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J. Chem. Phys. 136, 044304 (2012); http://dx.doi.org/10.1063/1.3676658 (8 pages)

Vibrational energy relaxation of benzene dimer and trimer in the CH stretching region studied by picosecond time-resolved IR-UV pump-probe spectroscopy

Ryoji Kusaka, Yoshiya Inokuchi, and Takayuki Ebata

Department of Chemistry, Graduate School of Science, Hiroshima University, Higashi-Hiroshima 739-8526, Japan

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(Received 12 October 2011; accepted 20 December 2011; published online 23 January 2012)

Vibrational energy relaxation (VER) of the Fermi polyads in the CH stretching vibration of the benzene dimer (Bz2) and trimer (Bz3) has been investigated by picosecond (ps) time-resolved IR-UV pump-probe spectroscopy in a supersonic beam. The vibrational bands in the 3000–3100 cm−1 region were excited by a ps IR pulse and the time evolutions at the pumped and redistributed (bath) levels were probed by resonance enhanced multiphoton ionization with a ps UV pulse. For Bz2, a site-selective excitation in the T-shaped structure was achieved by using the isotope-substituted heterodimer hd, where h = C6H6 and d = C6D6, and its result was compared with that of hh homodimer. In the hd heterodimer, the two isomers, h(stem)d(top) and h(top)d(stem), show remarkable site-dependence of the lifetime of intracluster vibrational energy redistribution (IVR); the lifetime of the Stem site [h(stem)d(top), 140–170 ps] is ∼2.5 times shorter than that of the Top site [h(top)d(stem), 370–400 ps]. In the transient UV spectra, a broad electronic transition due to the bath modes emerges and gradually decays with a nanosecond time scale. The broad transition shows different time profile depending on UV frequency monitored. These time profiles are described by a three-step VER model involving IVR and vibrational predissociation: initial → bath1(intramolecular) → bath2(intermolecular) → fragments. This model also describes well the observed time profile of the Bz fragment. The hh homodimer shows the stepwise VER process with time constants similar to those of the hd dimer, suggesting that the excitation-exchange coupling of the vibrations between the two sites is very weak. Bz3 also exhibited the stepwise VER process, though each step is faster than Bz2.

© 2012 American Institute of Physics

Article Outline

  1. INTRODUCTION
  2. EXPERIMENTAL AND ANALYSIS
  3. RESULTS AND DISCUSSION
    1. IR spectra of Bz 2
    2. Transient UV spectra of Bz 2 after the IR excitation of Fermi-polyad
    3. IVR of the IR-pumped levels of Bz 2
      1. IVR decay of hd and hh dimers
      2. Excitation-exchange coupling between Stem and Top sites of the hh dimer
    4. Time profile of the bath states and VER mechanism of Bz 2
      1. Time evolution of the bath states
      2. Origins of bath states 1 and 2
    5. Time evolution of Bz monomer fragment: VP of Bz 2
    6. VER of Bz 3
  4. CONCLUSION

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KEYWORDS, PACS, and IPC

PACS

  • 36.40.Mr

    Spectroscopy and geometrical structure of clusters

  • 33.15.Mt

    Rotation, vibration, and vibration-rotation constants

  • 33.20.Ea

    Infrared spectra

  • 33.20.Kf

    Visible spectra

  • 33.80.Eh

    Autoionization, photoionization, and photodetachment

  • 36.40.Cg

    Electronic and magnetic properties of clusters

International Patent Classification (IPC)

ARTICLE DATA

PUBLICATION DATA

ISSN

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

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