Entanglement wedge cross-section for noncommutative Yang-Mills theory

Abstract

The signature of noncommutativity on various measures of entanglement has been observed by considering the holographic dual of noncommutative super Yang-Mills theory. We have followed a systematic analytical approach in order to compute the holographic entanglement entropy corresponding to a strip like subsystem of length l. The relationship between the subsystem size (in dimensionless form) $$ \frac{l}{a} $$ l a and the turning point (in dimensionless form) introduces a critical length scale $$ \frac{l_c}{a} $$ l c a which leads to three domains in the theory, namely, the deep UV domain (l < lc; aut » 1, aut ∼ aub), deep noncommutative domain (l > lc, aub> aut » 1) and deep IR domain (l > lc, aut « 1). This in turn means that the length scale lc distinctly points out the UV/IR mixing property of the non-local theory under consideration. We have carried out the holographic study of entanglement entropy for each of these domains by employing both analytical and numerical techniques. The broken Lorentz symmetry induced by noncommutativity has motivated us to redefine the entropic c-function. We have obtained the noncommutative correction to the c-function upto leading order in the noncommutative parameter. We have also looked at the behaviour of this quantity over all the domains of the theory. We then move on to compute the minimal cross-section area of the entanglement wedge by considering two dis- joint subsystems A and B. On the basis of EP = EW duality, this leads to the holographic computation of the entanglement of purification. The correlation between two subsystems, namely, the holographic mutual information I(A : B) has also been computed. Moreover, the computations of EW and I(A : B) has been done for each of the domains in the theory. We have then briefly discussed the effect of the UV cut-off on the IR behaviours of these quantities. Finally, we consider a black hole geometry with a noncommutative parameter and study the influence of both noncommutativity and finite temperature on the various measures of quantum entanglement.

Mixed state information theoretic measures in boosted black brane

“…Upto x = x c , connected phase is the physical whereas beyond x > x c disconnected phase is physical. Some recent works in this direction can be found in [37][38][39][40][41]. In order to compute the critical length x c for the case in hand, we firstly fix the parameters d = 3, l = 3 and z 0 = 10.…”

The mixed-state entanglement in holographic p-wave superconductor model

“…Additionally, various types of mixed-state entanglement, such as reflected entropy, logarithmic negativity, balanced partial entanglement, and odd entropy have been linked to the EWCS in holographic systems [21][22][23][24][25][26]. In conclusion, EWCS is a powerful tool for investigating mixed-state entanglement in strongly coupled field theories [27][28][29][30][31][32][33][34][35][36][37].…”

The role of mutual information in the Page curve

“…We now explain the above proposal from the holographic perspective. We propose that just after the Page time, when the replica wormhole saddle points starts to dominate, the Hawking saddle point (which gives S(R) ∼ t b ), the entanglement wedge of B + ∪ B − makes the transition from connected to disconnected phase [53,55,56] which results in I(B + : B − ) = 0. We now apply our proposal.…”