Ground and low-lying excited states of DyCl studied by the four-component relativistic configuration interaction methods
The ground and low-lying excited states of the DyCl molecule are investigated by the four-component relativistic CI methods. Electronic states are classified into so-called families by applying the f -shell Omega decomposition method to the CI wavefunctions, and the characters of the states are clar...
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Veröffentlicht in: | Theoretical chemistry accounts 2018-08, Vol.137 (8), p.1-10, Article 112 |
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Sprache: | eng |
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Zusammenfassung: | The ground and low-lying excited states of the DyCl molecule are investigated by the four-component relativistic CI methods. Electronic states are classified into so-called families by applying the
f
-shell Omega decomposition method to the CI wavefunctions, and the characters of the states are clarified. The
X
7.5 ground state may be described as Dy
+
[(4
f
)
9
(6
s
)
2
]Cl
−
, but at large nuclear distance (
R
> 4.80 au), beyond the equilibrium nuclear distance (4.724 au), the dominant configuration changes to Dy
+
[(4
f
)
10
(6
s
)
1
]Cl
−
. The dominant configuration of Dy
+
[(4
f
)
9
(6
s
)
2
]F
−
is retained in DyF, but the dominant configuration in DyCl changes drastically as
R
increases. The calculated value (231 cm
−1
) of the vibrational frequency (
ω
e
) agrees well with the value of 233 cm
−1
observed by Linton et al. (J Mol Spectrosc 232:30–39,
2005
). This low frequency reflects the weakness of the Cl
−
ligand compared to F
−
. The
Y
[0.15]8.5,
Z
[0.85]7.5, and [0.97] states observed by Linton et al. are found to have a dominant configuration of [(4
f
)
10
(6
s
)
1
], and the
A
[16.4]8.5 and
B
[15.4]Ω states observed both have (4
f
)
10
([6
p
1/2,1/2
])
1
, belonging to different families. (The number in square brackets denotes the excitation energy in unit of k cm
−1
, and the number after a right square bracket denotes an
Ω
value.) The
Ω
value of the
B
[15.4]
Ω
state, which has not been determined experimentally, is calculated to be 6.5. |
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ISSN: | 1432-881X 1432-2234 |
DOI: | 10.1007/s00214-018-2296-y |