Vanadium-pumped titanium x-ray laser

Joseph Nilsen

doi:10.1364/OL.15.000798

Optics Letters
Vol. 15,
Issue 14,
pp. 798-800
(1990)
•https://doi.org/10.1364/OL.15.000798

Vanadium-pumped titanium x-ray laser

Joseph Nilsen

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Joseph Nilsen, "Vanadium-pumped titanium x-ray laser," Opt. Lett. 15, 798-800 (1990)

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Abstract

A new laboratory x-ray laser is described that is resonantly photopumped by two 3d → 2p emission lines in fluorinelike vanadium (Z = 23) and lases on several 3p → 3s transitions in neonlike titanium (Z = 22). Calculations show that five of the laser lines have gains greater than 5 cm⁻¹ for reasonable values of the pump lines, with the shortest wavelength of the five being at 32.65 nm.

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Transition	Wavelength (nm)	Gain (cm⁻¹)

		n_λ = 0.005	n_λ = 0.010	n_λ = 0.020
${\overset{̅}{2 p}}_{1 / 2} 3 p_{1 / 2} (J = 0) \to {\overset{̅}{2 p}}_{1 / 2} 3 s_{1 / 2} (J = 1)$	32.65	2.90	6.81	9.91
${\overset{̅}{2 p}}_{1 / 2} 3 p_{3 / 2} (J = 2) \to {\overset{̅}{2 p}}_{1 / 2} 3 s_{1 / 2} (J = 1)$	47.19		0.56	2.18
${\overset{̅}{2 p}}_{1 / 2} 3 p_{3 / 2} (J = 1) \to {\overset{̅}{2 p}}_{1 / 2} 3 s_{1 / 2} (J = 1)$	47.30	2.10	5.45	8.78
${\overset{̅}{2 p}}_{1 / 2} 3 p_{1 / 2} (J = 1) \to {\overset{̅}{2 p}}_{1 / 2} 3 s_{1 / 2} (J = 1)$	50.56	2.90	7.44	11.88
${\overset{̅}{2 p}}_{3 / 2} 3 p_{3 / 2} (J = 0) \to {\overset{̅}{2 p}}_{1 / 2} 3 s_{1 / 2} (J = 1)$	50.75	1.26	2.92	4.13
${\overset{̅}{2 p}}_{1 / 2} 3 p_{1 / 2} (J = 0) \to {\overset{̅}{2 p}}_{3 / 2} 3 s_{1 / 2} (J = 1)$	28.52	1.35	3.14	4.48
${\overset{̅}{2 p}}_{3 / 2} 3 p_{3 / 2} (J = 0) \to {\overset{̅}{2 p}}_{3 / 2} 3 s_{1 / 2} (J = 1)$	41.43	2.99	6.83	9.43
${\overset{̅}{2 p}}_{3 / 2} 3 p_{3 / 2} (J = 2) \to {\overset{̅}{2 p}}_{3 / 2} 3 s_{1 / 2} (J = 1)$	45.89	0.56	2.13	4.33
${\overset{̅}{2 p}}_{3 / 2} 3 p_{3 / 2} (J = 1) \to {\overset{̅}{2 p}}_{3 / 2} 3 s_{1 / 2} (J = 1)$	47.78	3.19	8.38	13.09
${\overset{̅}{2 p}}_{3 / 2} 3 p_{1 / 2} (J = 2) \to {\overset{̅}{2 p}}_{3 / 2} 3 s_{1 / 2} (J = 1)$	50.74	1.30	4.15	7.75

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Optics Letters