DocumentCode
1089230
Title
Performances of a frequency offset locked He-Xe laser system at 3.51 µm
Author
Ohtsu, Motoichi ; Katsuragi, Seiichi ; Tako, Toshiharu
Author_Institution
Tokyo Inst. of Tech., Yokohama, Japan
Volume
17
Issue
6
fYear
1981
fDate
6/1/1981 12:00:00 AM
Firstpage
1100
Lastpage
1107
Abstract
A highly stabilized frequency offset locked He-Xe laser system was constructed for high resolution laser spectroscopy of H2 CO [
] at 3.51μm. It is composed of three He-Xe lasers. The first laser is H2 CO-stabilized and is used as a frequency reference in the system. The second laser is frequency offset locked to the first laser by using the beat frequency between these lasers, and is used as a local oscillator. The third laser is frequency offset locked to the second laser, and is used to observe the H2 CO spectrum by slowly varying the beat frequency between these lasers. The frequency stability of the first laser, measured against a similarly stabilized and synchronously modulated laser, was
at
s, where τ represents the integration time. The frequency traceability of the second laser to the first laser was expressed as
for 10 ms
s. It was found that this value of the traceability was independent of the frequency modulation of the first and second lasers. The frequency traceability of the third laser to the second laser was nearly equal to that of the second laser described previously. The variable range of the frequency of the third laser was 19 MHz. In this range, the frequency traceability of the third laser to the second laser was independent of the beat frequency between these two lasers. From these results, it was concluded that this system can be used for the observation of the H2 CO spectrum.
] at 3.51μm. It is composed of three He-Xe lasers. The first laser is H
at
s, where τ represents the integration time. The frequency traceability of the second laser to the first laser was expressed as
for 10 ms
s. It was found that this value of the traceability was independent of the frequency modulation of the first and second lasers. The frequency traceability of the third laser to the second laser was nearly equal to that of the second laser described previously. The variable range of the frequency of the third laser was 19 MHz. In this range, the frequency traceability of the third laser to the second laser was independent of the beat frequency between these two lasers. From these results, it was concluded that this system can be used for the observation of the HKeywords
Infrared spectroscopy; Laser stability; Noble-gas lasers; Frequency measurement; Frequency modulation; Laboratories; Laser stability; Light sources; Local oscillators; Machinery; PROM; Spectroscopy; Time measurement;
fLanguage
English
Journal_Title
Quantum Electronics, IEEE Journal of
Publisher
ieee
ISSN
0018-9197
Type
jour
DOI
10.1109/JQE.1981.1071199
Filename
1071199
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