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二维红外光谱的时间关联函数理论及其在液态水中的应用

A time correlation function theory of two-dimensional infrared spectroscopy with applications to liquid water.

作者信息

DeVane Russell, Space Brian, Perry Angela, Neipert Christine, Ridley Christina, Keyes T

机构信息

Department of Chemistry, University of South Florida, SCA400 Tampa, Florida 33620-5250, USA.

出版信息

J Chem Phys. 2004 Aug 22;121(8):3688-701. doi: 10.1063/1.1776119.

Abstract

A theory describing the third-order response function R((3))(t(1),t(2),t(3)), which is associated with two-dimensional infrared (2DIR) spectroscopy, has been developed. R((3)) can be written as sums and differences of four distinct quantum mechanical dipole (multi)time correlation functions (TCF's), each with the same classical limit; the combination of TCF's has a leading contribution of order variant Planck's over 2pi (3) and thus there is no obvious classical limit that can be written in terms of a TCF. In order to calculate the response function in a form amenable to classical mechanical simulation techniques, it is rewritten approximately in terms of a single classical TCF, B(R)(t(1),t(2),t(3))=micro(j)(t(2)+t(1))micro(i)(t(3)+t(2)+t(1))micro(k)(t(1))micro(l)(0), where the subscripts denote the Cartesian dipole directions. The response function is then given, in the frequency domain, as the Fourier transform of a classical TCF multiplied by frequency factors. This classical expression can then further be quantum corrected to approximate the true response function, although for low frequency spectroscopy no correction is needed. In the classical limit, R((3)) becomes the sum of multidimensional time derivatives of B(R)(t(1),t(2),t(3)). To construct the theory, the response function's four TCF's are rewritten in terms of a single TCF: first, two TCF's are eliminated from R((3)) using frequency domain detailed balance relationships, and next, two more are removed by relating the remaining TCF's to each other within a harmonic oscillator approximation; the theory invokes a harmonic approximation only in relating the TCF's and applications of theory involve fully anharmonic, atomistically detailed molecular dynamics (MD). Writing the response function as a single TCF thus yields a form amenable to calculation using classical MD methods along with a suitable spectroscopic model. To demonstrate the theory, the response function is obtained for liquid water with emphasis on the OH stretching portion of the spectrum. This approach to evaluating R((3)) can easily be applied to chemically interesting systems currently being explored experimentally by 2DIR and to help understand the information content of the emerging multidimensional spectroscopy.

摘要

已开发出一种描述三阶响应函数(R^{(3)}(t_1,t_2,t_3))的理论,该函数与二维红外(2DIR)光谱相关。(R^{(3)})可写成四个不同的量子力学偶极(多)时间关联函数(TCF)的和与差,每个函数具有相同的经典极限;TCF的组合具有一个领先贡献,其量级为普朗克常量除以(2\pi)的三次方,因此不存在能用TCF表示的明显经典极限。为了以适合经典力学模拟技术的形式计算响应函数,它被近似地改写为一个单一的经典TCF,即(B_R(t_1,t_2,t_3)=\mu_j(t_2 + t_1)\mu_i(t_3 + t_2 + t_1)\mu_k(t_1)\mu_l(0)),其中下标表示笛卡尔偶极方向。然后,在频域中,响应函数由经典TCF乘以频率因子的傅里叶变换给出。尽管对于低频光谱不需要修正,但这个经典表达式随后可以进一步进行量子修正以近似真实的响应函数。在经典极限下,(R^{(3)})成为(B_R(t_1,t_2,t_3))的多维时间导数之和。为构建该理论,响应函数的四个TCF被改写为一个单一的TCF:首先,利用频域详细平衡关系从(R^{(3)})中消除两个TCF,接着,通过在简谐振子近似下将剩余的TCF相互关联,再消除另外两个;该理论仅在关联TCF时调用简谐近似,并且理论应用涉及完全非简谐的、原子级详细的分子动力学(MD)。将响应函数写成一个单一的TCF从而得到一种适合使用经典MD方法以及合适的光谱模型进行计算的形式。为了演示该理论,以液态水为例获得了响应函数,重点关注光谱中的OH伸缩部分。这种评估(R^{(3)})的方法可以很容易地应用于目前正在通过2DIR进行实验探索的具有化学意义的系统,并有助于理解新兴多维光谱的信息内容。

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