] <a
  href="https://youtu.be//YiRaDtslycE?t=475s">Getting deeper into the backg
 round</a>\n\n[00:09:14] <a href="https://youtu.be/YiRaDtslycE?t=554s">The 
 BAO scale as a "standard ruler"</a>\n\n[00:14:00] <a href="https://youtu.b
 e/YiRaDtslycE?t=840s">Mystery of Cosmic Acceleration slide</a>\n\n[00:15:1
 8] <a href="https://youtu.be/YiRaDtslycE?t=918s">Getting into details of B
 AO measurements from DESI DR2</a>\n\n[00:17:10] <a href="https://youtu.be/
 YiRaDtslycE?t=1030s">Transition from DESI DR1 to DR2</a>\n\n[00:18:43] <a 
 href="https://youtu.be/YiRaDtslycE?t=1123s">DESI Data Release 2</a>\n\n[00
 :20:13] <a href="https://youtu.be/YiRaDtslycE?t=1213s">Correlation functio
 n measurements</a>\n\n[00:28:16] <a href="https://youtu.be/YiRaDtslycE?t=1
 696s">DESI LyA Measurement</a>\n\n[00:32:50] <a href="https://youtu.be/YiR
 aDtslycE?t=1970s">DESI LyA BAO Measurement</a>\n\n[00:38:59] <a href="http
 s://youtu.be/YiRaDtslycE?t=2339">Cosmological constraints under LCDM</a>\n
 \n[00:50:33] <a href="https://youtu.be/YiRaDtslycE?t=3033">Omega_m under w
 0waCDM</a>\n\n[00:51:25] <a href="https://youtu.be/YiRaDtslycE?t=3085">Con
 straints on evolving dark energy</a>\n\n[00:58:45] <a href="https://youtu.
 be/YiRaDtslycE?t=3525">Robustness of the DE results</a>\n\n[01:03:38] <a h
 ref="https://youtu.be/YiRaDtslycE?t=3818">Binning the DE equation of state
 </a>\n\n[01:06:50] <a href="https://youtu.be/YiRaDtslycE?t=4010">DESI and 
 neutrino mass</a>\n\n[01:11:00] <a href="https://youtu.be/YiRaDtslycE?t=42
 60">Future outlook</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/97/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Wright\, Stölzner\, Reischke\, Asgari\, Kuijken (Kilo-Degree Surv
 ey (KiDS))
DTSTART:20250326T050000Z
DTEND:20250326T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/98
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/98/">KiDS­ Legacy - The Final Cosmology Results</a>\nby Wright\, Stöl
 zner\, Reischke\, Asgari\, Kuijken (Kilo-Degree Survey (KiDS)) as part of 
 Cosmology Talks\n\n\nAbstract\nAngus Wright\, Benjamin Stölzner\, Robert 
 Reischke\, Marika Asgari and Konrad Kuijken tell us about the final cosmol
 ogy results from the Kilo Degree Survey (KiDS-Legacy). After exhaustive im
 provement of their analysis\, and consistency tests\, and a six month wand
 er in the B-Mode wilderness they emerge with no S8 tension at all.\n\nTalk
  Video Recording: <a href="https://youtu.be/PIQKe-tW1xQ">youtu.be/PIQKe-tW
 1xQ</a>\n\nAngus: <a href="https://anguswright.github.io/">anguswright.git
 hub.io</a>\n\nBenjamin: <a href="https://inspirehep.net/authors/1944983">i
 nspirehep.net/authors/1944983</a>\n\nRobert: <a href="https://inspirehep.n
 et/authors/2219647">inspirehep.net/authors/2219647</a>\n\nMarika: <a href=
 "https://www.ncl.ac.uk/maths-physics/people/profile/marikaasgari.html">ncl
 .ac.uk/...</a>\n\nKonrad: <a href="https://www.universiteitleiden.nl/en/st
 affmembers/koen-kuijken#tab-1">universiteitleiden.nl/...</a>\n\n<b>Papers:
 </b>\n\n<a href="https://arxiv.org/abs/2503.19442">2503.19442</a>\n\n<a hr
 ef="https://arxiv.org/abs/2503.19441">2503.19441</a>\n\n<a href="https://a
 rxiv.org/abs/2503.19440">2503.19440</a>\n\n<hr>\n\n<b>Index to Key Parts o
 f Talk</b>\n\n[00:00:00] <a href="https://youtu.be/PIQKe-tW1xQ?t=0s">Shaun
 's intro</a>\n\n[00:01:00] <a href="https://youtu.be/PIQKe-tW1xQ?t=60s">Ov
