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Rotational and hyperfine analysis of the C 4Σ−- X 4Σ− (blue) system of niobium oxide, NbO

Identifieur interne : 003936 ( Main/Exploration ); précédent : 003935; suivant : 003937

Rotational and hyperfine analysis of the C 4Σ−- X 4Σ− (blue) system of niobium oxide, NbO

Auteurs : G. Cheval [France] ; J.-L Femenias [France] ; A. J Merer [Canada] ; U. Sassenberg [Suède]

Source :

RBID : ISTEX:022B83C10B67C061CAFCD9B8DCFB3523D7C85F1A

Abstract

The C4Σ−-X4Σ− (0, 0) band of NbO, whose R heads lie near 4690 Å, has been analyzed from high-resolution grating spectra. Both 4Σ− states have second-order spin-orbit splittings, 4λ = E(4Σ 3 2)-E(4Σ 1 2), of about 60 cm−1, so that they are in good case (a) coupling at low J, although the appearance of the band had been interpreted by previous workers as 4Σ(b)-4Σ(b). the 93Nb nuclear hyperfine structure (I= 9 2) is very impressive in the R1, P1, R4, and P4 branches, with the 10 hyperfine components of a rotational line spread over more than 0.9 cm−1 in the F1 branches. The hyperfine linewidths vary considerably with J, in the manner expected for the rapid spin uncoupling from case (aβ) to (bβJ) which occurs in a high-multiplicity state. The very great hyperfine linewidths arise because the sign of the Fermi contact parameter b (the coefficient of I·S in the magnetic hyperfine Hamiltonian) is different in the two 4Σ states, so that the observed patterns are the sums of the splittings in the two electronic states.

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DOI: 10.1016/0022-2852(88)90111-7


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<div type="abstract" xml:lang="en">The C4Σ−-X4Σ− (0, 0) band of NbO, whose R heads lie near 4690 Å, has been analyzed from high-resolution grating spectra. Both 4Σ− states have second-order spin-orbit splittings, 4λ = E(4Σ 3 2)-E(4Σ 1 2), of about 60 cm−1, so that they are in good case (a) coupling at low J, although the appearance of the band had been interpreted by previous workers as 4Σ(b)-4Σ(b). the 93Nb nuclear hyperfine structure (I= 9 2) is very impressive in the R1, P1, R4, and P4 branches, with the 10 hyperfine components of a rotational line spread over more than 0.9 cm−1 in the F1 branches. The hyperfine linewidths vary considerably with J, in the manner expected for the rapid spin uncoupling from case (aβ) to (bβJ) which occurs in a high-multiplicity state. The very great hyperfine linewidths arise because the sign of the Fermi contact parameter b (the coefficient of I·S in the magnetic hyperfine Hamiltonian) is different in the two 4Σ states, so that the observed patterns are the sums of the splittings in the two electronic states.</div>
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