论文标题
非马克维亚对量子奥托发动机的影响: - 系统 - 库 - 库库相互作用 -
Non-Markovian effect on quantum Otto engine: -Role of system--reservoir interaction-
论文作者
论文摘要
我们研究量子奥托发动机的极限周期,每个循环都由两个有限的量子等量子(加热或冷却)过程和两个量子绝热的工作提取过程。考虑到一个两级系统是一种工作物质,与包括无限数量的玻色子组成的两个储层相互作用,我们研究了非马克维亚效应(量子相位过程中降低动力学的短期行为(QIPS)在无限重复后工作提取的量子动力学(QIPS)。我们专注于参数区域,在该参数区域中,能量转移到储层可以以短期制度返回系统,我们将其称为能量回流以显示部分量子力学可逆性。作为一种与宏观热力学完全不同的情况,我们发现相互作用能量是有限的,并且通过通过全计数统计量来评估QIP期间储层的平均能量变化,这是有限的,而相互作用的能量是有限的,与两点测量相对应。该功能使我们得出以下发现:(1)Carnot定理与包括相互作用能量在内的工作的定义一致,尽管不包括相互作用的工作的常用定义导致与热力学定律发生严重冲突,并且(2)能量回流可以增加工作提取。我们的发现表明,我们需要注意设计在有限时间内操作的量子奥托引擎时的相互作用能量,这要求我们包括非马克维亚效应,即使系统 - 库库相互作用很弱。
We study a limit cycle of a quantum Otto engine whose each cycle consists of two finite-time quantum isochoric (heating or cooling) processes and two quantum adiabatic work-extracting processes. Considering a two-level system as a working substance that weakly interacts with two reservoirs comprising an infinite number of bosons, we investigate the non-Markovian effect (short-time behavior of the reduced dynamics in the quantum isochoric processes (QIPs)) on work extraction after infinite repetition of the cycles. We focus on the parameter region where energy transferred to the reservoir can come back to the system in a short-time regime, which we call energy backflow to show partial quantum-mechanical reversibility. As a situation completely different from macroscopic thermodynamics, we find that the interaction energy is finite and negative by evaluating the average energy change of the reservoir during the QIPs by means of the full-counting statistics, corresponding to the two-point measurements. The feature leads us to the following findings: (1) the Carnot theorem is consistent with a definition of work including the interaction energy, although the commonly used definition of work excluding the interaction leads to a serious conflict with the thermodynamic law, and (2) the energy backflow can increase the work extraction. Our findings show that we need to pay attention to the interaction energy in designing a quantum Otto engine operated in a finite time, which requires us to include the non-Markovian effect, even when the system-reservoir interaction is weak.