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Conference Paper: Electronic transitions of tungsten monosulfide

TitleElectronic transitions of tungsten monosulfide
Authors
Issue Date2017
Publisher The 1st Meeting: Asian Workshop on Molecular Spectroscopy.
Citation
The 1st Meeting of the Asian Workshop on Molecular Spectroscopy, Kyoto University, Kyoto, Japan, 20-21 May 2017. In Program and Abstracts Book, p. 53, Paper B08 How to Cite?
AbstractElectronic transition spectrum of the tungsten monosulfide (WS) molecule in the near infrared region between 725 nm and 885 nm has been recorded using laser ablation/reaction free-jet expansion and laser induced fluorescence spectroscopy. The WS molecule was produced by reacting laser - ablated tungsten atoms with 1% CS2 seeded in argon. Fifteen vibrational bands with resolved rotational structure have been recorded and analyzed, which were organized into seven electronic transition systems. The ground state has been identified to be the X3 Σ-(0+) state with bond length, ro, and vibrational frequency, Δ G1/2, determined to be 2.0676 Å and 556.7 cm-1 respectively. In addition, vibrational bands with Ω = 1 component in lower state have also been analyzed. Least-squares fit of the measured line positions yielded molecular constants for the electronic states involved. Spectroscopic constants and potential energy curves of 30 low-lying Λ-S states and Ω sub-states of the WS molecule have been calculated using state-averaged complete active space self-consistent field (SA-CASSCF) and followed by MRCISD+Q (internally contracted multi-reference configuration interaction with singles and doubles plus Davidson’s cluster correction). The active space consists of 10 electrons in 9 orbitals corresponding to the W 5d6s and S 3p shells. The lower molecular orbitals from W 5s5p and S 3s are inactive but are also correlated, and relativistic effective core potential (RECPs) are adopted to replace the core orbitals with 60 (W) and 10 (S) core electrons, respectively. The spin-orbit coupling (SOC) is calculated via the state-interaction (SI) approach with RECP spin-orbit operators using SA-CASSCF wavefunctions, where the diagonal elements in the SOC matrix are replaced by the corresponding MRCISD+Q energies calculated above. The calculated spectroscopic properties of the ground and lowlying electronic states are generally in good agreement with our experimental determinations. This work represents the first experimental investigation of the electronic and molecular structure of the WS molecule.
Persistent Identifierhttp://hdl.handle.net/10722/247743

 

DC FieldValueLanguage
dc.contributor.authorTsang, LF-
dc.contributor.authorChan, MC-
dc.contributor.authorZou, W-
dc.contributor.authorCheung, ASC-
dc.date.accessioned2017-10-18T08:31:56Z-
dc.date.available2017-10-18T08:31:56Z-
dc.date.issued2017-
dc.identifier.citationThe 1st Meeting of the Asian Workshop on Molecular Spectroscopy, Kyoto University, Kyoto, Japan, 20-21 May 2017. In Program and Abstracts Book, p. 53, Paper B08-
dc.identifier.urihttp://hdl.handle.net/10722/247743-
dc.description.abstractElectronic transition spectrum of the tungsten monosulfide (WS) molecule in the near infrared region between 725 nm and 885 nm has been recorded using laser ablation/reaction free-jet expansion and laser induced fluorescence spectroscopy. The WS molecule was produced by reacting laser - ablated tungsten atoms with 1% CS2 seeded in argon. Fifteen vibrational bands with resolved rotational structure have been recorded and analyzed, which were organized into seven electronic transition systems. The ground state has been identified to be the X3 Σ-(0+) state with bond length, ro, and vibrational frequency, Δ G1/2, determined to be 2.0676 Å and 556.7 cm-1 respectively. In addition, vibrational bands with Ω = 1 component in lower state have also been analyzed. Least-squares fit of the measured line positions yielded molecular constants for the electronic states involved. Spectroscopic constants and potential energy curves of 30 low-lying Λ-S states and Ω sub-states of the WS molecule have been calculated using state-averaged complete active space self-consistent field (SA-CASSCF) and followed by MRCISD+Q (internally contracted multi-reference configuration interaction with singles and doubles plus Davidson’s cluster correction). The active space consists of 10 electrons in 9 orbitals corresponding to the W 5d6s and S 3p shells. The lower molecular orbitals from W 5s5p and S 3s are inactive but are also correlated, and relativistic effective core potential (RECPs) are adopted to replace the core orbitals with 60 (W) and 10 (S) core electrons, respectively. The spin-orbit coupling (SOC) is calculated via the state-interaction (SI) approach with RECP spin-orbit operators using SA-CASSCF wavefunctions, where the diagonal elements in the SOC matrix are replaced by the corresponding MRCISD+Q energies calculated above. The calculated spectroscopic properties of the ground and lowlying electronic states are generally in good agreement with our experimental determinations. This work represents the first experimental investigation of the electronic and molecular structure of the WS molecule.-
dc.languageeng-
dc.publisher The 1st Meeting: Asian Workshop on Molecular Spectroscopy. -
dc.relation.ispartofFirst Asian Workshop on Molecular Spectroscopy, 2017-
dc.titleElectronic transitions of tungsten monosulfide-
dc.typeConference_Paper-
dc.identifier.emailCheung, ASC: hrsccsc@hkucc.hku.hk-
dc.identifier.authorityCheung, ASC=rp00676-
dc.identifier.hkuros281324-
dc.identifier.spage53, Paper B08-
dc.identifier.epage53, Paper B08-
dc.publisher.placeJapan-

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