The paper derives the entanglement entropy of two disjoint intervals in a thermal 2D conformal field theory, identifies its holographic dual as an entanglement wedge cross section in a BTZ black hole, and shows this cross section can cross the horizon in the thermofield double state.
An alternative to purification in CFT
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abstract
In conformal field theories, in contrast to \emph{adding} some auxiliary states into the bipartite mixed state $\rho_{AB}$ as the usual purifications do, we show a pure entangled state $\psi_{AB}$ can be constructed by \emph{subtracting} the undetectable regions. In this pure state $\psi_{AB}$, the von Neumann entropy $S_{\text{vN}}(A)$ naturally captures quantum entanglement between $A$ and $B$. We verify that $S_{\text{vN}}(A)$ is equal to the entanglement wedge cross-section $E_{W}$ in AdS spacetime, which is conjectured to be the holographic dual of the entanglement of purification. We show such constructed entanglement entropy has a phase transition. The ordinary entanglement entropies of critical and non-critical QFTs are simply limits of the two phases.
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Entanglement Entropy of Mixed State in Thermal CFT$_2$
The paper derives the entanglement entropy of two disjoint intervals in a thermal 2D conformal field theory, identifies its holographic dual as an entanglement wedge cross section in a BTZ black hole, and shows this cross section can cross the horizon in the thermofield double state.