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J. Chem. Phys. 134, 094313 (2011); http://dx.doi.org/10.1063/1.3559454 (12 pages)

Franck–Condon simulation of the A 1B2X 1A1 dispersed fluorescence spectrum of fluorobenzene and its rate of the internal conversion

Rongxing He1,2, Ling Yang1,3, Chaoyuan Zhu1, Masahiro Yamaki4, Yuan-Pern Lee1, and Sheng Hsien Lin1,4

1Department of Applied Chemistry, Institute of Molecular Science and Center for Interdisciplinary Molecular Science, National Chiao-Tung University, Hsinchu 30050, Taiwan
2College of Chemistry and Chemical Engineering, Southwest University, Chongqing 400715, China
3Department of Chemistry, Beijing Normal University, Beijing 100875, People's Republic of China
4Institute of Atomic and Molecular Sciences, Academia Sinica, Taipei 106, Taiwan

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(Received 16 August 2010; accepted 7 February 2011; published online 7 March 2011)

By using three different hybrid exchange-correlation functionals containing 20%, 35%, and 50% of exact Hartree–Fock (HF) exchange of the density functional theory and its time-dependent extension plus the Hartree–Fock and the configuration interaction of single excitation methods, equilibrium geometries, and their 30 vibrational–normal-mode frequencies of the ground S0(1A1) and the first excited S1(1B2) states of fluorobenzene (FB) were calculated. The dispersed fluorescence spectrum and internal conversion (IC) rate of the A 1B2X 1A1 transition were simulated by Franck–Condon (FC) calculations within the displaced harmonic oscillator approximation plus anharmonic and distorted corrections. The simulated spectral profile is primarily described by the Franck–Condon progression from the ring-breathing modes v9 and v10 which belong to totally symmetry modes. Anharmonic corrections simultaneously improve the intensity order of 910 and 1010 bands and diminish 110 transition that is fairly strong in harmonic simulations. It is concluded that the amount of Hartree–Fock exchange does impact the geometries and vibrational frequencies of FB molecule, but not the relative intensities of the transitions. It is anharmonic corrections that make the relative intensities of the transitions in good agreement with experimental results. Distorted corrections could assign most of the dominant overtones of out-of-plane nontotally symmetry modes, and the results agree well with the experimental assignments. Furthermore, it was found that the internal conversion rate is dominated by three promoting modes that are computed with lowing symmetry to C1. By choosing dephasing width as 10 cm−1 that is consistent with spectral simulation, we obtained the lifetimes of the A 1B2X 1A1 de-excitation as 11 and 19 ns, respectively, from TD(B3LYP) and HF/CIS calculations in comparison with the experimental value 14.75 ns.

© 2011 American Institute of Physics

Article Outline

  1. INTRODUCTION
  2. COMPUTATIONAL METHODS
    1. Ab initio methods for electronic properties
    2. Franck–Condon simulation for DF spectra
    3. Franck–Condon simulation for internal conversion
  3. RESULTS AND DISCUSSIONS
    1. Equilibrium geometries and vibrational frequencies
    2. Electronic structures and excitation energies
    3. Franck–Condon simulation of the DF spectrum
    4. Internal conversion and the lifetime of S 1 state
  4. CONCLUDING REMARKS

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KEYWORDS and PACS

PACS

  • 33.70.Ca

    Oscillator and band strengths, lifetimes, transition moments, and Franck-Condon factors

  • 33.50.Hv

    Radiationless transitions, quenching

  • 33.50.Dq

    Fluorescence and phosphorescence spectra

  • 31.15.ve

    Electron correlation calculations for atoms and ions: ground state

  • 31.15.vj

    Electron correlation calculations for atoms and ions: excited states

  • 31.15.xr

    Self-consistent-field methods

ARTICLE DATA

PUBLICATION DATA

ISSN

0021-9606 (print)  
1089-7690 (online)

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