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Advanced Solid-State Photonics, 2006
Raman laser was constructed on the base of new Nd:BaWO4 material Q-switched by LiF:F2- crystal. Emission at 1169 nm was obtained in 1.3 ns long pulse with energy 0.8 mJ.
J. Šulc +6 more
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Raman laser was constructed on the base of new Nd:BaWO4 material Q-switched by LiF:F2- crystal. Emission at 1169 nm was obtained in 1.3 ns long pulse with energy 0.8 mJ.
J. Šulc +6 more
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1981
For many years Raman spectroscopy has been a powerful tool for the investigation of molecular vibrations and rotations. In the pre-laser era, however, its main drawback was a lack of sufficiently intense radiation sources. The introduction of lasers, therefore, has indeed revolutionized this classical field of spectroscopy. Lasers have not only greatly
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For many years Raman spectroscopy has been a powerful tool for the investigation of molecular vibrations and rotations. In the pre-laser era, however, its main drawback was a lack of sufficiently intense radiation sources. The introduction of lasers, therefore, has indeed revolutionized this classical field of spectroscopy. Lasers have not only greatly
openaire +1 more source
2004
The use of stimulated Raman scattering (SRS) as a means of amplifying signals in telecommunication systems has been demonstrated since 1976 [1]. Yet despite its advantages over erbium-doped fiber, Raman amplification was not used in the first generation of deployed optically amplified systems.
C. Headley +2 more
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The use of stimulated Raman scattering (SRS) as a means of amplifying signals in telecommunication systems has been demonstrated since 1976 [1]. Yet despite its advantages over erbium-doped fiber, Raman amplification was not used in the first generation of deployed optically amplified systems.
C. Headley +2 more
openaire +1 more source