Electronic spectrum of TaO and its hyperfine structure

The B Φ 5 ∕ 2 2 − X 1 Δ 3 ∕ 2 2 ( 0 , 0 ) band at 778 nm and the C Δ 3 ∕ 2 2 − X 1 Δ 3 ∕ 2 2 ( 0 , 0 ) band at 737 nm of tantalum oxide (TaO) were recorded by laser excitation spectroscopy using a hollow cathode sputtering source to generate the molecules. The hyperfine structure arising from the Ta...

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Veröffentlicht in:The Journal of chemical physics 2008-03, Vol.128 (10), p.104302-104302-6
Hauptverfasser: Manke, Kara J., Vervoort, Tyson R., Kuwata, Keith T., Varberg, Thomas D.
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container_issue 10
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container_title The Journal of chemical physics
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creator Manke, Kara J.
Vervoort, Tyson R.
Kuwata, Keith T.
Varberg, Thomas D.
description The B Φ 5 ∕ 2 2 − X 1 Δ 3 ∕ 2 2 ( 0 , 0 ) band at 778 nm and the C Δ 3 ∕ 2 2 − X 1 Δ 3 ∕ 2 2 ( 0 , 0 ) band at 737 nm of tantalum oxide (TaO) were recorded by laser excitation spectroscopy using a hollow cathode sputtering source to generate the molecules. The hyperfine structure arising from the Ta 181 ( I = 7 ∕ 2 ) nucleus was measured at sub-Doppler resolution using the technique of intermodulated fluorescence spectroscopy. The hyperfine structure was assigned and fitted in order to derive accurate values for the magnetic dipole and electric quadrupole interactions. The magnetic hyperfine constant for the ground electronic state was also calculated using the density functional theory as h 3 ∕ 2 = 625 MHz , in good agreement with the experimental value of 647 ± 10 MHz . This result suggests that the X Δ 2 ground state of TaO is well described by a pure δ σ 2 electronic configuration, where the unpaired electron is located in a Ta 5 d δ orbital.
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title Electronic spectrum of TaO and its hyperfine structure
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