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In order to match the beams size a telescope in optics scheme was used. The following parameters of the active medium were adopted as the initial data: Second, there are no principal restrictions on the increase of the cross size of their active medium. In the case of the main amplifier, excited by a lower pump power, the following parameters of the active medium were adopted: These laser systems have high apertures of tens centimetres and a radiation energy from J to 1 kJ. After connecting the storage capacitor to the discharge gap, a x-ray source is switched on for this purpose ns before the attainment of the maximum voltage on the electrode and its radiation initiates the onset of the discharge. Lobachev, Baltic State Technical Univ. According to the calculations, for input radiation with an energy of 30 mJ filling completely the preamplifier aperture, the output energy amounts to 3. Since in our laser system the rectangular 5 cm x 10 cm preamplifier aperture had to be matched to the square aperture of the main amplifier in the system, it was necessary to estimate the energy losses incurred on amplification of a beam with a square cross section in the preamplifier. I Since a time-dependent model was used in the calculations, we were able to follow the useful radiation and ASE profiles. Topics include generation of ultrashort light pulses, application of nonlinear correction techniques in adaptive optics and lasers, advanced methods of beam control and pointing; diode-pumped solid state lasers; high average power gas and solidstate lasers; and lasers in medicine and medical applications. The high voltage pulse generator was used to switch and synchronize of an master oscillator with the amplifiers.

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In order to match the beams size a telescope in optics scheme was used. The following parameters of the active medium were adopted as the initial data: Second, there are no principal restrictions on the increase of the cross size of their active medium. In the case of the main amplifier, excited by a lower pump power, the following parameters of the active medium were adopted: These laser systems have high apertures of tens centimetres and a radiation energy from J to 1 kJ. After connecting the storage capacitor to the discharge gap, a x-ray source is switched on for this purpose ns before the attainment of the maximum voltage on the electrode and its radiation initiates the onset of the discharge. Lobachev, Baltic State Technical Univ. According to the calculations, for input radiation with an energy of 30 mJ filling completely the preamplifier aperture, the output energy amounts to 3. Since in our laser system the rectangular 5 cm x 10 cm preamplifier aperture had to be matched to the square aperture of the main amplifier in the system, it was necessary to estimate the energy losses incurred on amplification of a beam with a square cross section in the preamplifier. I Since a time-dependent model was used in the calculations, we were able to follow the useful radiation and ASE profiles. Topics include generation of ultrashort light pulses, application of nonlinear correction techniques in adaptive optics and lasers, advanced methods of beam control and pointing; diode-pumped solid state lasers; high average power gas and solidstate lasers; and lasers in medicine and medical applications. The high voltage pulse generator was used to switch and synchronize of an master oscillator with the amplifiers.




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    The results of the calculations and the duration of the input signal pulse permit us to conclude that an input energy of the order of 10 mJ should be sufficient to saturate this amplifier after two passes. Papers were selected by the conference program committee to be presented in oral or poster format, and were subject to review by volume editors or program committees.

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