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 |
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Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
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Zusammenfassung: | 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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ISSN: | 0021-9606 1089-7690 |
DOI: | 10.1063/1.2837470 |