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SUMMARY:Mark M. Wilde (Louisiana State University\, USA)
DTSTART:20210120T130000Z
DTEND:20210120T140000Z
DTSTAMP:20260423T052831Z
UID:FAOT/4
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/FAOT/4/">α-
 Logarithmic negativity</a>\nby Mark M. Wilde (Louisiana State University\,
  USA) as part of Functional Analysis and Operator Theory Webinar\n\n\nAbst
 ract\nThe logarithmic negativity of a bipartite quantum state is a widely 
 employed entanglement measure in quantum information theory\, due to the f
 act that it is easy to compute and serves as an upper bound on distillable
  entanglement. More recently\, the $\\kappa$-entanglement of a bipartite s
 tate was shown to be the first entanglement measure that is both easily co
 mputable and has a precise information-theoretic meaning\, being equal to 
 the exact entanglement cost of a bipartite quantum state when the free ope
 rations are those that completely preserve the positivity of the partial t
 ranspose [Wang and Wilde\, Phys. Rev. Lett. 125(4):040502\, July 2020]. \n
 \nIn this talk\, we discuss a non-trivial link between these two entanglem
 ent measures\, by showing that they are the extremes of an ordered family 
 of $\\alpha$-logarithmic negativity entanglement measures\, each of which 
 is identified by a parameter $\\alpha\\in[1\,\\infty]$. In this family\, t
 he original logarithmic negativity is recovered as the smallest with $\\al
 pha=1$\, and the $\\kappa$-entanglement is recovered as the largest with $
 \\alpha=\\infty$. We prove that the $\\alpha$-logarithmic negativity satis
 fies the following properties: entanglement monotone\, normalization\, fai
 thfulness\, and subadditivity. We also prove that it is neither convex nor
  monogamous. Finally\, we define the $\\alpha$-logarithmic negativity of a
  quantum channel as a generalization of the notion for quantum states\, an
 d we show how to generalize many of the concepts to arbitrary resource the
 ories.\n
LOCATION:https://researchseminars.org/talk/FAOT/4/
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