1993
DOI: 10.1070/qe1993v023n07abeh003124
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High-power compact laser with λ =308 and 249 nm pumped by a radially converging electron beam

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Cited by 10 publications
(3 citation statements)
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“…[6][7][8][9] 4). Since all calculation methods of the rate constants of electron mixing have a great error (up to 100 % and above) and the buffer mixing of Xe(5d) states constant information is absent the main stage of simulation consisted in variation of rate constants in region of errors of their calculation according to best agreement with experimental data.…”
Section: Description Of the Kinetic Modelmentioning
confidence: 99%
“…[6][7][8][9] 4). Since all calculation methods of the rate constants of electron mixing have a great error (up to 100 % and above) and the buffer mixing of Xe(5d) states constant information is absent the main stage of simulation consisted in variation of rate constants in region of errors of their calculation according to best agreement with experimental data.…”
Section: Description Of the Kinetic Modelmentioning
confidence: 99%
“…Russian institutions also develop and create the powerful excimer lasers and laser systems [4][5][6][7][8][9][10][11][12]. In particular, a KrF laser system with a Garpun output unit (Institute of Physics, Russian Academy of Sciences) has an output aperture with a size of 16 × 18 cm and one generates radiation pulses with energy of 80 J and pulse duration of 100 ns [12].…”
Section: Introductionmentioning
confidence: 99%
“…The excimer lasers developed at the High-Current Electronics Institute (HCEI), Siberian Division, Russian Academy of Sciences, generate pulses with an energy of greater than 100 J [4][5][6][8][9][10][11]. The two most powerful XeCl lasers (308 nm) with apertures of 40 [8] and 60 cm [9][10][11] generate pulses with energies of 660 J and 1.9 kJ and pulse durations of about 350 and 250 ns, respectively.…”
Section: Introductionmentioning
confidence: 99%