Dynamics of Electronic States and Spin−Flip for Photodissociation of Dihalogens in Matrices:  Experiment and Semiclassical Surface-Hopping and Quantum Model Simulations for F2 and ClF in Solid Ar

M. Bargheer, A. Cohen,*£ R. B. Gerber,£§ M. Gühr,*# M. V. Korolkov,* J. Manz, M. Y. Niv,£ M. Schröder, and N. Schwentner
Institut fr Experimentalphysik, Freie Universitt Berlin, Arnimallee 14, 14195 Berlin, Germany, Department of Physical Chemistry and the Fritz Haber Center for Molecular Dynamics, Hebrew University of Jerusalem, 91904 Israel, Department of Chemistry, University of California, Irvine, California 92697, Institute of Physics, National Academy of Sciences of Belarus, Skaryna Ave. 70, 220602 Minsk, Belarus, Institut fr Chemie und Biochemie, Freie Universitt Berlin, Takustrasse 3, 14195 Berlin, Germany, and Stanford PULSE Center, Stanford University, Stanford, California 94305
J. Phys. Chem. A, 2007, 111 (38), pp 9573–9585
DOI: 10.1021/jp071771t
Publication Date (Web): July 13, 2007
Copyright © 2007 American Chemical Society

 Part of the “Sheng Hsien Lin Festschrift”.

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 Institut für Experimentalphysik, Freie Universität Berlin.

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*

In papers with more than one author, the asterisk indicates the name of the author to whom inquiries about the paper should be addressed.

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 Hebrew University of Jerusalem.

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 University of California.

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 Stanford University.

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 National Academy of Sciences of Belarus.

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 Institut für Chemie und Biochemie, Freie Universität Berlin.

Abstract

Three approaches are combined to study the electronic states' dynamics in the photodissociation of F2 and ClF in solid argon. These include (a) semiclassical surface-hopping simulations of the nonadiabatic processes involved. These simulations are carried out for the F2 molecule in a slab of 255 argon atoms with periodic boundary conditions at the ends. The full manifold of 36 electronic states relevant to the process is included. (b) The second approach involves quantum mechanical reduced-dimensionality models for the initial processes induced by a pump laser pulse, which involve wavepacket propagation for the preoriented ClF in the frozen argon lattice and incorporate the important electronic states. The focus is on the study of quantum coherence effects. (c) The final approach is femtosecond laser pump−probe experiments for ClF in Ar. The combined results for the different systems shed light on general properties of the nonadiabatic processes involved, including the singlet to triplet and intertriplet transition dynamics. The main findings are (1) that the system remains in the initially excited-state only for a very brief, subpicosecond, time period. Thereafter, most of the population is transferred by nonadiabatic transitions to other states, with different time constants depending on the systems. (2) Another finding is that the dynamics is selective with regard to the electronic quantum numbers, including the Λ and Ω quantum numbers, and the spin of the states. (3) The semiclassical simulations show that prior to the first “collision” of the photodissociated F atom with an Ar atom, the argon atoms can be held frozen, without affecting the process. This justifies the rigid-lattice reduced-dimensionality quantum model for a brief initial time interval. (4) Finally, degeneracies between triplets and singlets are fairly localized, but intertriplet degeneracies and near degeneracies can span an extensive range. The importance of quantum effects in photochemistry of matrix-isolated molecules is discussed in light of the results.

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History

  • Published In Issue September 27, 2007
  • Received March 5, 2007
    Revised May 21, 2007

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