Abstract:Output power dependences of composite Nd 3+ :YVO 4 Raman laser stationary generation on the longitudinal diode pump power are measured at different transmissions of the output mirror at the Stokes radiation frequency. The deviation of the measured dependences from linear is explained by the influence of thermal effects on both the overlap of the beams and diffraction losses. A method to estimate the laser and Stokes losses in the cavity and the parameters characterizing the overlap of the laser radiation with … Show more
“…For example, for pump power level of 17 W the optimal transmission T s is 1.1%, which is close to the one for a qCW 1.2 µm CWSSRL at the diode pump power level of the same order [30]. With an output coupler with this transmission the laser under consideration should provide 117 mW of Stokes output power at the diode pump power level of 17 W which corresponds to efficiency of 0.7% with respect to the diode pump power.…”
Section: Modelling and Discussionsupporting
confidence: 60%
“…To simplify calculations we used fixed values of the beam sizes (P abs = 3.4 W); thus the slope of the theoretical curve is fixed. (Variation of the beams overlap with the pump power in the model used is given in paper [30]). Nevertheless, even with constant beam sizes the results provided by the model are in good agreement with the experimental data.…”
We demonstrate the first quasi-CW (ms-long pulses, pump duty cycle of 10%) end-diode pumped solid state laser generating eye-safe radiation via intracavity Raman conversion. The output power at the first Stokes wavelength (1524 nm) was 250 mW. A theoretical model was applied to analyze the laser system and provide routes for optimization. The possibility of true CW operation was discussed.
“…For example, for pump power level of 17 W the optimal transmission T s is 1.1%, which is close to the one for a qCW 1.2 µm CWSSRL at the diode pump power level of the same order [30]. With an output coupler with this transmission the laser under consideration should provide 117 mW of Stokes output power at the diode pump power level of 17 W which corresponds to efficiency of 0.7% with respect to the diode pump power.…”
Section: Modelling and Discussionsupporting
confidence: 60%
“…To simplify calculations we used fixed values of the beam sizes (P abs = 3.4 W); thus the slope of the theoretical curve is fixed. (Variation of the beams overlap with the pump power in the model used is given in paper [30]). Nevertheless, even with constant beam sizes the results provided by the model are in good agreement with the experimental data.…”
We demonstrate the first quasi-CW (ms-long pulses, pump duty cycle of 10%) end-diode pumped solid state laser generating eye-safe radiation via intracavity Raman conversion. The output power at the first Stokes wavelength (1524 nm) was 250 mW. A theoretical model was applied to analyze the laser system and provide routes for optimization. The possibility of true CW operation was discussed.
“…As it follows from [18], stationary SFG of the frequency ν SL = ν S + ν L in the laser shown schematically in Fig. 1…”
Section: Sum Frequency Generationmentioning
confidence: 91%
“…The coefficients G, K SL , and b/a are defined by properties of the respective media and overlap integrals of the interacting beams. As shown in [18][19][20], the relations for G and K LS are…”
Section: Is Described By Equationsmentioning
confidence: 97%
“…The ratio b/a has the meaning of the efficiency of the conversion of the diode pump radiation to the fundamental radiation. According to [18][19][20], it can be expressed as…”
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