NEST, Scuola Normale Superiore and Istituto Nanoscienze-CNR, I-56126 Pisa, Italy.
Sci Rep. 2016 Jul 5;6:29282. doi: 10.1038/srep29282.
According to the second law of thermodynamics, for every transformation performed on a system which is in contact with an environment of fixed temperature, the average extracted work is bounded by the decrease of the free energy of the system. However, in a single realization of a generic process, the extracted work is subject to statistical fluctuations which may allow for probabilistic violations of the previous bound. We are interested in enhancing this effect, i.e. we look for thermodynamic processes that maximize the probability of extracting work above a given arbitrary threshold. For any process obeying the Jarzynski identity, we determine an upper bound for the work extraction probability that depends also on the minimum amount of work that we are willing to extract in case of failure, or on the average work we wish to extract from the system. Then we show that this bound can be saturated within the thermodynamic formalism of quantum discrete processes composed by sequences of unitary quenches and complete thermalizations. We explicitly determine the optimal protocol which is given by two quasi-static isothermal transformations separated by a finite unitary quench.
根据热力学第二定律,对于与固定温度环境接触的系统进行的每一次变换,平均提取的功都受到系统自由能减少的限制。然而,在一般过程的单次实现中,提取的功受到统计波动的影响,这可能导致对先前界限的概率违反。我们感兴趣的是增强这种效果,即我们寻找最大程度地提高超过给定任意阈值的功提取概率的热力学过程。对于任何服从雅可比等式的过程,我们确定了功提取概率的上限,该上限还取决于我们在失败情况下愿意提取的最小功量,或者取决于我们希望从系统中提取的平均功量。然后,我们表明,在由单位淬火和完全热化组成的量子离散过程的热力学形式主义中,可以达到该上限。我们明确地确定了最佳协议,该协议由两个准静态等温变换通过有限的单位淬火分离。