Excited state Faraday anomalous dispersion optical filters based on indirect laser pumping

Longfei Yin; Bin Luo; Zhongjie Chen; Lei Zhong; Hong Guo

doi:10.1364/OL.39.000842

Optics Letters
Vol. 39,
Issue 4,
pp. 842-844
(2014)
•https://doi.org/10.1364/OL.39.000842

Excited state Faraday anomalous dispersion optical filters based on indirect laser pumping

Longfei Yin, Bin Luo, Zhongjie Chen, Lei Zhong, and Hong Guo

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Longfei Yin, Bin Luo, Zhongjie Chen, Lei Zhong, and Hong Guo, "Excited state Faraday anomalous dispersion optical filters based on indirect laser pumping," Opt. Lett. 39, 842-844 (2014)

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Abstract

The direct pump method now used in excited state Faraday anomalous dispersion optical filters (ES-FADOFs) requires that the transition between the target and the ground state is an electric dipole allowed transition and that a laser that operates at the exact pump wavelength is available. This is not always satisfied in practice. An indirect laser pump method for ES-FADOF is proposed and experimentally realized. Compared with the commonly used direct pump method, this indirect pump method can reach the same performance using lasers at very different wavelengths. This method can greatly extend the wavelength range of FADOF and provide a novel scheme for ES-FADOF design.

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No.	Transition	$λ$ (nm)	$A_{k i} (s^{- 1})$
1	$6 {{}^{2}P}_{1 / 2} \to 5 {{}^{2}S}_{1 / 2}$	421.667	$1.5 \times 10^{6}$
2	$5 {{}^{2}P}_{3 / 2} \to 5 {{}^{2}S}_{1 / 2}$	780.235	$3.81 \times 10^{7}$
3	$5 {{}^{2}P}_{1 / 2} \to 5 {{}^{2}S}_{1 / 2}$	794.972	$3.61 \times 10^{7}$
4	$6 {{}^{2}S}_{1 / 2} \to 5 {{}^{2}P}_{1 / 2}$	1323.867	$6.6 \times 10^{6}$
5	$6 {{}^{2}S}_{1 / 2} \to 5 {{}^{2}P}_{3 / 2}$	1366.863	$1.29 \times 10^{7}$
6	$4 {{}^{2}D}_{3 / 2} \to 5 {{}^{2}P}_{1 / 2}$	1475.631	$1.07 \times 10^{7}$
7	$4 {{}^{2}D}_{3 / 2} \to 5 {{}^{2}P}_{3 / 2}$	1529.248	$2.0 \times 10^{6}$
8	$6 {{}^{2}P}_{1 / 2} \to 4 {{}^{2}D}_{3 / 2}$	2293.853	$2.4 \times 10^{6}$
9	$6 {{}^{2}P}_{1 / 2} \to 6 {{}^{2}S}_{1 / 2}$	2791.274	$4.3 \times 10^{6}$

State	$5 {{}^{2}S}_{1 / 2}$	$5 {{}^{2}P}_{1 / 2}$	$5 {{}^{2}P}_{3 / 2}$	$4 {{}^{2}D}_{3 / 2}$	$6 {{}^{2}S}_{1 / 2}$	$6 {{}^{2}P}_{1 / 2}$
Population probability	40.5%	3.6%	3.1%	7.1%	8.2%	37.3%

No.	Transition	$λ$ (nm)	$A_{k i} (s^{- 1})$
1	$6 {{}^{2}P}_{1 / 2} \to 5 {{}^{2}S}_{1 / 2}$	421.667	$1.5 \times 10^{6}$
2	$5 {{}^{2}P}_{3 / 2} \to 5 {{}^{2}S}_{1 / 2}$	780.235	$3.81 \times 10^{7}$
3	$5 {{}^{2}P}_{1 / 2} \to 5 {{}^{2}S}_{1 / 2}$	794.972	$3.61 \times 10^{7}$
4	$6 {{}^{2}S}_{1 / 2} \to 5 {{}^{2}P}_{1 / 2}$	1323.867	$6.6 \times 10^{6}$
5	$6 {{}^{2}S}_{1 / 2} \to 5 {{}^{2}P}_{3 / 2}$	1366.863	$1.29 \times 10^{7}$
6	$4 {{}^{2}D}_{3 / 2} \to 5 {{}^{2}P}_{1 / 2}$	1475.631	$1.07 \times 10^{7}$
7	$4 {{}^{2}D}_{3 / 2} \to 5 {{}^{2}P}_{3 / 2}$	1529.248	$2.0 \times 10^{6}$
8	$6 {{}^{2}P}_{1 / 2} \to 4 {{}^{2}D}_{3 / 2}$	2293.853	$2.4 \times 10^{6}$
9	$6 {{}^{2}P}_{1 / 2} \to 6 {{}^{2}S}_{1 / 2}$	2791.274	$4.3 \times 10^{6}$

State	$5 {{}^{2}S}_{1 / 2}$	$5 {{}^{2}P}_{1 / 2}$	$5 {{}^{2}P}_{3 / 2}$	$4 {{}^{2}D}_{3 / 2}$	$6 {{}^{2}S}_{1 / 2}$	$6 {{}^{2}P}_{1 / 2}$
Population probability	40.5%	3.6%	3.1%	7.1%	8.2%	37.3%

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Optics Letters