Coherent spin-phonon scattering in facilitated Rydberg lattices

Matteo Magoni, Chris Nill, Igor Lesanovsky
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Abstract

We investigate the dynamics of a spin system with facilitation constraint that can be studied using Rydberg atoms in arrays of optical tweezer traps. The elementary degrees of freedom of the system are domains of Rydberg excitations that expand ballistically through the lattice. Due to mechanical forces, Rydberg excited atoms are coupled to vibrations within their traps. At zero temperature and large trap depth, it is known that virtually excited lattice vibrations only renormalize the timescale of the ballistic propagation. However, when vibrational excitations are initially present -- i.e., when the external motion of the atoms is prepared in an excited Fock state, coherent state or thermal state -- resonant scattering between spin domain walls and phonons takes place. This coherent and deterministic process, which is free from disorder, leads to a reduction of the power-law exponent characterizing the expansion of spin domains. Furthermore, the spin domain dynamics is sensitive to the coherence properties of the atoms' vibrational state, such as the relative phase of coherently superimposed Fock states. Even for a translationally invariant initial state the latter manifests macroscopically in a phase-sensitive asymmetric expansion.
易化里德堡晶格中的相干自旋声子散射
我们研究了具有易化约束的自旋系统的动力学,该系统可以用光学镊子阱阵列中的里德伯原子来研究。系统的基本自由度是里德伯激振的域,它在晶格中以弹道方式扩展。由于机械力的作用,里德伯激发态原子与它们的阱内的振动相耦合。在零温度和大阱深度下,已知虚激发晶格振动仅使弹道传播的时间尺度重新归一化。然而,当振动激发最初存在时——即,当原子的外部运动处于激发态、相干态或热态时——自旋畴壁和声子之间就会发生共振散射。这种无无序的相干和确定性过程导致表征自旋域扩展的幂律指数的降低。此外,自旋域动力学对原子振动态的相干性很敏感,例如相干叠加的Fock态的相对相位。即使对于非平移不变初始态,后者在宏观上也表现为相敏不对称膨胀。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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