LD end pumped mode locked and cavity dumped Nd:YAP laser at 1.34μm

Wang, X.; Wang, S.; Rhee, H.; Eichler, Hans Joachim; Meister, Stefan

doi:10.1016/j.optcom.2011.02.011

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“…The output wavelength of a Raman laser depends on Raman spectrum of the Raman crystal and the wavelength of the fundamental laser. The commonly known Raman crystals include Ba(NO 3 ) 2 [9,10], YVO 4 [11,12], GdVO 4 [13], diamond [14,15], and variety of tungstate crystals [16][17][18][19][20][21][22].…”

Section: Introductionmentioning

confidence: 99%

Diode-pumped actively Q-switched Tm:YAP/BaWO_4 intracavity Raman laser

et al. 2015

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We report an intracavity Raman laser based on BaWO(4) Raman conversion in a diode-pumped actively Q-switched Tm:YAP laser for the first time. With an incident diode power of 17.5 W and a pulse repetition rate of 1 kHz, the maximum average output powers of 880 mW and 306 mW for the fundamental laser at 1.94 μm and the first Stokes laser at 2.36 μm were obtained, respectively. The pulse width and pulse energy of the first Stokes laser were 14.1 ns and 0.31 mJ, respectively. The Raman gain coefficient of the BaWO(4) crystal was estimated to be 1.1 cm/GW at 1.94 μm.

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