Maximum and minimum entropy states yielding local continuity bounds
arXiv:1706.02212 · doi:10.1063/1.5000120
Abstract
Given an arbitrary quantum state (), we obtain an explicit construction of a state (resp. ) which has the maximum (resp. minimum) entropy among all states which lie in a specified neighbourhood (-ball) of . Computing the entropy of these states leads to a local strengthening of the continuity bound of the von Neumann entropy, i.e., the Audenaert-Fannes inequality. Our bound is local in the sense that it depends on the spectrum of . The states and depend only on the geometry of the -ball and are in fact optimizers for a larger class of entropies. These include the Rényi entropy and the min- and max- entropies. This allows us to obtain local continuity bounds for these quantities as well. In obtaining this bound, we first derive a more general result which may be of independent interest, namely a necessary and sufficient condition under which a state maximizes a concave and Gâteaux-differentiable function in an -ball around a given state . Examples of such a function include the von Neumann entropy, and the conditional entropy of bipartite states. Our proofs employ tools from the theory of convex optimization under non-differentiable constraints, in particular Fermat's Rule, and majorization theory.
38 pages; v2: added an application, streamlined proofs of Lem. 6.8-6.11, corrected typos, corrected figure 1, updated the style of figure 2
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