Zirconium isotope shift measurements using optogalvanic detection

Etienne Langlois; Jean-Marie Gagné

doi:10.1364/JOSAB.10.000774

Journal of the Optical Society of America B
Vol. 10,
Issue 5,
pp. 774-783
(1993)
•https://doi.org/10.1364/JOSAB.10.000774

Zirconium isotope shift measurements using optogalvanic detection

Etienne Langlois and Jean-Marie Gagné

Not Accessible

Your library or personal account may give you access

Get PDF
Email
Share
Get Citation
Copy Citation Text
Etienne Langlois and Jean-Marie Gagné, "Zirconium isotope shift measurements using optogalvanic detection," J. Opt. Soc. Am. B 10, 774-783 (1993)

Export Citation
- BibTex
- Endnote (RIS)
- HTML
- Plain Text
Citation alert
Save article

Abstract

Isotope shift measurements are reported for more than 300 zirconium lines in the spectral range 14 160–18 660 cm⁻¹. Most of these lines are predicted transitions between known energy levels, although several of them have not yet been reported. The zirconium vapor is produced in a homemade hollow-cathode lamp, and the atomic transitions are excited by a ring dye laser (dyes used: DCM, Rhodamine 6G, and Rhodamine 110). Light absorption in the vapor is detected by using the optogalvanic effect when either one or the other of two sub-Doppler techniques (intermodulation or saturation) is used, depending on the intensity of the line under study. Numerical values aside, our results also show that the optogalvanic effect is a useful tool for systematic high-resolution spectroscopic investigations.

Full Article | PDF Article

More Like This

Zirconium isotope shift measurement using laser pumping and optogalvanic detection

Etienne Langlois and Jean-Marie Gagné
J. Opt. Soc. Am. B 11(4) 552-557 (1994)

Hyperfine structures in ⁹¹Zr by saturation optogalvanic spectroscopy

G. Chevalier, J.-M. Gagné, and P. Pianarosa
J. Opt. Soc. Am. B 5(7) 1492-1499 (1988)

Optogalvanic measurement of isotope shifts of doubly ionized uranium (U iii) made using natural-U samples

K. N. Piyakis and J.-M. Gagné
J. Opt. Soc. Am. B 6(12) 2289-2294 (1989)

Previous Article Next Article

Cited By

You do not have subscription access to this journal. Cited by links are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Figures (6)

You do not have subscription access to this journal. Figure files are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Tables (1)

You do not have subscription access to this journal. Article tables are available to subscribers only. You may subscribe either as an Optica member, or as an authorized user of your institution.

Contact your librarian or system administrator
or
Login to access Optica Member Subscription

Measured Wave Number (cm⁻¹)	Ref.^a	Energy Levels		Calculated Wave Number (cm⁻¹)	Isotope Shifts (MHz) (Relative to ⁹⁰Zr)			Precision^b

		Lower	Upper		⁹²Zr	⁹⁴Zr	⁹⁶Zr
14 165.66	K	a³G₅	$x^{3} F_{4}^{\circ}$	14 165.64	−199	−382	−535	C
14 226.11	K	a⁵F₁	$z^{5} D_{1}^{\circ}$	14 226.00	−141	−311	−492	B
14 270.67	K	b³F₃	$x^{1} F_{3}^{\circ}$	14 270.64	−17	−107	−268	c
14 293.26	K	a⁵F₄	$z^{5} D_{4}^{\circ}$	14 293.22	−143	−307	−489	A
14 300.49	K	a⁵F₂	$z^{5} D_{2}^{\circ}$	14 300.43	−141	−308	−484	B
14 331.04	K	b³F₂	$y^{5} G_{3}^{\circ}$	14 330.99	−193	−339	−440	C
14 350.53	K	a³G₄	$x^{3} D_{3}^{\circ}$	14 350.50	−139	−295	−469	C
14 360.81		a³D₃	$v^{3} D_{2}^{\circ}$	14 360.81	−161	−326		e
14 376.52	K	a⁵F₃	$z^{5} D_{3}^{\circ}$	14 376.51	−138	−305	−493	C
14 387.64	K	a⁵P₃	$z^{5} P_{2}^{\circ}$	14 387.59	−141	−303	−479	C
14 421.01	K	b³F₂	$x^{3} F_{2}^{\circ}$	14 420.98	−98	−219	−361	B
14 423.33		b³F₄	$y^{5} G_{5}^{\circ}$	14 423.29	−249	−367		d
14 427.94	K	a³G₃	$z^{1} G_{4}^{\circ}$	14 427.91	−160	−323	−405	C
14 434.99	K	a³G₃	$x^{3} F_{4}^{\circ}$	14 434.98	−179	−352	−513	D
14 442.20	K	a³Gs	$y^{5} G_{6}^{\circ}$	14 442.11	−339			E
14 451.58		a³D₂	$v^{3} D_{1}^{\circ}$	14 451.73	−95	−208	−369	d
14 453.38	K	a⁵F₁	$z^{5} D_{2}^{\circ}$	14 453.31	−135	−302	−486	B
14 473.22	K	a⁵P₂	$z^{5} P_{1}^{\circ}$	14 473.22	−137	−300	−480	B
14 479.53	K	a³F₄	$z^{5} G_{4}^{\circ}$	14 479.52	−283	−460	−561	B
14 487.63	K	b³F₃	$x^{3} F_{3}^{\circ}$	14 487.55	−98	−227	−371	B
14 506.53		a¹G₄	$z^{3} G_{5}^{\circ}$	14 506.59	−305	−497		e
14 513.39	K	b³F₂	$x^{3} D_{1}^{\circ}$	14 513.41	−89	−222	−387	B
14 519.93	K			14 519.91	−98	−215		E
14 523.95	K	a³P₂	$z^{5} D_{3}^{\circ}$	14 523.90	−282	−462	−567	B
14 577.70	K	a³D₃	$v^{3} D_{3}^{\circ}$	14 577.79	−170	−326	−474	C
14 584.70	K	a⁵F₃	$z^{5} D_{4}^{\circ}$	14 584.71	−142	−300	−496	D
14 586.27	K	b³F₂	$x^{1} F_{3}^{\circ}$	14 586.25		−89	−232	E
14 589.02	K	b³F₄	$z^{1} G_{4}^{\circ}$	14 588.98	−123	−258	−355	C
14 596.02	K	b³F₄	$x^{3} F_{4}^{\circ}$	14 596.05	−140	−293	−439	B
14 600.10	K	a³P₁	$z^{5} D_{0}^{\circ}$	14 600.08	−291	−482	−601	C
14 600.87	K	b³F₃	$x^{3} D_{2}^{\circ}$	14 600.88	−104	−246	−406	B
14 602.12					−57	−149		E
14 602.21	K	a⁵F₂	$z^{5} D_{3}^{\circ}$	14 602.17	−141	−306	−493	B
14 604.53	K	a⁵P₁	$z^{5} P_{1}^{\circ}$	14 604.51	−136	−296	−483	B
14 618.61	K	a³G₃	$w^{3} D_{2}^{\circ}$	14 618.52	−90	−216	−369	D
14 629.37	K			14 629.35	160	270	351	D
14 630.93	K	a³F₃	$z^{5} G_{3}^{\circ}$	14 630.85	−281	−458	−565	B
14 639.77	K	a⁵P₃	$z^{5} P_{3}^{\circ}$	14 639.78	−154	−321	−479	C

Abstract

Cited By

Figures (6)

Tables (1)

Journal of the Optical Society of America B