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带电子摩擦的量子动力学

Quantum Dynamics with Electronic Friction.

作者信息

Martinazzo Rocco, Burghardt Irene

机构信息

Department of Chemistry, Università degli Studi di Milano, Via Golgi 19, 20133 Milano, Italy.

Istituto di Scienze e Tecnologie Chimiche "Giulio Natta", CNR, via Golgi 19, 20133 Milano, Italy.

出版信息

Phys Rev Lett. 2022 May 20;128(20):206002. doi: 10.1103/PhysRevLett.128.206002.

Abstract

A theory of electronic friction is developed using the exact factorization of the electronic-nuclear wave function. No assumption is made regarding the electronic bath, which can be made of independent or interacting electrons, and the nuclei are treated quantally. The ensuing equation of motion for the nuclear wave function is a nonlinear Schrödinger equation including a friction term. The resulting friction kernel agrees with a previously derived mixed quantum-classical result by Dou et al., [Phys. Rev. Lett. 119, 046001 (2017)]PRLTAO0031-900710.1103/PhysRevLett.119.046001, except for a pseudomagnetic contribution in the latter that is here removed. More specifically, it is shown that the electron dynamics generally washes out the gauge fields appearing in the adiabatic dynamics. However, these are fully re-established in the typical situation where the electrons respond rapidly on the slow time scale of the nuclear dynamics (Markov limit). Hence, we predict Berry's phase effects to be observable also in the presence of electronic friction. Application to a model vibrational relaxation problem proves that the proposed approach represents a viable way to account for electronic friction in a fully quantum setting for the nuclear dynamics.

摘要

利用电子 - 核波函数的精确因式分解发展了一种电子摩擦理论。对于电子库未作任何假设,电子库可以由独立电子或相互作用电子组成,并且对原子核进行量子处理。由此产生的核波函数运动方程是一个包含摩擦项的非线性薛定谔方程。所得的摩擦核与Dou等人先前推导的混合量子 - 经典结果[《物理评论快报》119, 046001 (2017)]PRLTAO0031 - 900710.1103/PhysRevLett.119.046001一致,只是后者中的一个赝磁贡献在这里被去除了。更具体地说,结果表明电子动力学通常会消除绝热动力学中出现的规范场。然而,在电子在原子核动力学的慢时间尺度上快速响应(马尔可夫极限)的典型情况下,这些规范场会完全重新建立。因此,我们预测在存在电子摩擦的情况下也可观测到贝里相位效应。将其应用于一个模型振动弛豫问题证明,所提出的方法是在原子核动力学的全量子设定中考虑电子摩擦的一种可行方法。

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