Center for Field Theory and Particle Physics, Department of Physics, Fudan University, Shanghai 200433, China.
Department of Physics, National Cheng Kung University, Tainan 70101, Taiwan.
Phys Rev E. 2018 Jan;97(1-1):012135. doi: 10.1103/PhysRevE.97.012135.
In a series of papers, we intend to take the perspective of open quantum systems and examine from their nonequilibrium dynamics the conditions when the physical quantities, their relations, and the laws of thermodynamics become well defined and viable for quantum many-body systems. We first describe how an open-system nonequilibrium dynamics (ONEq) approach is different from the closed combined system + environment in a global thermal state (CGTs) setup. Only after the open system equilibrates will it be amenable to conventional thermodynamics descriptions, thus quantum thermodynamics (QTD) comes at the end rather than assumed in the beginning. The linkage between the two comes from the reduced density matrix of ONEq in that stage having the same form as that of the system in the CGTs. We see the open-system approach having the advantage of dealing with nonequilibrium processes as many experiments in the near future will call for. Because it spells out the conditions of QTD's existence, it can also aid us in addressing the basic issues in quantum thermodynamics from first principles in a systematic way. We then study one broad class of open quantum systems where the full nonequilibrium dynamics can be solved exactly, that of the quantum Brownian motion of N strongly coupled harmonic oscillators, interacting strongly with a scalar-field environment. In this paper, we focus on the internal energy, heat capacity, and the third law. We show for this class of physical models, amongst other findings, the extensive property of the internal energy, the positivity of the heat capacity, and the validity of the third law from the perspective of the behavior of the heat capacity toward zero temperature. These conclusions obtained from exact solutions and quantitative analysis clearly disprove claims of negative specific heat in such systems and dispel allegations that in such systems the validity of the third law of thermodynamics relies on quantum entanglement. They are conceptually and factually unrelated issues. Entropy and entanglement will be the main theme of our second paper on this subject matter.
在一系列论文中,我们打算从开放量子系统的角度出发,从它们的非平衡动力学出发,研究当物理量、它们的关系和热力学定律变得明确和适用于量子多体系统时的条件。我们首先描述了开放系统非平衡动力学(ONEq)方法与处于全局热态(CGTs)的封闭组合系统+环境有何不同。只有当开放系统达到平衡后,它才能适用于传统的热力学描述,因此量子热力学(QTD)是在最后出现的,而不是在开始时就假设的。两者之间的联系来自于 ONEq 的约化密度矩阵,在那个阶段,它的形式与 CGTs 中的系统相同。我们看到,开放系统方法具有处理非平衡过程的优势,因为未来的许多实验都将需要这种方法。由于它阐明了 QTD 存在的条件,它也可以帮助我们从系统的角度来系统地解决量子热力学的基本问题。然后,我们研究了一类广泛的开放量子系统,其中完整的非平衡动力学可以精确求解,即 N 个强耦合谐振子的量子布朗运动与标量场环境的强相互作用。在本文中,我们重点研究内能、热容和第三定律。我们展示了对于这一类物理模型,除了其他发现之外,内能的广延性质、热容的正定性以及第三定律从热容对零温度的行为的有效性。从精确解和定量分析中得到的这些结论清楚地反驳了在这样的系统中存在负比热的说法,并驳斥了在这样的系统中热力学第三定律的有效性依赖于量子纠缠的说法。它们是概念上和事实上无关的问题。熵和纠缠将是我们关于这个主题的第二篇论文的主要内容。