Eigenstate‐free, Green function, calculation of molecular absorption and fluorescence line shapes

Green function techniques are used to develop a simple and efficient method towards the calculation of optical absorption, excitation, and dispersed fluorescence spectra of large harmonic polyatomic molecules. The molecular line shapes are expressed in terms of Fourier transforms of appropriate correlation functions which may be explicitly evaluated. Closed expressions are derived for a general harmonic molecule with two electronic states including equilibrium displacements, frequency changes, and Dushinsky rotation, within the Condon approximation. A simple method for extracting the complete set of parameters characterizing the ground and the electronically excited states from supersonic beam absorption and emission spectra is presented. Detailed calculations are performed for a model system with ten vibrational modes, and the sensitivity of the various experimental observables to Dushinsky rotation is analyzed.

[1]  K. Holtzclaw,et al.  Chemical timing 4. The rovibronic level structure associated with intramolecular vibrational redistribution in S1p‐difluorobenzene , 1986 .

[2]  J. Katriel Second quantization and the general two-centre harmonic oscillator integrals , 1970 .

[3]  M. Lax The Franck‐Condon Principle and Its Application to Crystals , 1952 .

[4]  C. Ultee Photoselective chemistry , 1982, IEEE Journal of Quantum Electronics.

[5]  N. Boccara,et al.  Polycyclic aromatic hydrocarbons and astrophysics , 1986 .

[6]  S. Mukamel Stochastic theory of resonance Raman line shapes of polyatomic molecules in condensed phases , 1985 .

[7]  Ryogo Kubo,et al.  Application of the Method of Generating Function to Radiative and Non-Radiative Transitions of a Trapped Electron in a Crystal , 1955 .

[8]  A. Zewail,et al.  Picosecond excitation and selective intramolecular rates in supersonic molecular beams. I. SVL fluorescence spectra and lifetimes of anthracene and deuterated anthracenes , 1984 .

[9]  S. Mukamel Fluorescence and absorption of large anharmonic molecules - spectroscopy without eigenstates , 1985 .

[10]  A. C. Albrecht,et al.  A direct inverse transform for resonance Raman scattering , 1986 .

[11]  S. Mukamel,et al.  Nonlinear susceptibilities and coherent and spontaneous Raman spectroscopy of polyatomic molecules in condensed phases , 1986 .

[12]  J. J. Markham Interaction of Normal Modes with Electron Traps , 1959 .

[13]  Warner L. Peticolas,et al.  Excited state geometry of uracil from the resonant Raman overtone spectrum using a Kramers–Kronig technique , 1982 .

[14]  E. Heller,et al.  Polyatomic Raman scattering for general harmonic potentials , 1982 .

[15]  C. Chan,et al.  Resonance Raman scattering study of azulene. II. Nonzero temperature multimode model calculations , 1985 .

[16]  Eleftherios N. Economou,et al.  Green's functions in quantum physics , 1979 .

[17]  R. Friesner,et al.  Calculation of temperature‐dependent multimode resonance Raman line shapes for harmonic potential surfacesa) , 1985 .

[18]  R. Feynman,et al.  Quantum Mechanics and Path Integrals , 1965 .

[19]  S. Mukamel Collisional broadening of spectral line shapes in two-photon and multiphoton processes , 1982 .

[20]  C. Haynam,et al.  Ultraviolet spectra of benzene clusters , 1981 .

[21]  Dieter Forster,et al.  Hydrodynamic fluctuations, broken symmetry, and correlation functions , 1975 .

[22]  Irene A. Stegun,et al.  Handbook of Mathematical Functions. , 1966 .

[23]  H. Kono,et al.  A theoretical study of resonance Raman scattering from molecules. III. Resonance Raman scattering and resonance fluorescence , 1981 .

[24]  W. Brand,et al.  Isomerization of internal-energy-selected ions , 1983 .

[25]  M. Trulson,et al.  Quantitation of homogeneous and inhomogeneous broadening mechanisms in trans‐stilbene using absolute resonance Raman intensities , 1985 .