Abstract

We consider the minimal area of the entanglement wedge cross section (EWCS) in Einstein gravity. In the context of holography, it is proposed that this quantity is dual to different information measures, e.g., entanglement of purification, logarithmic negativity and reflected entropy. Motivated by these proposals, we examine in detail the low and high temperature corrections to this quantity and show that it obeys the area law even in the finite temperature. We also study EWCS in nonrelativistic field theories with nontrivial Lifshitz and hyperscaling violating exponents. The resultant EWCS is an increasing function of the dynamical exponent due to the enhancement of spatial correlations between subregions for larger values of z. We find that EWCS is monotonically decreasing as the hyperscaling violating exponent increases. We also obtain this quantity for an entangling region with singular boundary in a three dimensional field theory and find a universal contribution where the coefficient depends on the central charge. Finally, we verify that for higher dimensional singular regions the corresponding EWCS obeys the area law.

Highlights

  • In particular when the entangling region is made by two disjoint spatial components, an important quantity to study is the holographic mutual information (HMI) given as follows1

  • We examine in detail the low and high temperature corrections to this quantity and show that it obeys the area law even in the finite temperature

  • In this paper, we focus on another concept that has recently entered this discussion which is the minimal area of the entanglement wedge cross section (EWCS) and on its conjectured holographic duals [13,14,15,16,17]

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Summary

EWCS at finite temperature in relativistic theories

We study the finite temperature contribution to the EW for holographic theories dual to Einstein gravity. We begin by reviewing the calculation of the finite temperature corrections to HEE and HMI using a systematic expansion, which was originally performed in [33, 34].4. The bulk geometry will be a (d + 2)-dimensional AdS black brane in Poincare coordinates ds. Where r0 is the horizon radius and L is the AdS radius.

Low and high temperature behavior of HEE and HMI
Low and high temperature behavior of EWCS
EWCS in theories with lifshitz scaling and hyperscaling violation
Corner contributions to EWCS
EWCS for a Union of Kinks in AdS4
Conclusions and disscusions
A Thermal corrections to HEE and HMI in nonrelativistic theories
Full Text
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