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基于溶剂动力学静电势表示的溶液反应空间哈密顿量。

Solution reaction space Hamiltonian based on an electrostatic potential representation of solvent dynamics.

机构信息

Department of Chemistry, Kyoto University, Kyoto 606-8502, Japan.

出版信息

J Chem Phys. 2011 Apr 14;134(14):144108. doi: 10.1063/1.3572057.

Abstract

Quantum chemical solvation models usually rely on the equilibrium solvation condition and is thus not immediately applicable to the study of nonequilibrium solvation dynamics, particularly those associated with chemical reactions. Here we address this problem by considering an effective Hamiltonian for solution-phase reactions based on an electrostatic potential (ESP) representation of solvent dynamics. In this approach a general ESP field of solvent is employed as collective solvent coordinate, and an effective Hamiltonian is constructed by treating both solute geometry and solvent ESP as dynamical variables. A harmonic bath is then attached onto the ESP variables in order to account for the stochastic nature of solvent dynamics. As an illustration we apply the above method to the proton transfer of a substituted phenol-amine complex in a polar solvent. The effective Hamiltonian is constructed by means of the reference interaction site model self-consistent field method (i.e., a type of quantum chemical solvation model), and a mixed quantum/classical simulation is performed in the space of solute geometry and solvent ESP. The results suggest that important dynamical features of proton transfer in solution can be captured by the present approach, including spontaneous fluctuations of solvent ESP that drives the proton from reactant to product potential wells.

摘要

量子化学溶剂化模型通常依赖于平衡溶剂化条件,因此不能立即应用于非平衡溶剂化动力学的研究,特别是与化学反应相关的动力学。在这里,我们通过考虑基于溶剂动力学静电势能(ESP)表示的溶液相反应的有效哈密顿量来解决这个问题。在这种方法中,通常采用广义的 ESP 场作为溶剂的集体溶剂坐标,并将溶质几何形状和溶剂 ESP 都作为动力学变量来构建有效哈密顿量。然后在 ESP 变量上附加一个调和浴,以考虑溶剂动力学的随机性质。作为说明,我们将上述方法应用于极性溶剂中取代的苯酚-胺配合物的质子转移。有效哈密顿量是通过参考相互作用位点模型自洽场方法(即一种量子化学溶剂化模型)构建的,并在溶质几何形状和溶剂 ESP 的空间中进行混合量子/经典模拟。结果表明,本方法可以捕捉到溶液中质子转移的重要动力学特征,包括驱动质子从反应物到产物势能阱的溶剂 ESP 的自发波动。

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