 erview and main cosmological constraints</a>\n\n[00:04:11] <a href="https:
 //youtu.be/PIQKe-tW1xQ?t=251s">Internal Consistency Constraints</a>\n\n[00
 :05:15] <a href="https://youtu.be/PIQKe-tW1xQ?t=315s">The early vs late de
 bate</a>\n\n[00:07:20] <a href="https://youtu.be/PIQKe-tW1xQ?t=440s">Bluep
 rint for Stage-IV\; Why now? Why not sooner?</a>\n\n[00:10:26] <a href="ht
 tps://youtu.be/PIQKe-tW1xQ?t=626s">Since 2021: Updated calibrations\, samp
 les\, and area</a>\n\n[00:20:00] <a href="https://youtu.be/PIQKe-tW1xQ?t=1
 200s">Details of KiDS Legacy analysis: Redshift Calibration</a>\n\n[00:27:
 43] <a href="https://youtu.be/PIQKe-tW1xQ?t=1663s">Covariance and modellin
 g</a>\n\n[00:33:51] <a href="https://youtu.be/PIQKe-tW1xQ?t=2031s">Updated
  Astrometric Calibration</a>\n\n[00:36:17] <a href="https://youtu.be/PIQKe
 -tW1xQ?t=2177s">B-modes issue</a>\n\n[00:43:05] <a href="https://youtu.be/
 PIQKe-tW1xQ?t=2585s">Internal Consistency</a>\n\n[00:54:20] <a href="https
 ://youtu.be/PIQKe-tW1xQ?t=3260s">Consistency motivates further joint analy
 ses</a>\n\n[01:00:21] <a href="https://youtu.be/PIQKe-tW1xQ?t=3621s">What'
 s next? Onwards to Stage-IV</a>\n\n[01:02:23] <a href="https://youtu.be/PI
 QKe-tW1xQ?t=3743s">What's underappreciated by the community in current cos
 mology work?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/98/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Sankarshana Srinivasan (Ludwig-Maximilians Universitat)
DTSTART:20251107T050000Z
DTEND:20251107T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/99
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/99/">Cosmological Gravity on All Scales</a>\nby Sankarshana Srinivasan 
 (Ludwig-Maximilians Universitat) as part of Cosmology Talks\n\n\nAbstract\
 nSankarshana Srinivasan tells us about his work building the framework to 
 constrain (or detect!) modified gravity using upcoming surveys. Building o
 n earlier work developing model independent modified gravity simulations\,
  Shankar now shows how a clever transform (the BNT transform) is able to b
 etter isolate the weak-lensing kernel\, meaning one can more cleanly cut o
 ut the fully messy non-linear scales without losing too much usable inform
 ation. We're all looking forward to the talk in 3-5 years' time applying t
 hese methods to Euclid and LSST data!\n\nPaper: <a href="https://arxiv.org
 /abs/2409.06569">arXiv: 2409.06569</a>\n\nTalk video: <a href="https://www
 .youtube.com/watch?v=nIdCpcObSVU">youtube.com/watch?v=nIdCpcObSVU</a>\n\nC
 osmology Talk on earlier work in this series by Dan Thomas: <a href="https
 ://www.youtube.com/watch?v=orMFALXtU8g">The first model independent cosmol
 ogical simulations of modified gravity</a>\n\n<b>Index to Key Parts of the
  Talk</b>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=0s">Shaun's intro</a>
 \n\n<a href="https://youtu.be/nIdCpcObSVU?t=64s">Shankar's brief overview 
 on the paper</a>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=216s">A key in
 sight: mitigating baryonic feedback</a>\n\n<a href="https://youtu.be/nIdCp
 cObSVU?t=358s">A physical intuition on mu μ and eta η parameters</a>\n\n
 <a href="https://youtu.be/nIdCpcObSVU?t=655s">Binning strategies</a>\n\n<a
  href="https://youtu.be/nIdCpcObSVU?t=744s">Some Problems with ΛCDM</a>\n
 \n<a href="https://youtu.be/nIdCpcObSVU?t=943s">Vast model space</a>\n\n<a
  href="https://youtu.be/nIdCpcObSVU?t=1099s">Post-Friedmann Formalism: Pix
