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Boundary mutual information in double holography

High Energy Physics - Theory 2026-02-16 v1 Strongly Correlated Electrons General Relativity and Quantum Cosmology Quantum Physics

Abstract

We consider a composite system where AdS3_3 gravity is coupled to a flat heat bath and investigate the mutual information between two subregions on the intersection of the AdS3_3 and bath, referred to as the boundary mutual information (BMI). The corresponding entanglement entropy is captured via quantum extremal surfaces (QES), which holographically be computed by a surface optimization algorithm based on ``Surface Evolver''. We focus on both connected and disconnected configurations of the quantum entanglement wedge (Q-EW) in the AdS3_3 bulk and analyze the finite corrections to the BMI. Our numerical results reveal a phase transition of the BMI as the separation between two subregions increases. Furthermore, we find that the BMI can naturally be decomposed into two distinct components: a geometric term arising from the areas of the quantum extremal surfaces, and a correction term resulting from bulk quantum fields within the Q-EW. Interestingly, the geometric contribution always exceeds the total BMI, indicating a negative correction from the bulk matter fields. This negativity can be understood as the result of subtracting a greater contribution from quantum fields in the connected Q-EW than in the disconnected one. We also reproduce the negative contribution of bulk quantum fields to BMI within a random tensor network (RTN) toy model of double holography. Modeling the bulk as a highly mixed state entangled with a large bath leads to a volume-law bulk entropy. In the large bond-dimension limit, the geometric part of the BMI remains non-negative, while the bulk entropy contribution becomes non-positive when the Q-EWs merge.

Keywords

Cite

@article{arxiv.2602.12627,
  title  = {Boundary mutual information in double holography},
  author = {Yuxuan Liu and Yi Ling and Zhuo-Yu Xian},
  journal= {arXiv preprint arXiv:2602.12627},
  year   = {2026}
}
R2 v1 2026-07-01T10:34:50.575Z