Entanglement wedge reconstruction using the Petz map
Chi-Fang Chen (Department of Physics, Stanford University, Stanford, CA, 94305, USA, Institute for Quantum Information and Matter, Caltech, Pasadena, CA, 91125, USA)
; Geoffrey Penington (Stanford Institute for Theoretical Physics, Stanford University, Stanford, CA, 94305, USA); Grant Salton (Department of Physics, Stanford University, Stanford, CA, 94305, USA, Institute for Quantum Information and Matter, Caltech, Pasadena, CA, 91125, USA, Stanford Institute for Theoretical Physics, Stanford University, Stanford, CA, 94305, USA)
At the heart of recent progress in AdS/CFT is the question of subregion duality, or entanglement wedge reconstruction: which part(s) of the boundary CFT are dual to a given subregion of the bulk? This question can be answered by appealing to the quantum error correcting properties of holography, and it was recently shown that robust bulk (entanglement wedge) reconstruction can be achieved using a universal recovery channel known as the . In short, one can use the twirled Petz map to recover bulk data from a subset of the boundary. However, this map involves an averaging procedure over bulk and boundary modular time, and hence it can be somewhat intractable to evaluate in practice. We show that a much simpler channel, the Petz map, is sufficient for entanglement wedge reconstruction for any code space of fixed finite dimension — no twirling is required. Moreover, the error in the reconstruction will always be non-perturbatively small. From a quantum information perspective, we prove a general theorem extending the use of the Petz map as a general-purpose recovery channel to subsystem and operator algebra quantum error correction.
