Built on

D. Marolf, A.C. Wall and Z. Wang, Restricted Maximin surfaces and HRT in generic black hole spacetimes , JHEP 05
Original
1901
Earlier work this paper cites.
S. Dutta and T. Faulkner, A canonical purification for the entanglement wedge cross-section , JHEP 03
Original
1905
Earlier work this paper cites.
Y. Kusuki, J. Kudler-Flam and S. Ryu, Derivation of holographic negativity in AdS 3 /CFT 2 , Phys. Rev. Lett. 123
Original
1907
Earlier work this paper cites.
J.M. Maldacena, The Large N limit of superconformal field theories and supergravity , Int. J. Theor. Phys. 38
1999
Earlier work this paper cites.
M.A. Nielsen and I.L. Chuang, Quantum computation and quantum information , Phys. Today 54
2001
Earlier work this paper cites.
S. Ryu and T. Takayanagi, Holographic derivation of entanglement entropy from AdS/CFT , Phys. Rev. Lett. 96
2006
Earlier work this paper cites.
V.E. Hubeny, M. Rangamani and T. Takayanagi, A Covariant holographic entanglement entropy proposal , JHEP 07
Original
2007
Earlier work this paper cites.
R. Bousso, V. Chandrasekaran, P. Rath and A. Shahbazi-Moghaddam, Gravity dual of Connes cocycle flow , Phys. Rev. D 102
Original
2007
Earlier work this paper cites.
C. Akers and G. Penington, Leading order corrections to the quantum extremal surface prescription , JHEP 04
Original
2008
Earlier work this paper cites.
M. Headrick, Entanglement Renyi entropies in holographic theories , Phys. Rev. D 82
Original
2010
Earlier work this paper cites.
L.-Y. Hung, R.C. Myers, M. Smolkin and A. Yale, Holographic Calculations of Renyi Entropy , JHEP 12
Original
2011
Earlier work this paper cites.
A. Lewkowycz and J. Maldacena, Generalized gravitational entropy , JHEP 08
Original
2013
Earlier work this paper cites.

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2023

Constrained HRT Surfaces and their Entropic Interpretation

Dong, Xi, Marolf, Donald, Rath, Pratik

Understand

Consider two boundary subregions $A$ and $B$ that lie in a common boundary Cauchy surface, and consider also the associated HRT surface $\gamma_B$ for $B$.

In that context, the constrained HRT surface $\gamma_{A:B}$ can be defined as the codimension-2 bulk surface anchored to $A$ that is obtained by a maximin construction restricted to Cauchy slices containing $\gamma_B$.
As a result, $\gamma_{A:B}$ is the union of two pieces, $\gamma^B_{A:B}$ and $\gamma^{\bar B}_{A:B}$ lying respectively in the entanglement wedges of $B$ and its complement $\bar B$.
Unlike the area $\mathcal{A}\left(\gamma_A\right)$ of the HRT surface $\gamma_A$, at least in the semiclassical limit, the area $\mathcal{A}\left(\gamma_{A:B}\right)$ of $\gamma_{A:B}$ commutes with the area $\mathcal{A}\left(\gamma_B\right)$ of $\gamma_B$.