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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 95-103 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We report absorption, laser fluorescence, and Raman spectra for Re2 in an argon matrix prepared by the mass-selected ion deposition technique. The dirhenium absorption spectrum consists of seven band systems (A–G) extending from the near infrared into the ultraviolet region. For the A system (a simple vibrational progression), we find T0=10 817(1) cm−1, ωe=317.1(5) cm−1 and ωexe=1.0(1) cm−1. A Franck–Condon analysis of the A system intensities predicts that this state has a smaller equilibrium internuclear distance than the ground state (Δre=−0.073 A(ring)), in violation of Badger's rule. The B system starts at 13 250 cm−1 and consists of four overlapping (and possibly perturbed) subsystems, whose average vibrational spacing is 270(11) cm−1. The C, D, E, and F systems (vibrational spacings in parentheses) are centered at 22 300 cm−1 (210 cm−1), 24 500 cm−1 (195 cm−1), 29 150 cm−1 (175 cm−1), and 32 900 cm−1 (160 cm−1), respectively. Weak fluorescence spectra, obtained upon laser excitation into the A system, were characterized by vibrational progressions to the dimer ground (X) state and to a low lying (X') state for which T0=357.6(5) cm−1 and ωe=332.3(2) cm−1. Raman and fluorescence progressions to the ground state were observed when the B system was excited. These data give ωe=337.9(49) cm−1 for the dimer ground state in good agreement with measurements from photodetachment spectra [J. Am. Chem. Soc. 108, 178 (1986)]. We propose likely assignments for the low lying electronic states of Re2 and discuss our results in terms of the bonding in the other group VIIB dimers, Mn2 and Tc2.
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