 elized Poisson Equation</a>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=162
 4s">N-body simulations: Measuring P(k) for binned μ</a>\n\n<a href="https
 ://youtu.be/nIdCpcObSVU?t=1886s">N-body simulations: ReACT for binned μ</
 a>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=2547s">N-body simulations: C
 omputing 3x2pt observables</a>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=
 2718s">Fisher Forecasts</a>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=282
 1s">Fisher Forecasts: Key questions</a>\n\n<a href="https://youtu.be/nIdCp
 cObSVU?t=2842s">The Bernardeau-Nimishi-Taruya (BNT) Transform</a>\n\n<a hr
 ef="https://youtu.be/nIdCpcObSVU?t=2988s">Mitigating Baryonic Feedback</a>
 \n\n<a href="https://youtu.be/nIdCpcObSVU?t=3388s">Where does the constrai
 ning power come from?</a>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=3502s
 ">Adding the concentration fit</a>\n\n<a href="https://youtu.be/nIdCpcObSV
 U?t=3534s">What next?</a>\n\n<a href="https://youtu.be/nIdCpcObSVU?t=3782s
 ">Summary slide points (but no discussion)</a>\n\n<a href="https://youtu.b
 e/nIdCpcObSVU?t=4325s">What current work in cosmology is interesting but u
 nderappreciated?</a>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/99/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Miguel Zumalacarregui (Max Planck  Institute for Gravitational Phy
 sics)
DTSTART:20260126T050000Z
DTEND:20260126T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/100
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/100/">A magnified and diffracted black hole merger (GW231123)</a>\nby M
 iguel Zumalacarregui (Max Planck  Institute for Gravitational Physics) as 
 part of Cosmology Talks\n\n\nAbstract\nCan gravitational waves get gravita
 tionally lensed? The first ever detection of this might have just happened
 . This is especially cool because if we could routinely measure lensing of
  gravitational waves\, we could use that to measure all sorts of other imp
 ortant things like the Hubble constant and precision tests of gravity to n
 ame just two. One of the interesting things you will hear about in today's
  talk is an improved modeling of the candidate lens. This better nails dow
 n the probability that the wave really was lensed and even more fun gives 
 insight into what astrophysical things the source and lens could be. In to
 day's talk\, we're joined by Miguel Zumalacarregui from the Max Plank Inst
 itute for Gravitational Physics in Potsdam\, Germany his new paper.\n\nVid
 eo recording: <a href="https://www.youtube.com/watch?v=ZGqOpDTL8k4">youtub
 e.com/watch?v=ZGqOpDTL8k4</a>\n\nMiguel: <a href="http://miguelzuma.github
 .io/">miguelzuma.github.io</a>\n\nPaper: <a href="https://arxiv.org/abs/25
 12.17631">arXiv: 2512.17631</a>\n\nLigo-Virgo-Kagra analysis: <a href="htt
 ps://arxiv.org/abs/2512.16347">arXiv: 2512.16347</a>\n\n<hr>\n\n<strong>In
 dex to Key Parts of the Talk</strong>\n\n<a href="https://www.youtube.com/
 watch?v=ZGqOpDTL8k46t=0s">[0:00:00] Shaun's intro\; potential new way to m
 easure H0 and test gravity</a><br>\n\n<a href="https://www.youtube.com/wat
 ch?v=ZGqOpDTL8k46t=54s">[0:00:54] Miguel's overview on paper and some thin
 gs it now allows doing</a><br>\n\n<a href="https://www.youtube.com/watch?v
 =ZGqOpDTL8k46t=145s">[0:02:25] Quick intro to the results\; statistical an
