1999
DOI: 10.1070/qe1999v029n01abeh001408
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Diffractive focusing of an input pulse and giant energy gain in a laser based on an auto-wave photon-branched network

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Cited by 5 publications
(12 citation statements)
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“…The optimal laser variant was found [2][3][4][5] to have a four-pass unstable telescopic cavity of length L = 49.5 cm, when the diameters of the mirrors are d 1 = 14 cm for the first one and d 2 = 5.98 cm for the second one, and the focal length of the second mirror is F = 53 cm. In our calculations we assumed that the cavity is filled with a high-energy-capacity working mixture, with composition H 2 :F 2 :O 2 :He = 166:334:40:210 torr, containing fine passivated aluminum particles of radius r 0 = 0.2 µm and concentration N 0 = 1.3×10 8 cm 3 .…”
Section: Diffractive Pumping Of a Pulsed H 2 -F 2 Laser Based On An Amentioning
confidence: 99%
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“…The optimal laser variant was found [2][3][4][5] to have a four-pass unstable telescopic cavity of length L = 49.5 cm, when the diameters of the mirrors are d 1 = 14 cm for the first one and d 2 = 5.98 cm for the second one, and the focal length of the second mirror is F = 53 cm. In our calculations we assumed that the cavity is filled with a high-energy-capacity working mixture, with composition H 2 :F 2 :O 2 :He = 166:334:40:210 torr, containing fine passivated aluminum particles of radius r 0 = 0.2 µm and concentration N 0 = 1.3×10 8 cm 3 .…”
Section: Diffractive Pumping Of a Pulsed H 2 -F 2 Laser Based On An Amentioning
confidence: 99%
“…[1][2][3][4][5] The mutual transformation of plane and spherical waves in the cavity, and the presence of an input control signal in the region of the coupling aperture, are taken into account by the boundary conditions (5) on the mirrors. The result is a closed system of equations, (1)-(6), describing the electrodynamics and laser-chemical processes in the active medium of a pulsed H 2 -F 2 laser-amplifier based on a PBCR in an unstable telescopic cavity.…”
Section: Diffractive Focusing Of An Input Signalmentioning
confidence: 99%
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