<i>Q</i>-switched chemical cw HF laser

Maksimov, Yurii P; Mashendzhinov, V. I.; Revich, V. E.; Rotinyan, Mikhail A; Sudarikov, V. V.; Tret'yakov, Nikolai E; Fedorov, I. A.; Eller, V. A.; Etsina, Alla L

doi:10.1070/qe2005v035n03abeh002834

Cited by 2 publications

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“…A new study is executed with the purpose of partial elimination of deficiencies of experiment 10 and of better understandings of nature of RPM with mechanical modulation of the resonator quality. Both the experimental study and the numerical simulation of RPM of the more powerful (average power Р ~ 8 kW) CW HF/DF-laser, in particular, the determination of the restoring time of the inverse population in active medium were performed.…”

Section: Introductionmentioning

confidence: 99%

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CW chemical HF/DF laser operating in the Q-switch mode

Azarov¹,

Alexandrov²,

Kuprenyuk

et al. 2006

XVI International Symposium on Gas Flow, Chemical Lasers, and High-Power Lasers

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The numerical end experimental study of the energy and temporal characteristics of the output radiation of the CW medium-scale chemical HF/DF-laser with mechanical modulation of the optical resonator quality by the mirror rotation with frequency up to 1 kHz is carried out. In experiment, a peak power of the laser radiation pulses has exceeded the radiation power in CW mode of the HF-laser operation not less than in four times. The average power in repetitively pulsed mode is lower than one in CW mode, but it grows with increase of the modulation frequency. Time of the complete recovery of a small signal gain of the active medium, which is about 6 -7 µs, is determined. Two numerical models are developed, which describe the dynamics of the laser oscillation in a mode of the resonator quality modulation for both HF-and DF-laser, some features of their operation are analyzed using these models.

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Section: Introductionmentioning

confidence: 99%

“…The experiment on the CW small-scale (average power Р ~ 1 kW) HF-laser was performed which results are given in Ref. 10 . The scheme of the experiment did not allow determining the time of the inverse population restoring in the active medium after a power pulse (in numerical simulation this time was accepted to be equal 4 µs).…”

Section: Introductionmentioning

confidence: 99%

CW chemical HF/DF laser operating in the Q-switch mode

Azarov¹,

Alexandrov²,

Kuprenyuk

et al. 2006

XVI International Symposium on Gas Flow, Chemical Lasers, and High-Power Lasers

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Computational and experimental study of aQ-switched cw chemical HF/DF laser

et al. 2007

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ReferencesBatlogg B 1990 Proc. Los Alamos Symp. on HTSC -1989 eds K S Bedell et a1 Gordon J E et a1 1989 Solid State Commun @ 625 and erratum Solid State Junod A et a1 1989 Physica c162 1401 Krakauer H et a1 1988 J. Superconductivity 1. 111 Loram J W and K A Mirza 1988 Physica C153-155 1020 Massidda A et a1 1987 Phys. Lett. A122 198 Padamsee H et a1 1973 J. Low Temp. Phys. 12 387 Phillips N E et a1 1990 Phys. Rev. Lett. 65 357 (Redwood City: Addison-Wesley) pp 37-93 Commun, to be published

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Q-switched chemical cw HF laser

Cited by 2 publications

References 0 publications

CW chemical HF/DF laser operating in the Q-switch mode

CW chemical HF/DF laser operating in the Q-switch mode

Computational and experimental study of aQ-switched cw chemical HF/DF laser

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