Entanglement Entropy of Free Fermions with a Random Matrix as a One-Body Hamiltonian
arXiv:2405.11342 · doi:10.3390/e26070564
Abstract
We consider a quantum system of large size and its subsystem of size assuming that is much larger than , which can also be sufficiently large, i.e., . A widely accepted mathematical version of this heuristic inequality is the asymptotic regime of successive limits: first the macroscopic limit , then an asymptotic analysis of the entanglement entropy as . In this paper, we consider another version of the above heuristic inequality: the regime of asymptotically proportional and , i.e., the simultaneous limits . Specifically, we consider the system of free fermions which is in its ground state and such that its one-body Hamiltonian is a large random matrix, that is often used to model the long-range hopping. By using random matrix theory, we show that in this case, the entanglement entropy obeys the volume law known for systems with short-ranged hopping but described either by a mixed state or a pure strongly excited state of the Hamiltonian. We also give a streamlined proof of Page's formula for the entanglement entropy of the black hole radiation for a wide class of typical ground states, thereby proving the universality of the formula.
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