Timelike and gravitational anomalous entanglement from the inner horizon
In the context of the AdS$_3$/CFT$_2$, the boundary causal development and the entanglement wedge of any boundary spacelike interval can be mapped to a thermal CFT$_2$ and a Rindler $\widetilde{\text{AdS}_3}$ respectively via certain boundary and bulk Rindler transformations. Nevertheless, the Rindl...
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Zusammenfassung: | In the context of the AdS$_3$/CFT$_2$, the boundary causal development and
the entanglement wedge of any boundary spacelike interval can be mapped to a
thermal CFT$_2$ and a Rindler $\widetilde{\text{AdS}_3}$ respectively via
certain boundary and bulk Rindler transformations. Nevertheless, the Rindler
mapping is not confined in the entanglement wedges. While the outer horizon of
the Rindler $\widetilde{\text{AdS}_3}$ is mapped to the RT surface, we also
identify the pre-image of the inner horizon in the original AdS$_3$, which we
call the inner RT surface. In this paper we give some new physical
interpretation for the inner RT surface. First, the inner RT surface breaks
into two pieces which anchor on the two tips of the causal development.
Furthermore, we can take the two tips as the endpoints of a certain timelike
interval and the inner RT surface is exactly the spacelike geodesic that
represents the real part of the so-called holographic timelike entanglement
entropy (HTEE). We also identify a timelike geodesic at boundary of the
extended entanglement wedge, which represents the imaginary part of the HTEE.
Second, in the duality between the topological massive gravity (TMG) and
gravitational anomalous CFT$_2$, the entanglement entropy and the mixed state
correlation that is dual to the entanglement wedge cross section (EWCS) receive
correction from the Chern-Simons term in the TMG. We find that, the correction
to the holographic entanglement entropy can be reproduced by the area of the
inner RT surface with a proper regulation, while the mixed state correlation
can be represented by the saddle geodesic chord connecting the two pieces of
the inner RT surface of the mixed state we consider, which we call the inner
EWCS. The equivalence between the twist on the RT surface and the length of
inner RT surface is also discussed. |
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DOI: | 10.48550/arxiv.2412.21058 |