quantum algorithms:
In the context of holography/AdS-CFT duality and holographic entanglement entropy, by an entanglement wedge one refers (since HHLR 2014) to a subspace of the bulk spacetime which is the holographic dual of a given subspace of the asymptotic boundary.
Concretely, the entanglement wedge of is the causal hull of the homology surface of , hence the maximal globally hyperbolic spacetime whose Cauchy surface is the homology surface of . (Here, the homology surface of is the minimal area bulk region whose boundary is the union of with its Ryu-Takayanagi surface.)
Closely related to but crucially different from the entanglement wedge is the causal wedge of , which is the intersection of the causal future and past of inside the bulk. In contrast to the entanglement wedge, the causal wedge is generally not globally hyperbolic (cf. Rangamani & Takayanagi 2017 §9.2.2).
The notion was introduced in:
and the term “entanglement wedge” was coined in:
The entanglement wedge reconstruction property was more comprehensively argued in:
Xi Dong, Daniel Harlow, Aron C. Wall: Reconstruction of Bulk Operators within the Entanglement Wedge in Gauge-Gravity Duality, Phys. Rev. Lett. 117 021601 (2016) [doi:10.1103/PhysRevLett.117.021601, arXiv:1601.05416]
Daniel L. Jafferis, Aitor Lewkowycz, Juan Maldacena, S. Josephine Suh: Relative entropy equals bulk relative entropy, J. High Energ. Phys. 2016 4 (2016) [doi:10.1007/JHEP06(2016)004, arXiv:1512.06431]
Review:
Created on April 4, 2026 at 20:07:14. See the history of this page for a list of all contributions to it.