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Quantum-classical dynamics of wave fields

机译:波场的量子经典动力学

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An approach to the quantum-classical mechanics of phase space dependent operators, which has been proposed recently, is remodeled as a formalism for wave fields. Such wave fields obey a system of coupled nonlinear equations that can be written by means of a suitable non-Hamiltonian bracket. As an example, the theory is applied to the relaxation dynamics of the spin-boson model. In the adiabatic limit, a good agreement with calculations performed by the operator approach is obtained. Moreover, the theory proposed in this paper can take nonadiabatic effects into account without resorting to surface-hopping approximations. Hence, the results obtained follow qualitatively those of previous surface-hopping calculations and increase by a factor of (at least) 2, the time length over which nonadiabatic dynamics can be propagated with small statistical errors. Moreover, it is worth to note that the dynamics of quantum-classical wave fields proposed here is a straightforward non-Hamiltonian generalization of the formalism for nonlinear quantum mechanics that Weinberg introduced recently. (c) 2007 American Institute of Physics.
机译:最近提出的一种相空间依赖算子的量子经典力学方法,被重新构建为波场的形式主义。这样的波场服从耦合非线性方程组,该非线性方程组可以通过合适的非哈密尔顿括号来写。例如,该理论被应用于自旋玻色子模型的弛豫动力学。在绝热极限中,与操作员方法执行的计算具有良好的一致性。此外,本文提出的理论可以考虑非绝热效应,而无需求助于表面跳变近似。因此,获得的结果定性地遵循先前的表面跳变计算的结果,并且增加(至少)2倍,即非绝热动力学可以以很小的统计误差传播的时间长度。此外,值得注意的是,这里提出的量子古典波场的动力学是温伯格最近引入的非线性量子力学形式主义的一种简单的非哈密尔顿式的概括。 (c)2007年美国物理研究所。

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