DocumentCode
1067894
Title
Fluorescence and oscillation characteristics of LiNdP4 O12 lasers at 1.317 µm
Author
Saruwatari, Masatoshi ; Otsuka, Kenju ; Miyazawa, Shintaro ; Yamada, Tomoaki ; Kimura, Tatsuya
Author_Institution
Nippon Telegraph and Telephone Public Corporation, Tokyo, Japan
Volume
13
Issue
10
fYear
1977
fDate
10/1/1977 12:00:00 AM
Firstpage
836
Lastpage
842
Abstract
Spectroscopic data and laser oscillation characteristics of the 1.317 μ line in lithium neodymium tetraphosphate (LNP) are reported. A stimulated emission cross section of this transition was spectroscopically determined as
cm2, which corresponds to 1/4.5 of that at the 1.047-μm transition. Cross-section temperature dependence, laser cavity loss, threshold versus crystal length, and threshold temperature dependence were measured experimentally. Since resonant loss was negligible at the 1.317 μm line, room temperature threshold is lower than that at 1.047-μm in the case of long crystal, and threshold temperature dependence is weaker than that at 1.047 μm. A miniaturized LNP laser, using a graded index fiber as a focusing medium, is also shown. LED pump intensity required to obtain a constant output is compared for 1.047- and 1.317-μm wavelengths. The 1.317-μm line seems to be useful as miniaturized optical sources in optical communication systems, since required intensity is around several W/cm2for the side pump, and the wavelength corresponds to the most transparent band of ultra low-loss optical fibers.
cm2, which corresponds to 1/4.5 of that at the 1.047-μm transition. Cross-section temperature dependence, laser cavity loss, threshold versus crystal length, and threshold temperature dependence were measured experimentally. Since resonant loss was negligible at the 1.317 μm line, room temperature threshold is lower than that at 1.047-μm in the case of long crystal, and threshold temperature dependence is weaker than that at 1.047 μm. A miniaturized LNP laser, using a graded index fiber as a focusing medium, is also shown. LED pump intensity required to obtain a constant output is compared for 1.047- and 1.317-μm wavelengths. The 1.317-μm line seems to be useful as miniaturized optical sources in optical communication systems, since required intensity is around several W/cm2for the side pump, and the wavelength corresponds to the most transparent band of ultra low-loss optical fibers.Keywords
Fluorescence; Laser transitions; Length measurement; Lithium; Loss measurement; Neodymium; Optical fiber communication; Spectroscopy; Stimulated emission; Temperature dependence;
fLanguage
English
Journal_Title
Quantum Electronics, IEEE Journal of
Publisher
ieee
ISSN
0018-9197
Type
jour
DOI
10.1109/JQE.1977.1069228
Filename
1069228
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