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Optical absorption spectra of Na/Ar systems are calculated by combining the classical Monte Carlo simulation method with a quantum mechanical first-order perturbation scheme [Balling and Wright, J. Chem. Phys. 79, 2941 (1983)] for estimating the energies of the Na* 3p(2P) excited states. The model incorporates many drastic approximations, but contains no adjustable parameters. Our Na/Ar matrix simulations generated relaxed structures for several candidate trapping sites based on various sized vacancies in face-centered-cubic (fcc) solid Ar. Trapping sites for which the equilibrium structures belong to the Oh or Td point groups yielded the experimentally well-known ‘‘triplet’’ absorption line shape; for these cases, the splitting of the degeneracy of the excited Na* 3p(2P) state is due solely to fluctuations away from the equilibrium structures. Simulations of Na/Ar clusters, surfaces, and matrix sites possessing a strong permanent axial asymmetry yielded a widely split ‘‘doublet plus singlet’’ absorption line shape. Despite our success at reproducing several qualitative aspects of the absorption spectroscopy of Na/Ar matrices, our simulations failed to quantitatively reproduce the experimental data. We discuss the major limitations of our model, as well as several possible improvements.
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Boatz et al. (1994) studied this question.
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