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SUMMARY:Thomas Barthel (Duke)
DTSTART:20201116T190000Z
DTEND:20201116T200000Z
DTSTAMP:20260423T023009Z
UID:UKYhepth/20
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/UKYhepth/20/
 ">Entanglement entropy of energy eigenstates follows a universal scaling f
 unction</a>\nby Thomas Barthel (Duke) as part of Theoretical Physics Semin
 ars (Kentucky)\n\n\nAbstract\nWe consider the entanglement entropies of en
 ergy eigenstates in quantum many-\nbody systems. For the typical models th
 at allow for a field-theoretical\ndescription of the long-range physics\, 
 we find that the entanglement entropy of\n(almost) all eigenstates is desc
 ribed by a single scaling function. This is\npredicated on the validity of
  the weak or strong eigenstate thermalization\nhypothesis (ETH)\, which th
 en implies that the scaling functions can be deduced\nfrom subsystem entro
 pies of thermal ensembles. The scaling functions describe\nthe full crosso
 ver from the groundstate entanglement regime for low energies\nand small s
 ubsystem size (area or log-area law) to the extensive volume-law\nregime f
 or high energies or large subsystem size. For critical 1d systems\, the\ns
 caling function follows from conformal field theory (CFT). We use it to al
 so\ndeduce the scaling function for Fermi liquids in d>1 dimensions. These
 \nanalytical results are complemented by numerics for large non-interactin
 g\nsystems of fermions in d=1\,2\,3 and the harmonic lattice model in d=1\
 ,2.\nLastly\, we demonstrate ETH for entanglement entropies and the validi
 ty of the\nscaling arguments in integrable and non-integrable interacting 
 spin chains. In\nparticular\, we analyze the XXZ and transverse-field Isin
 g models with and\nwithout next-nearest-neighbor interactions.\n\nReferenc
 es: arXiv:1905.07760\, arXiv:1912.10045\, arXiv:2010.07265\n
LOCATION:https://researchseminars.org/talk/UKYhepth/20/
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