We have used conventional high resolution optical spectroscopic methods to determine the principal values of the fine structure tensor for the lowest triplet state (B31 at 18 959 cm−1) of NO2− in Na NO2 single crystals. From the intensities in the Zeeman spectrum we find D − E = 0.86 ± 0.04 cm−1, D + E = 0.40 ± 0.04 cm−1, where the z axis is taken as the twofold axis and E = (Z − X) / 2. From the measurement of line positions in the high-field Zeeman spectrum we find D − E = 0.84 ± 0.05 cm−1, D + E = 0.41 ± 0.05 cm−1. The values of D and E calculated for one-center spin–spin interaction are D − E = 0.42 cm−1 and D + E = 0.24 cm−1. The calculated ordering of the spin states is the same as that observed, but we suggest that there is significant second-order spin–orbit energy associated with the real splittings. Roughly the same splittings are seen for different vibronic levels of B31 associated with ν2′.
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Hochstrasser et al. (1971) studied this question.
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