 alysis supports the lensing hypothesis\; non-symmetric lens</a><br>\n\n<a 
 href="https://www.youtube.com/watch?v=ZGqOpDTL8k46t=326s">[0:05:26] Is the
 re anything confusing about these results?</a><br>\n\n<a href="https://www
 .youtube.com/watch?v=ZGqOpDTL8k46t=386s">[0:06:26] Background and motivati
 on for this research</a><br>\n\n<a href="https://www.youtube.com/watch?v=Z
 GqOpDTL8k46t=675s">[0:11:15] Why lensing analysis can be done with gravita
 tional waves</a><br>\n\n<a href="https://www.youtube.com/watch?v=ZGqOpDTL8
 k46t=785s">[0:13:05] Error bars on the parameters</a><br>\n\n<a href="http
 s://www.youtube.com/watch?v=ZGqOpDTL8k46t=857s">[0:14:17] Journey of a len
 sed gravitational wave</a><br>\n\n<a href="https://www.youtube.com/watch?v
 =ZGqOpDTL8k46t=1162s">[0:19:22] Predicting and extracting these signals\; 
 Wave-optics lensing</a><br>\n\n<a href="https://www.youtube.com/watch?v=ZG
 qOpDTL8k46t=1318s">[0:21:58] Frequency evolution</a><br>\n\n<a href="https
 ://www.youtube.com/watch?v=ZGqOpDTL8k46t=1599s">[0:26:39] How different is
  a lensed one from unlensed one with different mass?</a><br>\n\n<a href="h
 ttps://www.youtube.com/watch?v=ZGqOpDTL8k46t=1637s">[0:27:17] Lens model\;
  Point lens + external potential</a><br>\n\n<a href="https://www.youtube.c
 om/watch?v=ZGqOpDTL8k46t=2062s">[0:34:22] GW231123 Bayesian analysis\; 3 m
 odels</a><br>\n\n<a href="https://www.youtube.com/watch?v=ZGqOpDTL8k46t=24
 64s">[0:41:04] Caveat: bias factors</a><br>\n\n<a href="https://www.youtub
 e.com/watch?v=ZGqOpDTL8k46t=2887s">[0:48:07] Resolution of unlensed analys
 is inconsistencies between different models</a><br>\n\n<a href="https://ww
 w.youtube.com/watch?v=ZGqOpDTL8k46t=3062s">[0:51:02] Surprising feature: s
 ky localization is much wider for the lensing analysis</a><br>\n\n<a href=
 "https://www.youtube.com/watch?v=ZGqOpDTL8k46t=3287s">[0:54:47] Microlens 
 properties</a><br>\n\n<a href="https://www.youtube.com/watch?v=ZGqOpDTL8k4
 6t=3483s">[0:58:03] What is the microlens? (IMBH\, stellar cluster\, DM ob
 ject\, etc?)</a><br>\n\n<a href="https://www.youtube.com/watch?v=ZGqOpDTL8
 k46t=3764s">[1:02:44] Additional macro-images?</a><br>\n\n<a href="https:/
 /www.youtube.com/watch?v=ZGqOpDTL8k46t=3951s">[1:05:51] Where to next? Out
 look: Additional lensing signatures</a><br>\n\n<a href="https://www.youtub
 e.com/watch?v=ZGqOpDTL8k46t=4217s">[1:10:17] Outlook: discover sources bey
 ond the detector horizon</a><br>\n\n<a href="https://www.youtube.com/watch
 ?v=ZGqOpDTL8k46t=4287s">[1:11:27] Another twist: lensing multi-messenger d
 elections</a><br>\n\n<a href="https://www.youtube.com/watch?v=ZGqOpDTL8k46
 t=4366s">[1:12:46] Conclusions</a><br>\n\n<a href="https://www.youtube.com
 /watch?v=ZGqOpDTL8k46t=4444s">[1:14:04] Particularly interesting cosmology
  work that's underappreciated by the community</a><br>\n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/100/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Jessie Muir\, Juan Mena-Fernández\, Santiago Avila\, Maria Vincen
 zi (Dark Energy Survey Collaboration)
DTSTART:20260204T050000Z
DTEND:20260204T060000Z
DTSTAMP:20260422T225706Z
UID:CosmologyTalks/101
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/CosmologyTal
 ks/101/">Dark Energy Survey - Combined cosmology from BAO + SN (+CMB)</a>\
 nby Jessie Muir\, Juan Mena-Fernández\, Santiago Avila\, Maria Vincenzi (
