Gao Chao, Sun Mingyuan, Zhang Peng, Zhai Hui
Department of Physics, Zhejiang Normal University, Jinhua 321004, China.
Institute for Advanced Study, Tsinghua University, Beijing 100084, China.
Phys Rev Lett. 2020 Jan 31;124(4):040403. doi: 10.1103/PhysRevLett.124.040403.
Motivated by an unexpected experimental observation from the Cambridge group, [Eigen et al., Nature 563, 221 (2018)], we study the evolution of the momentum distribution of a degenerate Bose gas quenched from the weakly interacting regime to the unitary regime. For the two-body problem, we establish a relation that connects the momentum distribution at a long time to a subleading term in the initial wave function. For the many-body problem, we employ the time-dependent Bogoliubov variational wave function and find that, in certain momentum regimes, the momentum distribution at long times displays the same exponential behavior found by the experiment. Moreover, we find that this behavior is universal and is independent of the short-range details of the interaction potential. Consistent with the relation found in the two-body problem, we also numerically show that this exponential form is hidden in the same subleading term of the Bogoliubov wave function in the initial stages. Conceptually, our results show that, for quench to the universal regime and coherent quantum dynamics afterward, the universal longtime behavior is hidden in the initial state.
受剑桥团队一项意外实验观测结果的启发,[艾根等人,《自然》563, 221 (2018)],我们研究了从弱相互作用区域猝灭到幺正区域的简并玻色气体动量分布的演化。对于两体问题,我们建立了一个将长时间的动量分布与初始波函数中的一个次主导项联系起来的关系。对于多体问题,我们采用含时博戈留波夫变分波函数,发现,在某些动量区域,长时间的动量分布呈现出与实验中发现的相同的指数行为。此外,我们发现这种行为是普遍的,且与相互作用势的短程细节无关。与两体问题中发现的关系一致,我们还通过数值计算表明,这种指数形式在初始阶段隐藏在博戈留波夫波函数的同一个次主导项中。从概念上讲,我们的结果表明,对于猝灭到普适区域并随后进行相干量子动力学的情况,普适的长时间行为隐藏在初始状态中。