论文标题
熵连续性界限并最终纠缠破裂的频道
Entropic Continuity Bounds & Eventually Entanglement-Breaking Channels
论文作者
论文摘要
在本文的第一部分中,我们提出了一种通用技术,用于建立Schur凹入函数的局部和统一连续性界限。我们的技术使用量子状态之间的主要关系与痕量距离之间的特定关系。也就是说,在此距离内,多数化预订至少超过$ε$。通过追踪大型少量器的路径是距离$ε$的函数,我们获得了“多数化流程”的路径。这产生了通用框架中为von Neumann熵绑定的Audenaert-Fannes连续性的新证明,该框架延伸到其他功能,包括$α$-Rényi熵,在此情况下,我们获得了新的界限。我们将此技术应用于其他Schur凹面函数,例如某个随机图模型的连接组件的数量以及随机变量的不同实现的数量。 在第二部分中,我们考虑重复的相互作用系统,其中感兴趣系统一次与一系列探针相互作用。我们表征了哪些重复的交互系统破坏了系统和未触及的参考之间的任何最初存在的纠缠。此外,当探针及其与系统的相互作用缓慢变化(即绝热)时,我们分析了Landauer界限的饱和度,系统的熵变化与探针的能量变化之间的不平等,以无限限度的限制倾向于无限量与连续探测器之间的差异之间的差异和互动之间的差异之间的差异。该分析通过两次测量方案以细粒的水平进行,其中探针的能量在每次相互作用之前和之后进行测量。
In the first part of this thesis, we present a general technique for establishing local and uniform continuity bounds for Schur concave functions. Our technique uses a particular relationship between majorization and the trace distance between quantum states. Namely, the majorization pre-order attains a minimum over $ε$-balls in this distance. By tracing the path of the majorization-minimizer as a function of the distance $ε$, we obtain the path of "majorization flow". This yields a new proof of the Audenaert-Fannes continuity bound for the von Neumann entropy in a universal framework which extends to the other functions, including the $α$-Rényi entropy, for which we obtain novel bounds in the case $α> 1$. We apply this technique to other Schur concave functions, such as the number of connected components of a certain random graph model, and the number of distinct realizations of a random variable. In the second part, we consider repeated interaction systems, in which a system of interest interacts with a sequence of probes one at a time. We characterize which repeated interaction systems break any initially-present entanglement between the system and an untouched reference after finitely many steps. Additionally, when the probes and their interactions with the system are slowly-varying (i.e. adiabatic), we analyze the saturation of Landauer's bound, an inequality between the entropy change of the system and the energy change of the probes, in the limit in which the number of steps tends to infinity and both the difference between consecutive probes and the difference between their interactions vanishes. This analysis proceeds at a fine-grained level by means of a two-time measurement protocol, in which the energy of the probes is measured before and after each interaction.