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具有非线性耦合的自旋-晶格弛豫:费米黄金规则与扩展耗散运动方程的比较

Spin-lattice relaxation with non-linear couplings: Comparison between Fermi's golden rule and extended dissipaton equation of motion.

作者信息

Bi Rui-Hao, Su Yu, Wang Yao, Sun Lei, Dou Wenjie

机构信息

Department of Chemistry, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou, Zhejiang 310024, China.

Hefei National Research Center for Physical Sciences at the Microscale, University of Science and Technology of China, Hefei, Anhui 230026, China.

出版信息

J Chem Phys. 2024 Jul 14;161(2). doi: 10.1063/5.0212870.

Abstract

Fermi's golden rule (FGR) offers an empirical framework for understanding the dynamics of spin-lattice relaxation in magnetic molecules, encompassing mechanisms like direct (one-phonon) and Raman (two-phonon) processes. These principles effectively model experimental longitudinal relaxation rates, denoted as T1-1. However, under scenarios of increased coupling strength and nonlinear spin-lattice interactions, FGR's applicability may diminish. This paper numerically evaluates the exact spin-lattice relaxation rate kernels, employing the extended dissipaton equation of motion formalism. Our calculations reveal that when quadratic spin-lattice coupling is considered, the rate kernels exhibit a free induction decay-like feature, and the damping rates depend on the interaction strength. We observe that the temperature dependence predicted by FGR significantly deviates from the exact results since FGR ignores the higher order effects and the non-Markovian nature of spin-lattice relaxation. Our methods can be easily extended to study other systems with nonlinear spin-lattice interactions and provide valuable insights into the temperature dependence of T1 in molecular qubits when the coupling is strong.

摘要

费米黄金规则(FGR)为理解磁性分子中自旋 - 晶格弛豫的动力学提供了一个经验框架,涵盖直接(单声子)和拉曼(双声子)等过程。这些原理有效地模拟了实验纵向弛豫率,记为T1-1。然而,在耦合强度增加和非线性自旋 - 晶格相互作用的情况下,FGR的适用性可能会降低。本文采用扩展的运动耗散方程形式,对精确的自旋 - 晶格弛豫率核进行了数值评估。我们的计算表明,当考虑二次自旋 - 晶格耦合时,率核呈现出类似自由感应衰减的特征,并且阻尼率取决于相互作用强度。我们观察到,由于FGR忽略了高阶效应和自旋 - 晶格弛豫的非马尔可夫性质,FGR预测的温度依赖性与精确结果有显著偏差。我们的方法可以很容易地扩展到研究其他具有非线性自旋 - 晶格相互作用的系统,并在耦合较强时为分子量子比特中T1的温度依赖性提供有价值的见解。

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