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Article: Laser spectroscopy of VO: Analysis of the rotational and hyperfine structure of the C4Σ--X4Σ- (0, 0) band
Title | Laser spectroscopy of VO: Analysis of the rotational and hyperfine structure of the C4Σ--X4Σ- (0, 0) band |
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Authors | |
Issue Date | 1982 |
Publisher | Academic Press. The Journal's web site is located at http://www.elsevier.com/locate/yjmsp |
Citation | Journal Of Molecular Spectroscopy, 1982, v. 91 n. 1, p. 165-208 How to Cite? |
Abstract | The (0, 0) band of the C 4Σ --X 4Σ - electronic transition of VO was recorded by intermodulated laser-induced fluorescence at a resolution of about 100 MHz over the range 17 300-17 427 cm -1. The hyperfine structure caused by the 51V nucleus (I = 7 2) is almost completely resolved, and provides good examples of case (b βJ) coupling in both electronic states. Internal hyperfine perturbations between the F 2 and F 3 electron spin components (where N = J - 1 2 and J + 1 2, respectively) occur in both electronic states; these are caused by hyperfine matrix elements of the type ΔJ = ±1, and induce hundreds of extra hyperfine lines which permit the courses of the electron spin and hyperfine levels to be followed in detail. In the band center observations of Q lines, center dips and transitions with ΔF ≠ ΔJ have allowed the hyperfine and electron spin constants for the two electronic states to be determined separately despite the parallel polarization of the electronic transition. Numerous local electronic-rotational perturbations occur in the C 4Σ - state, which have required that the line positions be corrected for their effects before meaningful centrifugal distortion constants could be obtained. The C 4Σ - state also suffers from large spin-orbit perturbations by distant electronic states, for which it has been necessary to introduce a second spin-rotation parameter, γ S, following the formalism of Brown and Milton. The corresponding isotropic hyperfine parameter b S is also required. Both γ S and b S result from third-order cross-terms involving the spin-orbit interaction; given sufficient resolution they are always needed in a full description of electronic states of quartet and higher multiplicity. © 1982. |
Persistent Identifier | http://hdl.handle.net/10722/147710 |
ISSN | 2023 Impact Factor: 1.4 2023 SCImago Journal Rankings: 0.374 |
ISI Accession Number ID |
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Cheung, ASC | en_HK |
dc.contributor.author | Hansen, RC | en_HK |
dc.contributor.author | Merer, AJ | en_HK |
dc.date.accessioned | 2012-05-29T06:08:50Z | - |
dc.date.available | 2012-05-29T06:08:50Z | - |
dc.date.issued | 1982 | en_HK |
dc.identifier.citation | Journal Of Molecular Spectroscopy, 1982, v. 91 n. 1, p. 165-208 | en_HK |
dc.identifier.issn | 0022-2852 | en_HK |
dc.identifier.uri | http://hdl.handle.net/10722/147710 | - |
dc.description.abstract | The (0, 0) band of the C 4Σ --X 4Σ - electronic transition of VO was recorded by intermodulated laser-induced fluorescence at a resolution of about 100 MHz over the range 17 300-17 427 cm -1. The hyperfine structure caused by the 51V nucleus (I = 7 2) is almost completely resolved, and provides good examples of case (b βJ) coupling in both electronic states. Internal hyperfine perturbations between the F 2 and F 3 electron spin components (where N = J - 1 2 and J + 1 2, respectively) occur in both electronic states; these are caused by hyperfine matrix elements of the type ΔJ = ±1, and induce hundreds of extra hyperfine lines which permit the courses of the electron spin and hyperfine levels to be followed in detail. In the band center observations of Q lines, center dips and transitions with ΔF ≠ ΔJ have allowed the hyperfine and electron spin constants for the two electronic states to be determined separately despite the parallel polarization of the electronic transition. Numerous local electronic-rotational perturbations occur in the C 4Σ - state, which have required that the line positions be corrected for their effects before meaningful centrifugal distortion constants could be obtained. The C 4Σ - state also suffers from large spin-orbit perturbations by distant electronic states, for which it has been necessary to introduce a second spin-rotation parameter, γ S, following the formalism of Brown and Milton. The corresponding isotropic hyperfine parameter b S is also required. Both γ S and b S result from third-order cross-terms involving the spin-orbit interaction; given sufficient resolution they are always needed in a full description of electronic states of quartet and higher multiplicity. © 1982. | en_HK |
dc.language | eng | en_US |
dc.publisher | Academic Press. The Journal's web site is located at http://www.elsevier.com/locate/yjmsp | en_HK |
dc.relation.ispartof | Journal of Molecular Spectroscopy | en_HK |
dc.title | Laser spectroscopy of VO: Analysis of the rotational and hyperfine structure of the C4Σ--X4Σ- (0, 0) band | en_HK |
dc.type | Article | en_HK |
dc.identifier.email | Cheung, ASC:hrsccsc@hku.hk | en_HK |
dc.identifier.authority | Cheung, ASC=rp00676 | en_HK |
dc.description.nature | link_to_subscribed_fulltext | en_US |
dc.identifier.doi | 10.1016/0022-2852(82)90039-X | - |
dc.identifier.scopus | eid_2-s2.0-0001579203 | en_HK |
dc.identifier.volume | 91 | en_HK |
dc.identifier.issue | 1 | en_HK |
dc.identifier.spage | 165 | en_HK |
dc.identifier.epage | 208 | en_HK |
dc.identifier.isi | WOS:A1982MY67200014 | - |
dc.publisher.place | United States | en_HK |
dc.identifier.scopusauthorid | Cheung, ASC=7401806538 | en_HK |
dc.identifier.scopusauthorid | Hansen, RC=24517867700 | en_HK |
dc.identifier.scopusauthorid | Merer, AJ=6603864922 | en_HK |
dc.identifier.issnl | 0022-2852 | - |