<p>In holography, the boundary entanglement structure is believed to be encoded in the bulk geometry. In this work, we investigate the precise correspondence between the boundary real-space entanglement and the bulk geometry. By the boundary real-space entanglement, we refer to the conditional mutual information (CMI) for two infinitesimal subsystems separated by a distance <i>l</i>, and the corresponding bulk geometry is at a radial position <i>z</i><sub>*</sub>, namely the turning point of the entanglement wedge for a boundary region with a length scale <i>l</i>. In a generic geometry described by a given coordinate system, <i>z</i><sub>*</sub> can be determined locally by <i>l</i>, while the exact expression for <i>z</i><sub>*</sub>(<i>l</i>) depends on the gauge choice, reflecting the inherent nonlocality of this seemingly local correspondence. We propose to specify the function <i>z</i><sub>*</sub>(<i>l</i>) as the criterion for a gauge choice, and with the specified gauge function, we verify the exact correspondence between the boundary real-space entanglement and the bulk geometry. Inspired by this correspondence, we propose a new method of bulk metric reconstruction from boundary entanglement data, namely the CMI reconstruction. In this CMI proposal, with the gauge fixed a priori by specifying <i>z</i><sub>*</sub>(<i>l</i>), the bulk metric can be reconstructed from the relation between the bulk geometry and the boundary CMI. The CMI reconstruction method establishes a connection between the differential entropy prescription and Bilson’s general algorithm for metric reconstruction.</p>

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Holographic geometry/real-space entanglement correspondence and metric reconstruction

  • Xuanting Ji,
  • Xin-Xiang Ju,
  • Ya-Wen Sun,
  • Yuan-Tai Wang,
  • He-Lin Zhou

摘要

In holography, the boundary entanglement structure is believed to be encoded in the bulk geometry. In this work, we investigate the precise correspondence between the boundary real-space entanglement and the bulk geometry. By the boundary real-space entanglement, we refer to the conditional mutual information (CMI) for two infinitesimal subsystems separated by a distance l, and the corresponding bulk geometry is at a radial position z*, namely the turning point of the entanglement wedge for a boundary region with a length scale l. In a generic geometry described by a given coordinate system, z* can be determined locally by l, while the exact expression for z*(l) depends on the gauge choice, reflecting the inherent nonlocality of this seemingly local correspondence. We propose to specify the function z*(l) as the criterion for a gauge choice, and with the specified gauge function, we verify the exact correspondence between the boundary real-space entanglement and the bulk geometry. Inspired by this correspondence, we propose a new method of bulk metric reconstruction from boundary entanglement data, namely the CMI reconstruction. In this CMI proposal, with the gauge fixed a priori by specifying z*(l), the bulk metric can be reconstructed from the relation between the bulk geometry and the boundary CMI. The CMI reconstruction method establishes a connection between the differential entropy prescription and Bilson’s general algorithm for metric reconstruction.