 Dark Energy Survey Collaboration) as part of Cosmology Talks\n\n\nAbstract
 \nFour members of the Dark Energy Survey Collaboration discuss the latest 
 findings. This talk is based on these two papers on the arXiv:\n\n(1) Main
  talk content: <a href="https://arxiv.org/abs/2503.06712">[2503.06712] Dar
 k Energy Survey: implications for cosmological expansion models from the f
 inal DES Baryon Acoustic Oscillation and Supernova data</a>\n\n(2) Newly r
 eleased paper: <a href="https://arxiv.org/abs/2601.14864">[2601.14864] Dar
 k Energy Survey: DESI-Independent Angular BAO Measurement</a>\n\nAbout the
  authors: <a href="https://www.jessiemuir.com/">Jessie Muir</a>\, <a href=
 "https://inspirehep.net/authors/2011410">Juan Mena-Fernández</a>\, <a hre
 f="https://savila.github.io/">Santiago Avila</a>\, <a href="https://www.ph
 ysics.ox.ac.uk/our-people/vincenzi">Maria Vincenzi</a>\n\n<hr>\n\n<b>Index
  to Key Parts of the Talk</b>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=0
 s">[0:00:00] Shaun's intro</a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=
 76s">[0:01:16] Overview of findings</a>\n\n<a href="https://youtu.be/ukMQg
 Hj6NMI?t=160s">[0:02:40] How independent is this from DESI?</a>\n\n<a href
 ="https://youtu.be/ukMQgHj6NMI?t=218s">[0:03:38] Anything particularly sur
 prising from the analysis?</a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=
 255s">[0:04:15] Tensions in simpler models\, data reconciled with w0waCDM<
 /a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=520s">[0:08:40] SN Ia and B
 AO as distance probes</a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=617s"
 >[0:10:17] The Dark Energy Survey (photometric)</a>\n\n<a href="https://yo
 utu.be/ukMQgHj6NMI?t=703s">[0:11:43] 4 probes: SN Ia\, BAO\, WL + GC\, GC 
 counts</a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=745s">[0:12:25] 2024
 : Λ's annus horribilis</a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=908
 s">[0:15:08] The DES SN Y5 sample</a>\n\n<a href="https://youtu.be/ukMQgHj
 6NMI?t=1155s">[0:19:15] DES SN Systematics</a>\n\n<a href="https://youtu.b
 e/ukMQgHj6NMI?t=1357s">[0:22:37] DES Y6 BAO</a>\n\n<a href="https://youtu.
 be/ukMQgHj6NMI?t=1858s">[0:30:58] Galaxy clustering: BAO signal</a>\n\n<a 
 href="https://youtu.be/ukMQgHj6NMI?t=2132s">[0:35:32] Combining SN and BAO
 : expansion history model</a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=2
 291s">[0:38:11] DES BAO + SN + ΛCDM + θₛ: tensions</a>\n\n<a href="htt
 ps://youtu.be/ukMQgHj6NMI?t=2460s">[0:41:00] Curvature: kΛCDM</a>\n\n<a h
 ref="https://youtu.be/ukMQgHj6NMI?t=2725s">[0:45:25] DES expansion models:
  wCDM and w0waCDM</a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=3564s">[0
 :54:24] Hubble tension is not resolved</a>\n\n<a href="https://youtu.be/uk
 MQgHj6NMI?t=3758s">[1:02:38] Results in νΛCDM</a>\n\n<a href="https://yo
 utu.be/ukMQgHj6NMI?t=3967s">[1:06:07] Where to next? Future of DES</a>\n\n
 <a href="https://youtu.be/ukMQgHj6NMI?t=4070s">[1:07:50] Future of BAO</a>
 \n\n<a href="https://youtu.be/ukMQgHj6NMI?t=4162s">[1:09:22] Future of SN<
 /a>\n\n<a href="https://youtu.be/ukMQgHj6NMI?t=4345s">[1:12:55] What curre
 nt cosmology work is underappreciated by the community?</a>\n\n<a href="ht
 tps://youtu.be/ukMQgHj6NMI?t=4420s">[1:13:40] Impact of DES SN-Dovekie</a>
 \n
LOCATION:https://researchseminars.org/talk/CosmologyTalks/101/
END:VEVENT
END:VCALENDAR
