Stimulated Raman scattering and four-wave mixing from a mixture of carbon disulfide and phenylethanol in a hollow optical fiber

Yiqing Chen; Lei Wang; Xuebiao Lu; Yangqing Chen; Mingxing Qiu

doi:10.1364/OL.16.001469

Optics Letters
Vol. 16,
Issue 19,
pp. 1469-1471
(1991)
•https://doi.org/10.1364/OL.16.001469

Stimulated Raman scattering and four-wave mixing from a mixture of carbon disulfide and phenylethanol in a hollow optical fiber

Yiqing Chen, Lei Wang, Xuebiao Lu, Yangqing Chen, and Mingxing Qiu

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Yiqing Chen, Lei Wang, Xuebiao Lu, Yangqing Chen, and Mingxing Qiu, "Stimulated Raman scattering and four-wave mixing from a mixture of carbon disulfide and phenylethanol in a hollow optical fiber," Opt. Lett. 16, 1469-1471 (1991)

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Abstract

We observe, for what is to our knowledge the first time, stimulated Raman scattering and four-wave mixing in a liquid-core optical fiber filled with a mixture of carbon disulfide and phenylethanol pumped by the frequency-doubled output of a Q-switched YAG laser (λ = 532.1 nm). The frequencies of the stimulated Raman scattering and four-wave mixing spectra are specified, and theoretical interpretations are also given.

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No.	Frequency (cm⁻¹)	Frequency Shift Relative to the Pump Light (cm⁻¹)	Nonlinear Process^a	Relative Intensity
1	15,708	−3085	ω_S3^PE = ω_S2^PE − Δω_PE (S)	W
2	16,133	−2660	ω_F = ω₀ + ω_S2^PE − ω_ai^CS₂ (FWM)	VW
3	16,152	−2641	ω_s4^CS₂ = ω_S3^CS₂ − Δω_CS₂ (S)	W
4	16,784	−2009	ω_S2^PE = ω_si^PE − Δω_PE (S)	M
5	16,818	−1975	ω_S3^CS₂ = ω_S2^CS₂ − Δω_CS₂ (S)	S
6	17,127	−1666	ω_F = ω_si^CS₂ + ω_si^PE − ω₀ (FWM)	M
7	17,482	−1311	ω_s2^CS₂ = ω_si^CS₂ − Δω_CS₂ (S)	S
8	17,787	−1006	ω_si^PE = ω₀ − Δω_PE (S)	VS
9	18,137	−656	ω_si^CS₂ = ω₀− Δω_CS₂ (S)	VS
10	18,793	0	Frequency of the pump light	VS
11	19,132	339	ω_F = ω₀ + ω_si^CS₂ − ω_si^PE (FWM)	W
12	19,447	654	ω_ai^CS₂ = 2ω₀ − ω_si^CS₂ (AS)	M
13	19,787	994	ω_ai^PE = 2ω₀ − ω_si^PE (AS)	M
14	20,094	1301	ω_a2^CS₂ = 2ω₀ − ω_S2^CS₂ (AS)	M
15	20,110	1317	ω_F = ω₀ − ω_S2^PE + ω_si^CS₂ (FWM)	VW
16	20,442	1649	$ω_{F} = {\begin{cases} ω_{0} + {ω_{ai}}^{{CS}_{2}} - {ω_{si}}^{PE} \\ ω_{0} + {ω_{ai}}^{PE} - {ω_{si}}^{{CS}_{2}} \end{cases} (FWM)$	VW
17	20,983	2190	${\begin{cases} {ω_{a 2}}^{PE} = 2 ω_{0} - {ω_{s 2}}^{PE} (AS) \\ {ω_{a 3}}^{{CS}_{2}} = 2 ω_{0} - {ω_{s 3}}^{{CS}_{2}} (AS) \end{cases}$	W
18	21,434	2641	ω_a4^CS₂ = 2ω₀ − ω_S4^CS₂ (AS)	VW
19	21,463	2670	ω_F = ω₀− ω_s2^PE + ω_ai^CS₂ (FWM)	VW

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