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Characterization of the ground state of Br2 by laser-induced fluorescence Fourier transform spectroscopy of the B3∏0+u-X1∑g+ system. Focsa C,Li H,Bernath P F. Journal of Molecular Spectroscopy . 2000
[2]
Studies on the vibrational, rovibrational energies and vibrational force constants of diatomic molecular states using algebraic and variational methods. Sun W G,Hou S L,Feng H,et al. Journal of Molecular Spectroscopy . 2002
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Vibrational-state-to-state collision-induced intramolecular energy transfer N2(A3∑u+, v11 →B3∏g,v1). Bachmann R,Li X,Ottinger Ch,et al. The Journal of Chemical Physics . 1993
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The spectrum of molecular Nitrogen. Lofthus A,Krupenie P H. Journal of Physical and Chemical Reference Data . 1977
[5]
Fine structure of the schumann-runge bands near the convergence limit and the dissociation energy of the oxygen molecule. Brix P,Herzberg G. Canadian Journal of Physics . 1954
[6]
Transition probabilities in the A~2∑~+-X~2∏_i electronic system of OH. Luque J,Crosley D. The Journal of Chemical Physics . 1998
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The calculation of potential-energy curves from band-spectroscopic data. Rees A L G. Proceedings of the Physical Society . 1947
[8]
The energy levels of a rotating vibrator. Dunham J L. Physical Review . 1932
[9]
The B3∏0u+-X1∑g+system of Br2: rotational analysis, Frank-Condon factors, and ??long rang potential in the B3∏0u+ state. Barrow R F,Clark T C,Coxon J A,et al. Journal of Molecular Spectroscopy . 1974
[10]
The B3∏（Ou+）←X1∑g system of 79 Br79 Br. Coxon J A. Journal of Molecular Spectroscopy . 1971