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Mohammed Anber (Lewis & Clark College, Portland)07/11/2019, 09:00
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Mithat Ünsal (NC State U)07/11/2019, 09:55
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Andreas Laeuchli (Innsbruck U)07/11/2019, 11:15
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Bernd Rosenow (Leipzig U)07/11/2019, 12:10
Equilibration of isolated quantum systems has attracted much attention recently. Due to their integrability, one-dimensional systems often equilibrate towards a non-thermal steady state. In coupled quantum Hall edge states, the approach towards such a non-equilibrium steady state can be understood in terms of charge fractionalization, i.e. the decomposition of injected charges into eigenmodes...
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Lukas Janssen (TU Dresden)07/11/2019, 15:00
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Andrei Alexandru (George Washington University)07/11/2019, 16:20
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Camilo Lopez (FSU Jena)07/11/2019, 17:15
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Riccardo Martini (Okinawa Institute if Science and Technology)07/11/2019, 18:00
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Jobst Ziebell (FSU Jena)07/11/2019, 18:00
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Johannes Knaute07/11/2019, 18:00
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Phillip Lakaschus (U Frankfurt)07/11/2019, 18:10
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Jan Mandrysch (Leipzig U)07/11/2019, 18:10
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Elena Mosman (Tomsk PU)07/11/2019, 18:10
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Marc Steinhauser (FSU Jena)07/11/2019, 18:20
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Martin Steil (TU Darmstadt)07/11/2019, 18:20
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Sajid Ali (U Münster)07/11/2019, 18:20
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Michael Mandl (Graz U)07/11/2019, 18:30
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Shouryya Ray (TU Dresden)07/11/2019, 18:30
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Mari-Carmen Bañuls (MPQ München)08/11/2019, 09:00
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Esperanza Lopez08/11/2019, 09:55
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Stefano Carignano (Barcelona U)08/11/2019, 11:15
In the past few years a growing consensus has been building around the idea that a spatially inhomogeneous chiral condensate may form in dense quark matter. In this talk, I will give a brief historical overview and review some recent developments on the characterization of such crystalline condensates using effective models for describing of QCD at finite density.
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Tomas Brauner08/11/2019, 12:10
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Andreas Schmitt (Southampton U)08/11/2019, 15:00
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Sean Gray (FSU Jena)08/11/2019, 16:20
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Julian Lenz (FSU Jena)08/11/2019, 16:55
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Sylvain Carrozza (Perimeter Institute, Waterloo)09/11/2019, 09:00
I will summarize the structure and scope of the so-called melonic large N expansion, which typically governs the large N behaviour of theories involving higher rank tensors. Compared to vector and matrix theories, What distinguishes it from the large N expansions of vector or matrix theories is that it is dominated by a non-trivial family of Feynman diagrams -- the melon diagrams -- which...
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Tamaz Khunjua (Lomonosov Moscow State U)09/11/2019, 09:55
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Marc Wagner (Frankfurt U)09/11/2019, 11:15
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Jens Braun (TU Darmstadt)09/11/2019, 12:10
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