The 3d<sup>2</sup>–3d4f transitions in V iv†

George V. Shalimoff; John G. Conway

doi:10.1364/JOSA.68.000267

Journal of the Optical Society of America
Vol. 68,
Issue 2,
pp. 267-268
(1978)
•https://doi.org/10.1364/JOSA.68.000267

The 3d²–3d4f transitions in V iv

George V. Shalimoff and John G. Conway

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George V. Shalimoff and John G. Conway, "The 3d²–3d4f transitions in V iv†," J. Opt. Soc. Am. 68, 267-268 (1978)

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Abstract

Nineteen transitions from the ground configuration 3d² to the 3d4f configuration and three transitions from ground to the 3d5p configurations have been observed and measured in the 378–402 Å region for vandanium iv.

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Corrections

George V. Shalimoff and John G. Conway, "Errata: The 3d²–3d4f transitions in V iv," J. Opt. Soc. Am. 68, 1292_1-1292 (1978)
https://opg.optica.org/josa/abstract.cfm?uri=josa-68-9-1292_1

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				Levels^a
λ(Å)	Int.	σ(cm⁻¹)	Classification	Odd	Even	Δ^b
378.678	3	264 076.6	$3 d 4 f {{}^{3}G}_{4}^{o} - 3 d^{2} {{}^{3}F}_{3}$	264 401.9–	325.4	+0.1
378.929	4	263 901.7	$3 d 4 f {{}^{3}G}_{3}^{o} - 3 d^{2} {{}^{3}F}_{2}$	263 902.3–	0	−0.6
378.993	4	263 857.1	$3 d 4 f {{}^{3}G}_{5}^{o} - 3 d^{2} {{}^{3}F}_{4}$	264 591.9–	734.7	−0.1
379.093	4	263 787.5	$3 d 4 f {{}^{3}F}_{4}^{o} - 3 d^{2} {{}^{3}F}_{3}$	264 113.1–	325.4	−0.2
379.353	5	263 606.7	$3 d 4 f {{}^{3}F}_{3}^{o} - 3 d^{2} {{}^{3}F}_{2}$	263 608.3–	0	−1.6
379.372	3	263 593.5	$3 d 4 f {{}^{3}F}_{2}^{o} - 3 d^{2} {{}^{3}F}_{2}$	263 593.0–	0	+0.5
379.395	3	263 577.5	$3 d 4 f {{}^{3}G}_{3}^{o} - 3 d^{2} {{}^{3}F}_{3}$	263 902.3–	325.4	+0.6
379.512	5	263 496.3	$3 d 4 f {{}^{3}H}_{4}^{o} - 3 d^{2} {{}^{3}F}_{3}$	263 822.4–	325.4	−0.7
379.613	7	263 426.9	$3 d 4 f {{}^{3}H}_{5}^{o} - 3 d^{2} {{}^{3}F}_{4}$	264 161.8–	734.7	−0.2
379.682	4	263 378.3	$3 d 4 f {{}^{3}F}_{4}^{o} - 3 d^{2} {{}^{3}F}_{4}$	264 113.1–	734.7	−0.1
380.101	0	263 088.0	$3 d 4 f {{}^{3}F}_{4}^{o} - 3 d^{2} {{}^{3}F}_{4}$	263 822.4–	734.7	+0.3
380.537	0	262 786.5	$3 d 4 f {{}^{1}G}_{4}^{o} - 3 d^{2} {{}^{3}F}_{3}$	263 111.4–	325.4	+0.5
391.362	0	255 517.9	$3 d 5 p {{}^{3}F}_{4}^{o} - 3 d^{2} {{}^{3}F}_{4}$	265 251.7–	734.7	+0.9
392.428	3	254 823.8	$3 d 5 p {{}^{3}D}_{1}^{o} - 3 d^{2} {{}^{3}F}_{2}$	254 824.1–	0	−0.3
392.602	2	254 710.9	$3 d 5 p {{}^{3}D}_{3}^{o} - 3 d^{2} {{}^{3}F}_{4}$	255 445.5–	734.7	+0.1
393.217	0	254 312.5	$3 d 4 f {{}^{3}D}_{3}^{o} - 3 d^{2} {{}^{1}D}_{2}$	265 271.6–	10 959.3	+0.2
393.790	4	253 942.5	$3 d 4 f {{}^{1}F}_{3}^{o} - 3 d^{2} {{}^{1}D}_{2}$	264 902.2–	10 959.3	−0.4
394.441	3	253 523.3	$3 d 4 f {{}^{1}D}_{2}^{o} - 3 d^{2} {{}^{1}D}_{2}$	264 482.8–	10 959.3	−0.2
396.991	0	251 894.9	$3 d 4 f {{}^{3}D}_{1}^{o} - 3 d^{2} {{}^{3}P}_{o}$	265 019.7–	13 122.8	−2.0
397.097	3	251 827.6	$3 d 4 f {{}^{3}D}_{2}^{o} - 3 d^{2} {{}^{3}P}_{1}$	265 067.4–	13 239.2	−0.6
397.122	4	251 811.8	$3 d 4 f {{}^{3}D}_{3}^{o} - 3 d^{2} {{}^{3}P}_{2}$	265 271.6–	13 458.3	−1.5
402.885	6	248 209.8	$3 d 4 f {{}^{1}H}_{5}^{o} - 3 d^{2} {{}^{1}G}_{4}$	266 600.3–	18 391.2	+0.7

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