The measured data were sufficient to evaluate the performance of the gain module suggested as thermal effects and energy-storage features, with a simple measurement scheme in terms of practical aspects. We verified
The energy storage capacity of large-aperture Nd:LuAG is investigated and compared with that of Nd:YAG. Energy amplification up to 10.3 J at 10 Hz is achieved, which, to the best of our knowledge
calculation, excitation densities, upconversion rates, heat generation, temperature profiles, and thermal lensing are calculated. Differences in thermal lens power between nonlasing and
The diode-pumped Nd:YAG laser has opened up a wider range of applications, thanks to its increased source stability, efficiency and lifetime, and reduced power consumption and size. Commercial Nd:YAG lasers with repetition rates higher
where E i n is the injected energy fluence, E s t o is the energy storage per unit volume, and l is the path length of the laser in the gain medium. According to Eq. 3, it is known
Abstract: We have experimentally measured the energy stored and the heat generated in flashlamp-pumped Nd:YAG and six different commercially available Nd-doped phosphate
Frantz–Nodvik approach for the calculation of the saturated amplifica-tion of 100 ps pulses in Nd:YAG laser system was in a good agreement with experimental data if saturation fluence
Diode-pumped Nd:YAG lasers for generation of blue light by frequency doubling The influence of energy-transfer upconversion (ETU) is a detrimental effect in Nd- The results of the
We have experimentally measured the energy stored and the heat generated in flashlamp-pumped Nd:YAG and six different commercially available Nd-doped phosphate glasses. We
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