论文标题
在开放量子系统放松期间,临界缩放时间的迹象表明
Indication of critical scaling in time during the relaxation of an open quantum system
论文作者
论文摘要
相变的相对于响应连续控制参数(如温度或外部场),物理系统的奇异行为对应。发现与相关长度的差异相关的几乎连续的相变,通用幂律缩放行为与关键指数与显微镜系统细节无关。最近,在淬灭后,已经预测并观察到在分离的量子系统的非平衡动力学中观察到的动力学量子相变和通用缩放,随着时间的流逝起着控制参数的作用。但是,到目前为止,由于与环境的耗散接触驱动的开放系统中,这种关键现象的签名是迄今为止难以捉摸的。在这里,我们提出的结果表明,在混合状态描述的开放量子系统的松弛动力学中,还可能发生有关时间的临界缩放。我们在实验上测量了通过自旋交换过程诱导的个体原子的大原子自旋的弛豫动力学,以诱导的rubidium原子的超速卵形气体。对于远离平衡的初始状态,发现自旋状态的熵在时间上达到峰值,瞬时接近其最大值的值,然后最终放松到其较低的平衡值。此外,基于数值模拟的有限尺寸缩放分析表明,它与大型系统尺寸极限的耗散系统时间相对于临界点。它是由特征长度在关键时间的差异发出的,其特征是关键指数被发现独立于系统细节。
Phase transitions correspond to the singular behavior of physical systems in response to continuous control parameters like temperature or external fields. Near continuous phase transitions, associated with the divergence of a correlation length, universal power-law scaling behavior with critical exponents independent of microscopic system details is found. Recently, dynamical quantum phase transitions and universal scaling have been predicted and also observed in the non-equilibrium dynamics of isolated quantum systems after a quench, with time playing the role of the control parameter. However, signatures of such critical phenomena in time in open systems, whose dynamics is driven by the dissipative contact to an environment, were so far elusive. Here, we present results indicating that critical scaling with respect to time can also occur during the relaxation dynamics of an open quantum system described by mixed states. We experimentally measure the relaxation dynamics of the large atomic spin of individual Caesium atoms induced by the dissipative coupling via spin-exchange processes to an ultracold Bose gas of Rubidium atoms. For initial states far from equilibrium, the entropy of the spin state is found to peak in time, transiently approaching its maximum possible value, before eventually relaxing to its lower equilibrium value. Moreover, a finite-size scaling analysis based on numerical simulations shows that it corresponds to a critical point with respect to time of the dissipative system in the limit of large system sizes. It is signalled by the divergence of a characteristic length at a critical time, characterized by critical exponents that are found to be independent of system details.