Quantum thermalization and average entropy of a subsystem
arXiv:2506.19896 · doi:10.1016/j.physleta.2025.131000
Abstract
Page's seminal result on the average von Neumann (VN) entropy does not immediately apply to realistic many-body systems which are restricted to physically relevant smaller subspaces. We investigate here the VN entropy averaged over the pure states in the subspace corresponding to a narrow energy shell centered at energy . We find that the average entropy is , where represents first subsystem's effective number of states relevant to the energy scale . If and () is the Hilbert space dimension of the full system (first subsystem), we estimate that , where for nonintegrable (chaotic) systems and for integrable systems. This result can be reinterpreted as a volume-law of entropy, where the volume-law coefficient depends on the density-of-states for nonintegrable systems, and remains below the maximal possible value for integrable systems. We numerically analyze a spin model to substantiate our main results.
9 pages, 3 figures; final version
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