DocumentCode
1092653
Title
Multijoule performance of the photolytically pumped XeF(C→A) laser
Author
Eckstrom, Donald J. ; Walker, Homer C., Jr.
Author_Institution
Molecular Physics Lab., SRI International, Menlo Park, CA, USA
Volume
18
Issue
2
fYear
1982
fDate
2/1/1982 12:00:00 AM
Firstpage
176
Lastpage
181
Abstract
An XeF(
) laser with output up to 5.8 J/pulse has been demonstrated. The photolytic pumping scheme begins with
-beam excitation of xenon to produce Xe*2 fluorescence at 172 nm. This VUV radiation is transmitted through an array of CaF2 windows into the laser cell, where it photodissociates XeF2 to produce primarily XeF(
). Collisions with N2 buffer gas relax the excited states to XeF(
), which lases on a transition centered at 481 nm and continuously tunable over more than ±35 nm. Typical values of the experimental parameters were as follows. The 420 kV, 1 m
-beam source delivered an average current of 10 A/cm2over an aperture 14 × 100 cm for pulse lengths up to 1 μs. Total
-beam energy available was 3.5 kJ, of which 2.4 kJ was deposited in the xenon. The total VUV energy radiated was 720 J, of which 115 J was coupled into the laser cell. This produced 32 J of available XeF* energy, of which up to 18 percent was extracted as laser energy. The total system efficiency was 0.2 percent. Optimized designs should achieve better than 1 percent efficiency.
) laser with output up to 5.8 J/pulse has been demonstrated. The photolytic pumping scheme begins with
-beam excitation of xenon to produce Xe*
). Collisions with N
), which lases on a transition centered at 481 nm and continuously tunable over more than ±35 nm. Typical values of the experimental parameters were as follows. The 420 kV, 1 m
-beam source delivered an average current of 10 A/cm2over an aperture 14 × 100 cm for pulse lengths up to 1 μs. Total
-beam energy available was 3.5 kJ, of which 2.4 kJ was deposited in the xenon. The total VUV energy radiated was 720 J, of which 115 J was coupled into the laser cell. This produced 32 J of available XeF* energy, of which up to 18 percent was extracted as laser energy. The total system efficiency was 0.2 percent. Optimized designs should achieve better than 1 percent efficiency.Keywords
Laser tuning; Noble-gas lasers; Pulsed lasers; Visible lasers; Fluorescence; Gas lasers; Laser excitation; Laser transitions; Optical arrays; Optical pulses; Pulsed laser deposition; Pump lasers; Tunable circuits and devices; Xenon;
fLanguage
English
Journal_Title
Quantum Electronics, IEEE Journal of
Publisher
ieee
ISSN
0018-9197
Type
jour
DOI
10.1109/JQE.1982.1071517
Filename
1071517
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