1991
DOI: 10.1007/bf02100287
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The proper formula for relative entropy and its asymptotics in quantum probability

Abstract: Umegaki's relative entropy S(ω,φ) = TrD ω (\ogD ω -\ogD φ ) (of states ω and φ with density operators D ω and D φ , respectively) is shown to be an asymptotic exponent considered from the quantum hypothesis testing viewpoint. It is also proved that some other versions of the relative entropy give rise to the same asymptotics as Umegaki's one. As a byproduct, the inequality ΎT A log AB is obtained for positive definite matrices A and B.

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Cited by 420 publications
(299 citation statements)
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“…This was conjectured already in Hiai/Petz [3] and proved for the case that both states are product (i.i.d.) states by Ogawa and Nagaoka in [4].…”
Section: Introductionmentioning
confidence: 56%
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“…This was conjectured already in Hiai/Petz [3] and proved for the case that both states are product (i.i.d.) states by Ogawa and Nagaoka in [4].…”
Section: Introductionmentioning
confidence: 56%
“…An important ingredient in our proof of the Theorem 2.1 is a result proved by Hiai and Petz in [3]. The starting point is the spectral decomposition of the density operator D ϕ (1) corresponding to the state ϕ (1) on A:…”
Section: For Each G L -Ergodic State ψ X In the Convex Decomposition mentioning
confidence: 99%
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“…Indeed, by the contractivity of the trace distance under quantum operations (compare Thm. 9.2 in [29]) and by assumption (17), it holds…”
Section: Be a Subset Of One-dimensional Mutually Orthogonal Projectiomentioning
confidence: 92%
“…The quantum extension of the Shannon-McMillan Theorem was first obtained in [19] for Bernoulli sources, then a partial assertion was obtained for the restricted class of completely ergodic sources in [17], and finally in [7], a complete quantum extension was shown for general ergodic sources. The latter result is based on the construction of subspaces of dimension close to 2 ns , being typical for the source, in the sense that for sufficiently large block length n, their corresponding orthogonal projectors have an expectation value arbitrarily close to 1 with respect to the state of the quantum source.…”
Section: Introductionmentioning
confidence: 99%