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Few-body quantum and many-body classical hyperspherical approaches to reactions and to cluster dynamics

机译:几体量子和多体经典超球面反应和簇动力学方法

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The hyperspherical method is a widely used and successful approach for the quantum treatment of elementary chemical processes.It has been mostly applied to three-atomic systems,and current progress is here outlined concerning the basic theoretical framework for the extension to four-body bound state and reactive scattering problems.Although most applications only exploit the advantages of the hyperspherical coordinate systems for the formulation of the few-body problem,the full power of the technique implies representations explicitly involving quantum hyperangular momentum operators as dynamical quantities and hyperspherical harmonics as basis functions.In terms of discrete analogues of these harmonics one has a universal representation for the kinetic energy and a diagonal representation for the potential (hyperquantization algorithm).Very recently,advances have been made on the use of the approach in classical dynamics,provided that a hyperspherical formulation is given based on "classical" definitions of the hyperangular momenta and related quantities.The aim of the present paper is to offer a retrospective and prospective view of the hyperspherical methods both in quantum and classical dynamics.Specifically,regarding the general quantum hyperspherical approaches for three-and four-body systems,we first focus on the basis set issue,and then we present developments on the classical formulation that has led to applications involving the implementations of hyperspherical techniques for classical molecular dynamics simulations of simple nanoaggregates.
机译:超球面法是一种用于基本化学过程量子处理的广泛成功的方法,它已广泛应用于三原子系统,在此概述了有关扩展至四体结合态的基本理论框架的最新进展。尽管大多数应用程序仅利用超球面坐标系的优势来表示少数物体问题,但该技术的全部功能暗示了将量子超角动量算符作为动态量以及将超球面谐波作为基本函数的表示形式就这些谐波的离散类似物而言,一个具有动能的通用表示形式,具有一个势能的对角线表示形式(超量化算法)。最近,在经典动力学中使用该方法已取得了一些进步,条件是根据“ cl本文的目的是对量子动力学和经典动力学中的超球面方法提供回顾性和前瞻性的观点。特别是关于三元和四元的一般量子超球面方法。在人体系统中,我们首先关注基集问题,然后介绍经典配方的发展,这些进展导致应用涉及涉及超球面技术的实现,用于简单纳米聚集体的经典分子动力学模拟。

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