15min:
MAGNETIC ROTATION STUDY OF THE A3 Pi1u--X1 Sigma+g SYSTEM OF 79Br2.

C. D. BOONE, A. CHAND, F. W. DALBY AND I. OZIER, Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, BC, Canada, V6T 1Z1.

The magnetic rotation spectrum of 79Br2 has been measured from 14,988 to 15,488 cm-1 using a tunable, cw dye laser (effective linewidth sim 2 MHz) with DCM dye. The study was carried out using a cell filled to sim6.5 Torr with 99.4% isotopically pure 79Br2. Over 5000 transitions (with Doppler width of about 450 MHz) were measured, the majority of which (> 4500) belong to the A3 Pi1u--X1 Sigma+g system of the molecule. The range of upper-state vibrational levels observed (v' = 13 to 38) extended very close to the dissociation limit of the A state. With more standard techniques such as absorption or fluorescence, transitions in the A--X system are typically difficult to detect because of much stronger transitions in the same region from the B3 Pi_0+u--X1 Sigma+g system; the opposite is true for magnetic rotation, due to magnetic activity of the A3 Pi1u electronic state.

Magnetic rotation signals normally get weaker with increasing J, since the effective g-factor, gJ, decreases as J increases. As a result, magnetic rotation spectra usually give strong signals only for low-J transitions. For the A--X system of Br2, however, an interference effect between spin-uncoupling and magnetic mixing to other electronic states---primarily the A'3 Pi2u state---led to the measurement of rotational transitions right up to the breaking-off point (e.g. J = 82 for v' = 25). These high-J transitions were comparable in strength with those at low-J. The interference effect manifests itself as the addition to gJ of a term that increases with J.

Structure observed in low-J transitions has been attributed to hyperfine effects in the A state. Transitions to quasi-bound levels above the dissociation limit of the A state appear to suffer from strong, systematic perturbations, likely due to interaction with a dissociative state. Perhaps the most interesting feature of the spectrum is a series of extra lines tentatively identified as belonging to the A'3 Pi2u--X1 Sigma+g system, the result of intensity-borrowing from near-resonant perturbations with the A state v' = 27 rotational levels 2 \le J \le 31.

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