Analytical Evaluation for Calculation of Two-Center Franck – Condon Factor and Matrix Elements

/e Franck–Condon (FC) factor is defined as squares of the Franck–Condon (FC) overlap integral and represents one of the principle fundamental factors of molecular physics. /e FC factor is used to determine the transition probabilities in different vibrational levels of the two electronic states and the spectral line intensities of diatomic and polyatomic molecules. In this study, new analytical formulas were derived to calculate Franck–Condon integral (FCI) of harmonic oscillators and matrix elements (xη, e−2cx, and e−cx ) including simple finite summations of binomial coefficients. /ese formulas are valid for arbitrary values. /e results of formulas are in agreement with the results in the literature.


Introduction
e Franck-Condon (FC) principle is used to determine the transition probabilities between different vibrational levels of the two electronic states showing the intensity distribution in the band spectrum [1].e FC principle provides a choice rule for the relative probability of the oscillation transition.Since the transition probabilities and the spectral line intensities have been determined by the FC factor, it also plays an important role in determination of the optical and radiationless transition rates between vibration levels [1][2][3].
e generalized matrix elements of the coordinate operator (i.e., x η , e −2cx , and e −cx 2 ) are considered as issues requiring solution during determination of nonradiative transition ratios between two vibrational states in quantum mechanical problems.
Calculations of the FC overlap integral with matrix elements are basic problems in molecular physics [15][16][17][18][19][20][21].e FC factor has been studied both experimentally and theoretically for the solution of the many problems mentioned above .
e purpose of this study was to present simple and easily computable analytical formulas by the calculation of binomial coefficients for Franck-Condon integral (FCI) of harmonic oscillators and for x η , e −2cx , and e −cx 2 matrix elements.e suggested analytical method was compared to the results of similar calculations for Franck-Condon integral and matrix elements.

Franck-Condon Overlap Integral Based on Harmonic Oscillator Wave Function
Two-center Franck-Condon (FC) integral over harmonic oscillators wave functions have the following form: where ψ n is an eigen function of the one-dimensional (1D) harmonic oscillator.e Schrödinger equation for this wave function can be written as where μ is the reduced mass, and the normalized wave function for harmonic oscillators is defined as where In Equation ( 3), Hermite polynomial H n (x) is defined as a final series as follows [2,47]: 1) can be written as Substituting ( 5) into (6), we obtain the following equation for the FC overlap integral: For the evaluation of Equation ( 7), we use the following binomial expansion theorem for an arbitrary real n [58,59]: Substituting Equation ( 8) into (7), we obtain the following series formula for the integral in Equation ( 7): where and K n is the basic integral defined by [60] K where Substituting Equation ( 9) into Equation ( 7), we obtain the following formula for the FC overlap integral: where where

Matrix Elements Based on Harmonic Oscillator Wave Function
Matrix elements over the harmonic oscillator wave function are defined as follows: In Equation (15), f(x) is the operator and can be examined in the forms of power of the coordinate (x η ), exponential function (e −2cx ), and Gaussian function (e −cx 2 ).

Journal of Chemistry
If the method used in determination of the FC overlap integral is used for x η , e −2cx , and e −cx 2 matrix elements in Equation (15), the following analytical equations are obtained.

Numerical Results and Discussion
In this work, new analytical formulas were derived to calculate the FC overlap integral and matrix elements based on harmonic oscillator functions as an alternative to approaches in the literature.Suggested formulas include simple finite sums and can be easily used calculate arbitrary values of ] and ] ′ .Equation ( 15) was confirmed as reduced analytical expressions of Equations ( 16), (17), and (19) where the f(x) function is specified as Gaussian, exponential, or the power of x. e Franck-Condon overlap integral and the analytical expressions of matrix elements obtained by the use of onedimensional harmonic oscillators above can be used for diatomic molecules.
e calculation of the FC factor is important to investigate the vibration transitions in diatomic molecules.Because the polyatomic molecules have more arbitrary degrees, it will be necessary to use two-dimensional or multidimensional vibrations.e different methods have been proposed in the literature to calculate the Franck-Condon Factor in polyatomic molecules [45][46][47].To study excited molecular states in accordance with developed experimental data, it is important to model these excited situations of molecules and the transitions between them.e general analysis was performed successfully here because the results obtained for the FC Reference [16] for Equation (2.9) Reference [17] for Equation (20) Reference [14] 0 2 0.001 overlap integral and matrix elements over one-dimensional harmonic oscillators wave function completely overlap with the analytical results of Guseinov et al. [15], Iachello and Ibrahim [16], and Chang [17] (Tables 1-4).The computer program for Equations ( 12), ( 16), (17), and (19) containing simple finite sums of binomial coefficients was developed using Mathematica 8.0 software.e comparison between the results of developed software and literature is shown in Tables 1-4 for arbitrary values of the integral parameters calculated.e results for the FC overlap integral and matrix elements showed considerably high accuracy with the results in the literature within the integral parameters.e results of this study can be used to determine the various spectral line densities of molecules and to calculate the transition problems of various vibration levels.

Table 1 :
e values of FC overlap integral over harmonic oscillator wave functions.

Table 2 :
e values of two-center harmonic oscillator matrix elements of x η .

Table 3 :
e values of two-center harmonic oscillator matrix elements of e −2cx .

Table 4 :
e values of two-center harmonic oscillator matrix elements of e −cx 2 .