The A–X transition of diatomic bismuth, Bi2, was revisited by laser induced fluorescence in solid Ne at 3 K. Molecular constants, i.e., vibrational frequencies of 137 cm–1 and 174 cm–1, were reproduced for… Click to show full abstract
The A–X transition of diatomic bismuth, Bi2, was revisited by laser induced fluorescence in solid Ne at 3 K. Molecular constants, i.e., vibrational frequencies of 137 cm–1 and 174 cm–1, were reproduced for the upper and lower electronic states as reported by Bondybey et al. [Chem. Phys. Lett. 76, 30 (1980)]. Two-dimensional mapping of emission spectra confirmed satellite bands in higher and lower excitation/emission energies for each of the major bands in the vibrational progression of v′–v″ (v′ = 0–5, v″ = 5–12). Based on the molecular orbital calculations, presence of clusters, Bi2Nen (n = 1–6), is proposed for possible carriers of the observed satellites. For the relatively large matrix shift of ∼67 cm−1 in solid Ne for the term energy of the A state, the diatomic bismuth is supposed to exist as a linearly coordinated cluster of Bi2Ne in the matrix.The A–X transition of diatomic bismuth, Bi2, was revisited by laser induced fluorescence in solid Ne at 3 K. Molecular constants, i.e., vibrational frequencies of 137 cm–1 and 174 cm–1, were reproduced for the upper and lower electronic states as reported by Bondybey et al. [Chem. Phys. Lett. 76, 30 (1980)]. Two-dimensional mapping of emission spectra confirmed satellite bands in higher and lower excitation/emission energies for each of the major bands in the vibrational progression of v′–v″ (v′ = 0–5, v″ = 5–12). Based on the molecular orbital calculations, presence of clusters, Bi2Nen (n = 1–6), is proposed for possible carriers of the observed satellites. For the relatively large matrix shift of ∼67 cm−1 in solid Ne for the term energy of the A state, the diatomic bismuth is supposed to exist as a linearly coordinated cluster of Bi2Ne in the matrix.
               
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