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首页> 外文期刊>The Journal of Chemical Physics >Exact numerical computation of a kinetic energy operator in curvilinear coordinates
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Exact numerical computation of a kinetic energy operator in curvilinear coordinates

机译:曲线坐标中动能算子的精确数值计算

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The conformation and dynamical behavior of molecular systems is very often advantageously described in terms of physically well-adapted curvilinear coordinates. It is rather easy to show that the numerous analytical expressions of the kinetic energy operator of a molecular system described in terms of n curvilinear coordinates can all be transformed into the following more usable expression: T = #EPSILON#_(ij)f_2~(ij)(q) partial deriv~2/partial derivq~ipartial derivq~j + #EPSILON#_if_1~i(q) partial deriv/partial derivq~i + v(q), where f_2~ij(q), f_1~i(q), and v(q) are functions of the curvilinear coordinates q = (...,q~i,...). If the advantages of curvilinear coordinates are unquestionable, they do have a major drawback: the sometimes awful complexity of the analytical expression of the kinetic operator T for molecular systems with more than five atoms. Therefore, we develop an algorithm for computing T for a given value of the n curvilinear coordinates q. The calculation of the functions f_2~(ij)(q), f_1~i(q), and v(q) only requires the knowledge of the Cartesian coordinates and their derivatives in terms of the n curvilinear coordinates. This coordinate transformation (curvilinear -> Cartesian) is very easy to perform and is widely used in quantym chemistry codes resorting to a Z-matrix to define the curvilinear coordinates. Thus, the functions f_2~(ij)(q), f_1~i(q), and v(q) can be evaluated numerically and exactly for a given value of q, which makes it possible to propagate wavepackets or to simulate the spectra of rather complex systems (constrained Hamiltonian). The accuracy of this numerical procedure is tested by comparing two calculations of the bending spectrum of HCN: the first one, performed by using the present numerical kinetic operator procedure, the second one, obtained in previous studies, by using an analytical kinetic operator. Finally, the ab initio computation of the internal rotatin spectrum and wave functions of 2-methylpropanal by means of dimensionality reduction, is given as an original application.
机译:分子系统的构象和动力学行为通常根据物理上适应性良好的曲线坐标进行描述。很容易证明,用n个曲线坐标描述的分子系统动能算符的众多解析表达式都可以转化为以下更有用的表达式:T = #EPSILON #_(ij)f_2〜( ij)(q)偏导数〜2 /偏导数〜i偏导数j +#EPSILON#_if_1〜i(q)偏导数/偏导数i + v(q),其中f_2〜ij(q),f_1〜 i(q)和v(q)是曲线坐标q =(...,q〜i,...)的函数。如果曲线坐标的优点是毋庸置疑的,那么它们的确存在一个主要缺点:对于具有五个以上原子的分子系统,动力学算子T的解析表达式有时非常复杂。因此,我们开发了一种算法,用于针对n个曲线坐标q的给定值计算T。函数f_2〜(ij)(q),f_1〜i(q)和v(q)的计算仅需要了解n曲线坐标下的笛卡尔坐标及其导数。这种坐标变换(曲线->笛卡尔坐标)非常易于执行,并广泛用于依靠Z矩阵定义曲线坐标的量子化学代码中。因此,对于给定的q值,可以数值精确地评估函数f_2〜(ij)(q),f_1〜i(q)和v(q),从而可以传播波包或模拟频谱相当复杂的系统(受约束的哈密顿量)。通过比较HCN弯曲谱的两个计算来测试此数值程序的准确性:第一个通过使用当前的数值动力学算子过程执行,第二个在以前的研究中通过使用解析动力学算子获得。最后,通过降维从头计算2-甲基丙醛的内部rotatin光谱和波函数作为原始应用。

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