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BEGIN:VEVENT
SUMMARY:Ilkka Mäkinen (University of Warsaw)
DTSTART:20200430T183000Z
DTEND:20200430T193000Z
DTSTAMP:20260422T212709Z
UID:PIQuantumGravity/1
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/PIQuantumGra
 vity/1/">Quantum-reduced loop gravity from the perspective of full LQG</a>
 \nby Ilkka Mäkinen (University of Warsaw) as part of PI Quantum Gravity\n
 \n\nAbstract\nQuantum-reduced loop gravity is a model of loop quantum grav
 ity\, whose characteristic feature is the considerable simplicity of its k
 inematical structure in comparison with that of full loop quantum gravity.
  The model therefore provides an accessible testing ground for probing the
  physical implications of loop quantum gravity. In my talk I will give a b
 rief introduction to quantum-reduced loop gravity\, and examine the relati
 on between the quantum-reduced model and full loop quantum gravity. In par
 ticular\, I will focus on clarifying how the operators of the quantum redu
 ced model are related to those of the full theory. I will show that despit
 e their simplicity\, the operators of the quantum-reduced model are simply
  the operators of the full theory acting on states in the Hilbert space of
  the quantum-reduced model. In order to pass from the full theory operator
 s to the "reduced" operators\, one only has to keep in mind that the state
 s of the quantum-reduced model are labeled with large spins\, and discard 
 terms which are of lower than leading order in j.\n
LOCATION:https://researchseminars.org/talk/PIQuantumGravity/1/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Simone Speziale (Aix Marseille University)
DTSTART:20200514T190000Z
DTEND:20200514T203000Z
DTSTAMP:20260422T212709Z
UID:PIQuantumGravity/2
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/PIQuantumGra
 vity/2/">Asymptotics of the EPRL model on arbitrary vertices</a>\nby Simon
 e Speziale (Aix Marseille University) as part of PI Quantum Gravity\n\n\nA
 bstract\nWe introduce a new technique to study the critical point equation
 s of the eprl model. We show that it correctly reproduces the 4-simplex as
 ymptotics\, and how to apply it to an arbitrary vertex. We find that for g
 eneral vertices\, the asymptotics can be linked to a Regge action for poly
 topes\, but contain also more general geometries\, called conformal twiste
 d geometries. We present explicit examples including the hypercube\, and d
 iscuss implications.\n
LOCATION:https://researchseminars.org/talk/PIQuantumGravity/2/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Thomas Mertens (Universiteit Gent)
DTSTART:20200521T183000Z
DTEND:20200521T193000Z
DTSTAMP:20260422T212709Z
UID:PIQuantumGravity/3
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/PIQuantumGra
 vity/3/">Bulk observables in JT gravity</a>\nby Thomas Mertens (Universite
 it Gent) as part of PI Quantum Gravity\n\n\nAbstract\nUsing a definition o
 f bulk diff-invariant observables\, we go into the bulk of 2d Jackiw-Teite
 lboim gravity. By mapping the computation to a Schwarzian path integral\, 
 we study exact bulk correlation functions and discuss their physical impli
 cations. We describe how the black hole thermal atmosphere gets modified b
 y quantum gravitational corrections. Finally\, we will discuss how higher 
 topological effects further modify the spectral density and detector respo
 nse in the Unruh heat bath.\n
LOCATION:https://researchseminars.org/talk/PIQuantumGravity/3/
END:VEVENT
BEGIN:VEVENT
SUMMARY:Yannick Herfray (Université Libre de Bruxelles)
DTSTART:20200528T183000Z
DTEND:20200528T193000Z
DTSTAMP:20260422T212709Z
UID:PIQuantumGravity/4
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/PIQuantumGra
 vity/4/">Conformal Geometry of Null Infinity\, including gravitational wav
 es</a>\nby Yannick Herfray (Université Libre de Bruxelles) as part of PI 
 Quantum Gravity\n\n\nAbstract\nSince the seminal work of Penrose\, it has 
 been understood that conformal compactifications (or "asymptotic simplicit
 y") is the geometrical framework underlying Bondi-Sachs' description of as
 ymptotically flat space-times as an asymptotic expansion. From this point 
 of view the asymptotic boundary\, a.k.a "null-infinity"\, naturally is a c
 onformal null (i.e degenerate) manifold. In particular\, "Weyl rescaling" 
 of null-infinity should be understood as gauge transformations. As far as 
 gravitational waves are concerned\, it has been well advertised by Ashteka
 r that if one work with a fixed representative for the conformal metric\, 
 gravitational radiations can be neatly parametrized as a choice of "equiva
 lence class of metric-compatible connections". This nice intrinsic descrip
 tion however amounts to working in a fixed gauge and\, what is more\, the 
 presence of equivalence class tend to make this point of view tedious to w
 ork with.\n\nI will review these well-known facts and show how modern meth
 ods in conformal geometry (namely tractor calculus) can be adapted to the 
 degenerate conformal geometry of null-infinity to encode the presence of g
 ravitational waves in a completely geometrical (gauge invariant) way: Asht
 ekar's (equivalence class of) connections are proved to be in 1-1 correspo
 ndence with choices of (genuine) tractor connection\, gravitational radiat
 ion is invariantly described by the tractor curvature and the degeneracy o
 f gravity vacua correspond to the degeneracy of flat tractor connections. 
 The whole construction is fully geometrical and manifestly conformally inv
 ariant."\n
LOCATION:https://researchseminars.org/talk/PIQuantumGravity/4/
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