paper

Bulk-boundary entanglement correspondence and the Ryu-Takayanagi conjecture in an setup

arXiv:2502.01144 · doi:10.1007/JHEP06(2025)195

Abstract

Using recent developments in expressing one-loop partition functions in Euclidean space-times in terms of character integrals, we relate the one-loop effective action for a free field theory in (comprised of a massless scalar field and a massless Majorana fermion field) to the partition function of the de Alfaro-Fubini-Furlan (DFF) conformal quantum mechanics (CQM) models on the two global boundaries. The equal number of bosonic and fermionic degrees in the field theory guarantee that the one-loop calculation is free of all UV divergences except a logarithmic one consistent with the expected entanglement entropy behaviour in a CQM. Via a thermofield double representation, we compute the entanglement entropy between two copies of the (CQM), each living near one of the two boundaries of global , in a state at global time . This entanglement entropy is expressed in terms of the logarithm of the regularised length of a closed particle trajectory infinitesimally near the rim of the Euclidean disc. We view this relation between boundary quantum entanglement and a bulk geometrical quantity as the version of the Ryu-Takayanagi conjecture in our setup. The boundary entanglement entropy is equal to 4 times the thermodynamic entropy read off from the regularised one-loop effective action in . Further, we compute the bulk entanglement entropy associated with black hole horizons in Lorentzian and show that it precisely matches the boundary entanglement entropy.

v2:typographical corrections and assorted improvements; references added, 35 pages and 1 figure,

References in corpus (24)