Observation of Continuous Time Crystal in a Spin Maser System

Weiyu Wang, Mingjun Feng, Qianjin Ma, Zi Cai, Erwei Li, Guobin Liu
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Abstract

Pair interaction potentials between atoms in a crystal are in general non-monotonic in distance, with a local minimum whose position gives the lattice constant of the crystal. A temporal analogue of this idea of crystal formation is still pending despite intensive studies on the time crystal phase. In a hybrid spin maser system with a time delay feedback, we report the observation of a continuous time crystal induced by a retarded interaction with a characteristic time scale. This nonequilibrium phase features a self-sustained oscillation with an emergent frequency other than the intrinsic Larmor precession frequency of the spin maser system. It is shown that the amplitude of the oscillation is robust against perturbation, while its time phase randomly distributes from 0 to $2\pi$ for different realizations, a signature of spontaneous continuous time translation symmetry breaking. This CTC phase emerges only when the feedback strength exceeds a critical value, at which the system experiences a first order phase transition. Such a retarded interaction induced CTC is closer to the original idea of crystal, compared to mechanisms in other time crystal proposals.
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自旋激光系统中的连续时间晶体观测
晶体中原子间的成对相互作用势在距离上一般是非单调的,有一个局部最小值,其位置给出了晶体的晶格常数。在一个具有时延反馈的混合自旋 maser 系统中,我们观测到了由具有特征时间尺度的迟滞相互作用诱导的连续时间晶体。这种非平衡相的特点是自持振荡,其出现频率与自旋芒星系统的固有拉莫尔前驱频率不同。研究表明,振荡的振幅对扰动是稳健的,而其时相在不同的实现情况下随机分布在 0 到 2 美元之间,这是自发连续时间平移对称性破缺的特征。只有当反馈强度超过临界值时,系统才会经历一阶相变,此时才会出现 CTC 阶段。与其他时间晶体方案中的机制相比,这种迟滞相互作用诱导的 CTC 更接近晶体的原始构想。
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