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与耗散浴相互作用的伊辛链的量子猝灭及相干-非相干动力学

Quantum quench and coherent-incoherent dynamics of Ising chains interacting with dissipative baths.

作者信息

Dani Reshmi, Makri Nancy

机构信息

Department of Chemistry, University of Illinois, Urbana, Illinois 61801, USA.

出版信息

J Chem Phys. 2021 Dec 21;155(23):234705. doi: 10.1063/5.0066891.

Abstract

The modular path integral methodology is used to extend the well-known spin-boson dynamics to finite-length quantum Ising chains, where each spin is coupled to a dissipative harmonic bath. The chain is initially prepared in the ferromagnetic phase where all spins are aligned, and the magnetization is calculated with spin-spin coupling parameters corresponding to the paramagnetic phase, mimicking a quantum quench experiment. The observed dynamics is found to depend significantly on the location of the tagged spin. In the absence of a dissipative bath, the time evolution displays irregular patterns that arise from multiple frequencies associated with the eigenvalues of the chain Hamiltonian. Coupling of each spin to a harmonic bath leads to smoother dynamics, with damping effects that are stronger compared to those observed in the spin-boson model and more prominent in interior spins, a consequence of additional damping from the spin environment. Interior spins exhibit a transition from underdamped oscillatory to overdamped monotonic dynamics as the temperature, spin-bath, or spin-spin coupling is increased. In addition to these behaviors, a new dynamical pattern emerges in the evolution of edge spins with strong spin-spin coupling at low and intermediate temperatures, where the magnetization oscillates either above or below the equilibrium value.

摘要

模块化路径积分方法用于将著名的自旋 - 玻色子动力学扩展到有限长度的量子伊辛链,其中每个自旋都与一个耗散性谐振子浴耦合。该链最初制备在铁磁相中,此时所有自旋都排列整齐,并且使用对应于顺磁相的自旋 - 自旋耦合参数来计算磁化强度,以此模拟量子猝灭实验。发现所观察到的动力学显著依赖于被标记自旋的位置。在没有耗散浴的情况下,时间演化呈现出不规则模式,这些模式源于与链哈密顿量的本征值相关的多个频率。每个自旋与谐振子浴的耦合导致动力学更平滑,与自旋 - 玻色子模型中观察到的阻尼效应相比更强,并且在内部自旋中更显著,这是自旋环境产生额外阻尼的结果。随着温度、自旋 - 浴或自旋 - 自旋耦合的增加,内部自旋表现出从欠阻尼振荡到过阻尼单调动力学的转变。除了这些行为外,在低温和中温下具有强自旋 - 自旋耦合的边缘自旋的演化中出现了一种新的动力学模式,其中磁化强度在平衡值之上或之下振荡。

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