Multiwavelength, picosecond, synchronously pumped, Pb(MoO4)0.2(WO4)0.8 Raman laser oscillating at 12 wavelengths in a range of 1128–1360 nm

Milan Frank; Sergei N. Smetanin; Michal Jelínek; David Vyhlídal; Ksenia A. Gubina; Vladislav E. Shukshin; Petr G. Zverev; Václav Kubeček

doi:10.1364/OL.441592

Optics Letters
Vol. 46,
Issue 20,
pp. 5272-5275
(2021)
•https://doi.org/10.1364/OL.441592

Multiwavelength, picosecond, synchronously pumped, Pb(MoO₄)_0.2(WO₄)_0.8 Raman laser oscillating at 12 wavelengths in a range of 1128–1360 nm

Milan Frank, Sergei N. Smetanin, Michal Jelínek, David Vyhlídal, Ksenia A. Gubina, Vladislav E. Shukshin, Petr G. Zverev, and Václav Kubeček

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Milan Frank, Sergei N. Smetanin, Michal Jelínek, David Vyhlídal, Ksenia A. Gubina, Vladislav E. Shukshin, Petr G. Zverev, and Václav Kubeček, "Multiwavelength, picosecond, synchronously pumped, Pb(MoO₄)_0.2(WO₄)_0.8 Raman laser oscillating at 12 wavelengths in a range of 1128–1360 nm," Opt. Lett. 46, 5272-5275 (2021)

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- Nonlinear Optics
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About this Article
History
- Original Manuscript: August 26, 2021
- Revised Manuscript: September 23, 2021
- Manuscript Accepted: September 29, 2021
- Published: October 15, 2021

Abstract

In this Letter, a mixed ${\rm Pb}{({{\rm MoO}_4})_{0.2}}{({{\rm WO}_4})_{0.8}}$ as a new, to the best of our knowledge, active medium with optimized content for a synchronously pumped multiwavelength Raman laser with a combined frequency shift is presented. The unique structure of this crystal resulted in oscillations at 12 closely spaced output wavelengths in a spectral range from 1128 to 1360 nm. The strongest pulse shortening in comparison with nominally pure scheelite-like crystals has been achieved.

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Data underlying the results presented in this paper are not publicly available at this time but may be obtained from the authors upon reasonable request.

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	1063 nm	1128/1132 nm	1171/1176 nm	1217/1222 nm	1250 nm	1266/1272 nm	1303/1316 nm	1360 nm
PM	1.3	72.3/80.8	98.7/98.9	99.4/99.4	99.1	98.4/98.0	85.4/53.8	79.0
CM	1.6	99.5/99.6	99.6/99.6	99.6/99.6	99.7	99.6/99.6	99.0/98.7	87.2
FM	99.8	99.9/99.9	99.8/99.8	99.8/99.8	99.8	99.6/99.5	95.6/87.8	61.2
OC	99.8	99.7/99.7	99.5/99.4	89.8/83.5	33.8	50.7/53.4	17.5/28.5	16.7

$λ_{G}$ [nm]	1171/1176	1128/1132	1217/1222	1303/1316	1266/1272 nm	1250	1360
$λ_{F}$ [nm]	1063	1171/1176	1171/1176	1171/1176	1217/1222	1303	1303
Raman Shift	$ν_{1 M} / ν_{1 W}$	$- ν_{2}$	$ν_{2}$	$ν_{1 M} / ν_{1 W}$	$ν_{2}$	$- ν_{2}$	$ν_{2}$

	1063 nm	1128/1132 nm	1171/1176 nm	1217/1222 nm	1250 nm	1266/1272 nm	1303/1316 nm	1360 nm
PM	1.3	72.3/80.8	98.7/98.9	99.4/99.4	99.1	98.4/98.0	85.4/53.8	79.0
CM	1.6	99.5/99.6	99.6/99.6	99.6/99.6	99.7	99.6/99.6	99.0/98.7	87.2
FM	99.8	99.9/99.9	99.8/99.8	99.8/99.8	99.8	99.6/99.5	95.6/87.8	61.2
OC	99.8	99.7/99.7	99.5/99.4	89.8/83.5	33.8	50.7/53.4	17.5/28.5	16.7

$λ_{G}$ [nm]	1171/1176	1128/1132	1217/1222	1303/1316	1266/1272 nm	1250	1360
$λ_{F}$ [nm]	1063	1171/1176	1171/1176	1171/1176	1217/1222	1303	1303
Raman Shift	$ν_{1 M} / ν_{1 W}$	$- ν_{2}$	$ν_{2}$	$ν_{1 M} / ν_{1 W}$	$ν_{2}$	$- ν_{2}$	$ν_{2}$

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