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We establish a tight upper bound for the difference in von Neumann entropies between two quantum states, ₁ and ₂. This bound is expressed in terms of the von Neumann entropies of the mutually orthogonal states derived from the Jordan-Hahn decomposition of the difference operator (₁ - ₂). This yields a novel entropic inequality that implies the well-known Audenaert-Fannes inequality. We employ this inequality to obtain a uniform continuity bound for the quantum conditional entropy of two states whose marginals on the conditioning system coincide. We additionally use it to derive a continuity bound for the quantum relative entropy in both variables. Our proofs are largely based on majorization theory and convex optimization.
Audenaert et al. (Tue,) studied this question.