High‐order stimulated Raman scattering combined with second harmonic generation in [χ (2) +χ (3) ]‐nonlinear LaBGeO 5 , β′‐Gd 2 (MoO 4 ) 3  and Ca 4 Gd(BO 3 ) 3 O laser host crystals under picosecond excitation | Zendy

Kaminskii A. A. | Zendy; Butashin A. V. | Zendy; Eichler H. J. | Zendy; Grebe D. | Zendy; Macdonald R. | Zendy; Findeisen J. | Zendy; Bagayev S. N. | Zendy; Pavlyuk A. A. | Zendy; Aka G. | Zendy; Vivien D. | Zendy; Pelenc D. | Zendy

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High‐order stimulated Raman scattering combined with second harmonic generation in [χ (2) +χ (3) ]‐nonlinear LaBGeO 5 , β′‐Gd 2 (MoO 4 ) 3 and Ca 4 Gd(BO 3 ) 3 O laser host crystals under picosecond excitation

Author(s) -

Kaminskii A. A.,

Butashin A. V.,

Eichler H. J.,

Grebe D.,

Macdonald R.,

Findeisen J.,

Bagayev S. N.,

Pavlyuk A. A.,

Aka G.,

Vivien D.,

Pelenc D.

Publication year - 1998

Publication title -

journal of raman spectroscopy

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.748

H-Index - 110

eISSN - 1097-4555

pISSN - 0377-0486

DOI - 10.1002/(sici)1097-4555(199807)29:7<645::aid-jrs273>3.0.co;2-s

Subject(s) - picosecond , raman scattering , raman spectroscopy , laser , excitation , second harmonic generation , nonlinear optics , chemistry , raman laser , wavelength , high harmonic generation , coherent anti stokes raman spectroscopy , nonlinear system , optics , materials science , optoelectronics , physics , quantum mechanics

New frequency conversion processes leading to emission in the visible spectral range were observed for the first time by multiple Stokes and anti‐Stokes Raman generation arising from intrinsic second harmonic generation in three different [χ (2) +χ (3) ]‐nonlinear LaBGeO 5 , β′‐Gd 2 (MoO 4 ) 3 and Ca 4 Gd(BO 3 ) 3 O laser host crystals under picosecond pumping at a fundamental wavelength of 1 μm. © 1998 John Wiley & Sons, Ltd.

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