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SUMMARY:Monika Aidelsburger (LMU Munich)
DTSTART:20210303T181500Z
DTEND:20210303T194500Z
DTSTAMP:20260423T035909Z
UID:VSFLRC/8
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/VSFLRC/8/">U
 ltracold atoms in optical lattices out-of-equilibrium</a>\nby Monika Aidel
 sburger (LMU Munich) as part of VSF Long Range Colloquium\n\n\nAbstract\nW
 ell-controlled synthetic quantum systems\, such as ultracold atoms in opti
 cal lattices\, offer intriguing possibilities to study complex many-body p
 roblems relevant to a variety of research areas\, ranging from condensed m
 atter to high-energy physics. In particular\, out-of-equilibrium phenomena
  constitute natural applications of quantum simulators\, which have alread
 y successfully demonstrated simulations in regimes that are beyond reach u
 sing state-of-the-art numerical techniques.\nThis enables us to shed new l
 ight on fundamental questions about the thermalization of isolated quantum
  many-body systems. While generic models are expected to thermalize accord
 ing to the eigenstate thermalization hypothesis (ETH)\, violation of ETH i
 s believed to occur mainly in two types of systems: integrable models and 
 many-body localized systems. In between these two extreme limits there is\
 , however\, a whole range of models that exhibit more complex dynamics\, f
 or instance\, due to an emergent fragmentation of the Hilbert space into m
 any dynamically disconnected subspaces. Here\, we realize such a model by 
 implementing the 1D Fermi-Hubbard model with a strong linear potential [1]
  and observe strong initial-state dependent thermalization - a smoking-gun
  signature of Hilbert-space fragmentation.\nEngineering quantum systems ou
 t-of-equilibrium\, on the other hand\, further can be used as a tool to en
 gineer novel quantum phases of matter\, which cannot be accessed in static
  realizations. To this end\, the system’s parameters are varied periodic
 ally\, a method commonly known as Floquet engineering [2]. This facilitate
 d the realization of paradigmatic topological lattice models and recently 
 inspired ideas for implementing Z2 lattice gauge theories [3]. The rich pr
 operties of topological Floquet systems\, however\, transcend those of the
 ir static counterparts\, resulting in a generalized bulk-edge corresponden
 ce. As a consequence\, topological edge modes can exist even in situations
  where the bulk bands have zero Chern numbers. The novel properties of suc
 h anomalous Floquet systems open the door to exciting new non- equilibrium
  many-body phases without any static analogue [4].\n\n[1] S. Scherg et al.
 \, arXiv:2010.12965 (2020)\n[2] A. Eckardt\, Phys. Mod. Phys. 89\, 311 (20
 17)\n[3] C. Schweizer et al.\, Nat. Phys. 15\, 1168-1173 (2019)\n[4] K. Wi
 ntersperger et al.\, Nature Physics 16\, 1058-1063 (2020)\n
LOCATION:https://researchseminars.org/talk/VSFLRC/8/
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