A 650-J XeCl laser

Abstract

A 308-nm XeCl laser with an active volume of 200 L is described and the results of its tests are presented. The output energy of 660 J is obtained by pumping the Ar: Xe: HCl = 1520: 40: 2-Torr mixture. The FWHM laser pulse duration is ∼ 350 ns. The nonuniformity of the laser-radiation density distribution over the cross section of the output beam in the near-field zone is within 10%. An accelerator that forms a radially converging electron beam with an electron energy of up to 550 keV, a vacuum-diode current of up to 320 kA, a beam-current pulse duration of ∼ 1 μs, and a beam current of up to 250 kA is used to pump the system. Two linear transformers with a 98-kJ energy stored in the primary storage serve as high-voltage sources. To reduce the effect of the self-magnetic field on the beam formation, the vacuum diode is divided into six diodes magnetically insulated from each other.

Original language	English
Pages (from-to)	199-202
Number of pages	4
Journal	Quantum Electronics
Volume	34
Issue number	3
DOIs	https://doi.org/10.1070/QE2004v034n03ABEH002610
Publication status	Published - Mar 2004

Keywords

Electron-beam pump
XeCl laser

ASJC Scopus subject areas

Electrical and Electronic Engineering
Physics and Astronomy (miscellaneous)

Access to Document

10.1070/QE2004v034n03ABEH002610

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A 650-J XeCl laser. / Abdullin, E. N.; Grishin, D. M.; Gubanov, V. P.; Zorin, V. B.; Kim, A. A.; Koval'chuk, B. M.; Kumpyak, E. V.; Liu, J.; Morozov, A. V.; Skakun, V. S.; Stepchenko, A. S.; Tarasenko, V. F.; Tolkachev, V. S.; Tsoi, N. V.; Shchanin, P. M.

In: Quantum Electronics, Vol. 34, No. 3, 03.2004, p. 199-202.

Research output: Contribution to journal › Article › peer-review

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title = "A 650-J XeCl laser",

abstract = "A 308-nm XeCl laser with an active volume of 200 L is described and the results of its tests are presented. The output energy of 660 J is obtained by pumping the Ar: Xe: HCl = 1520: 40: 2-Torr mixture. The FWHM laser pulse duration is ∼ 350 ns. The nonuniformity of the laser-radiation density distribution over the cross section of the output beam in the near-field zone is within 10%. An accelerator that forms a radially converging electron beam with an electron energy of up to 550 keV, a vacuum-diode current of up to 320 kA, a beam-current pulse duration of ∼ 1 μs, and a beam current of up to 250 kA is used to pump the system. Two linear transformers with a 98-kJ energy stored in the primary storage serve as high-voltage sources. To reduce the effect of the self-magnetic field on the beam formation, the vacuum diode is divided into six diodes magnetically insulated from each other.",

keywords = "Electron-beam pump, XeCl laser",

author = "Abdullin, {E. N.} and Grishin, {D. M.} and Gubanov, {V. P.} and Zorin, {V. B.} and Kim, {A. A.} and Koval'chuk, {B. M.} and Kumpyak, {E. V.} and J. Liu and Morozov, {A. V.} and Skakun, {V. S.} and Stepchenko, {A. S.} and Tarasenko, {V. F.} and Tolkachev, {V. S.} and Tsoi, {N. V.} and Shchanin, {P. M.}",

year = "2004",

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doi = "10.1070/QE2004v034n03ABEH002610",

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AU - Abdullin, E. N.

AU - Grishin, D. M.

AU - Gubanov, V. P.

AU - Zorin, V. B.

AU - Kim, A. A.

AU - Koval'chuk, B. M.

AU - Kumpyak, E. V.

AU - Liu, J.

AU - Morozov, A. V.

AU - Skakun, V. S.

AU - Stepchenko, A. S.

AU - Tarasenko, V. F.

AU - Tolkachev, V. S.

AU - Tsoi, N. V.

AU - Shchanin, P. M.

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N2 - A 308-nm XeCl laser with an active volume of 200 L is described and the results of its tests are presented. The output energy of 660 J is obtained by pumping the Ar: Xe: HCl = 1520: 40: 2-Torr mixture. The FWHM laser pulse duration is ∼ 350 ns. The nonuniformity of the laser-radiation density distribution over the cross section of the output beam in the near-field zone is within 10%. An accelerator that forms a radially converging electron beam with an electron energy of up to 550 keV, a vacuum-diode current of up to 320 kA, a beam-current pulse duration of ∼ 1 μs, and a beam current of up to 250 kA is used to pump the system. Two linear transformers with a 98-kJ energy stored in the primary storage serve as high-voltage sources. To reduce the effect of the self-magnetic field on the beam formation, the vacuum diode is divided into six diodes magnetically insulated from each other.

AB - A 308-nm XeCl laser with an active volume of 200 L is described and the results of its tests are presented. The output energy of 660 J is obtained by pumping the Ar: Xe: HCl = 1520: 40: 2-Torr mixture. The FWHM laser pulse duration is ∼ 350 ns. The nonuniformity of the laser-radiation density distribution over the cross section of the output beam in the near-field zone is within 10%. An accelerator that forms a radially converging electron beam with an electron energy of up to 550 keV, a vacuum-diode current of up to 320 kA, a beam-current pulse duration of ∼ 1 μs, and a beam current of up to 250 kA is used to pump the system. Two linear transformers with a 98-kJ energy stored in the primary storage serve as high-voltage sources. To reduce the effect of the self-magnetic field on the beam formation, the vacuum diode is divided into six diodes magnetically insulated from each other.

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