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ACCURATE CALCULATION OF QUANTUM AND DIFFUSION PROPAGATORS ARBITRARY DIMENSIONS

机译:量子和扩散传播器任意尺寸的精确计算

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A new approach to calculating the dynamics and equilibrium thermodynamics of an arbitrary (quantum or stochastic) system is presented. Its key points are representing the full propagator as a product of the harmonic-oscillator propagator with the configuration function, and expanding the configuration function (its exponent) in a power series in a given function of t. Recursion relations are obtained for the expansion coefficients which can be analytically evaluated for any number of degrees of freedom. This representation is particularly attractive for two reasons. Being structurally similar to the standard Taylorlike expansions for the propagator already known in the literature, it nevertheless shows a dramatic improvement over the latter in that it converges significantly better over a much broader range of t. Another attractive feature of the present expansion is that it is amenable to subsequent approximations. With this technique a minimal computational effort is required for constructing an improved global approximation for the propagator which is exact not only if t goes to zero, but also in the limit t-->infinity. Numerical applications to the coordinate space density matrix, quantum-mechanical time correlation function, and Fokker-Planck conditional probability show an accurate description of dynamical (statistical) properties to be already achieved for arbitrarily large times (small temperatures) with just the first term of the present expansion taken into account. Its use in a path integral means that a dramatic reduction of the number of integration variables which is required for convergence will be achieved even though simulations over very long times are desirable. (C) 1996 American Institute of Physics. [References: 52]
机译:提出了一种计算任意(量子或随机)系统动力学和平衡热力学的新方法。它的要点是将整个传播器表示为具有配置函数的谐波振荡器传播器的乘积,并在给定的t函数的幂级数中扩展配置函数(其指数)。获得膨胀系数的递归关系,可以对任意数量的自由度进行分析评估。由于两个原因,这种表示特别吸引人。与文献中已知的传播子的标准泰勒式展开在结构上相似,但它在后者上显示出显着改进,因为它在更大的t范围内收敛得更好。本扩展的另一个吸引人的特征是它适合于后续近似。使用这种技术,只需最少的计算工作即可为传播子构建一个改进的全局近似值,不仅在t变为零时,而且在极限t->无穷大时都非常精确。坐标空间密度矩阵,量子力学时间相关函数和Fokker-Planck条件概率的数值应用表明,对于任意长的时间(较小的温度),仅需将第一个项作为条件,就可以准确地描述动态(统计)性质。目前的扩张考虑在内。它在路径积分中的使用意味着,即使需要进行很长时间的模拟,也可以显着减少收敛所需的积分变量数量。 (C)1996年美国物理研究所。 [参考:52]

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