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首页> 外文期刊>Communications in Mathematical Physics >Tight Uniform Continuity Bounds for Quantum Entropies: Conditional Entropy, Relative Entropy Distance and Energy Constraints
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Tight Uniform Continuity Bounds for Quantum Entropies: Conditional Entropy, Relative Entropy Distance and Energy Constraints

机译:量子熵的紧一致连续性界:条件熵,相对熵距离和能量约束

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摘要

We present a bouquet of continuity bounds for quantum entropies, falling broadly into two classes: first, a tight analysis of the Alicki-Fannes continuity bounds for the conditional von Neumann entropy, reaching almost the best possible form that depends only on the system dimension and the trace distance of the states. Almost the same proof can be used to derive similar continuity bounds for the relative entropy distance from a convex set of states or positive operators. As applications, we give new proofs, with tighter bounds, of the asymptotic continuity of the relative entropy of entanglement, E (R) , and its regularization , as well as of the entanglement of formation, E (F) . Using a novel "quantum coupling" of density operators, which may be of independent interest, we extend the latter to an asymptotic continuity bound for the regularized entanglement of formation, aka entanglement cost, . Second, we derive analogous continuity bounds for the von Neumann entropy and conditional entropy in infinite dimensional systems under an energy constraint, most importantly systems of multiple quantum harmonic oscillators. While without an energy bound the entropy is discontinuous, it is well-known to be continuous on states of bounded energy. However, a quantitative statement to that effect seems not to have been known. Here, under some regularity assumptions on the Hamiltonian, we find that, quite intuitively, the Gibbs entropy at the given energy roughly takes the role of the Hilbert space dimension in the finite-dimensional Fannes inequality.
机译:我们提供了一束量子熵的连续边界,大致分为两类:第一,对条件冯·诺依曼熵的Alicki-Fannes连续边界进行严格分析,几乎达到了仅取决于系统维数的最佳形式。状态的跟踪距离。几乎相同的证明可用于从一组凸状态或正算子得出相对熵距离的相似连续性边界。作为应用,我们给出了更严格的界限,证明了纠缠的相对熵E(R)及其正则化的渐近连续性,以及形成的纠缠E(F)。使用密度算符的一种新颖的“量子耦合”,它可能具有独立的意义,我们将后者扩展到一个渐近的连续性边界,用于形成的正则纠缠,也称为纠缠成本。其次,我们在能量约束下,最重要的是多个量子谐波振荡器的系统中,推导了无限维系统中冯·诺伊曼熵和条件熵的相似连续性边界。尽管没有能量限制,熵是不连续的,但是众所周知,熵在能量限制的状态下是连续的。但是,关于这种效果的定量陈述似乎尚不清楚。在此,在关于哈密顿量的一些规律性假设下,我们很直观地发现,在给定能量下的吉布斯熵在有限维Fannes不等式中大致扮演了希尔伯特空间维的角色。

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