论文标题
具有有限尺寸环境的催化转化:冷却和温度法应用
Catalytic transformations with finite-size environments: applications to cooling and thermometry
论文作者
论文摘要
热力学定律通常是在无限大环境的假设下制定的。尽管这种理想化有助于理论治疗,但实际的物理系统始终是有限的,其相互作用范围是有限的。这些限制对重要任务(例如冷却,而不是由热力学的第二定律捕获)有后果。在这里,我们研究了系统专门与有限环境相互作用时无法实现的催化转化。我们的核心结果包括针对这些转换的建设性条件,其中包括相应的全球统一操作和所有相关系统的明确状态。从此结果,我们提出了有关使用催化剂进行冷却的各种发现。首先,我们表明,如果催化剂的尺寸足够大,催化冷却始终是可能的。特别是,使用热量量子线冷却量子,可以用小至三级系统的催化剂最大化。我们还确定了在没有催化剂的情况下实施的任务的催化增强功能。例如,我们发现在多Qubit Setup催化冷却中,基于三体相互作用的催化冷却优于标准(非催化)冷却,使用高阶相互作用。在温度计方案中说明了另一个优点,其中使用量子探测环境的温度。在这种情况下,我们表明催化剂允许仅使用探针实现的最佳温度估计。
The laws of thermodynamics are usually formulated under the assumption of infinitely large environments. While this idealization facilitates theoretical treatments, real physical systems are always finite and their interaction range is limited. These constraints have consequences for important tasks such as cooling, not directly captured by the second law of thermodynamics. Here, we study catalytic transformations that cannot be achieved when a system exclusively interacts with a finite environment. Our core result consists of constructive conditions for these transformations, which include the corresponding global unitary operation and the explicit states of all the systems involved. From this result we present various findings regarding the use of catalysts for cooling. First, we show that catalytic cooling is always possible if the dimension of the catalyst is sufficiently large. In particular, the cooling of a qubit using a hot qubit can be maximized with a catalyst as small as a three-level system. We also identify catalytic enhancements for tasks whose implementation is possible without a catalyst. For example, we find that in a multiqubit setup catalytic cooling based on a three-body interaction outperforms standard (non-catalytic) cooling using higher order interactions. Another advantage is illustrated in a thermometry scenario, where a qubit is employed to probe the temperature of the environment. In this case, we show that a catalyst allows to surpass the optimal temperature estimation attained only with the probe.