Using techniques proposed in [Sason, IEEE Trans. Inf. Th. 59, 7118 (2013)] and [Becker, Datta and Jabbour, IEEE Trans. Inf. Th. 69, 4128 (2023)], and building on results from the latter, we construct a globally optimal continuity bound for the von Neumann entropy under energy constraints imposed by arbitrary Hamiltonians, satisfying the Gibbs hypothesis. In particular, this provides a precise expression for the modulus of continuity of the von Neumann entropy over the set of states with bounded energy for infinite-dimensional quantum systems. Thus, it completely solves the problem of finding an optimal continuity bound for the von Neumann entropy in this setting, which was previously known only for pairs of states which were sufficiently close to each other. This continuity bound follows from a globally optimal semicontinuity bound for the von Neumann entropy under general energy constraints, which is our main technical result.

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