DocumentCode
1103817
Title
Sequence-frequency three-wave mixing emissions in a birefringent optical fiber
Author
Kitayama, Ken-ichi ; Ohashi, Masaharu ; Gustafson, T. Kenneth
Author_Institution
NTT Public Corporation, Japan
Volume
21
Issue
10
fYear
1985
fDate
10/1/1985 12:00:00 AM
Firstpage
1689
Lastpage
1700
Abstract
Efficient parametric stimulated and parametric mixing processes involving waves with many optical frequencies can occur in a highly birefringent single-mode optical fiber due to the third-order nonlinear susceptibility
. Three types of multiple-order sequence-frequency emissions, two associated with the LP01 mode, with fundamental frequency-shifts
of approximately 1500 cm-1and 150 cm-1, and one associated with the
mode, with
cm-1, have been observed. Emissions are seen to be due to both degenerate stimulated four-photon mixing, which provides simultaneous amplification proportional to the square of the pump intensity for Stokes and anti-Stokes generation from noise, and parametric three-wave mixing in which already generated Stokes and anti-Stokes fields are mixed with a strong pump field to produce the newly generated field. Both the 1500 cm-1and the 150 cm-1fundamental anti-Stokes shifts associated with the LP01 mode sequence-frequency emissions originate from the off-diagonal component of
. The value of the shifts are such as to have compensation of the bulk material phase mismatch Km of fused silica with the high birefringence of the mutually orthogonal
and
modes. On the other hand. the 1000 cm-1shift of the mixed-mode excitation of the LP01 and LP11 modes originates from the diagonal component of
, and has a value such that the phase mismatch due to the mode dispersion Kw cancels the material dispersion term Km . The observed polarization directions of the generated waves are in good agreement with theoretical predictions, supporting the identification of the relevant waves. This is the first report of three-wave mixing due to the off-diagonal component of
. Three-wave mixing due to the diagonal component has been seen previously, as has stimulated four-photon mixing due to both the diagonal and off-diagonal components.
. Three types of multiple-order sequence-frequency emissions, two associated with the LP
of approximately 1500 cm-1and 150 cm-1, and one associated with the
mode, with
cm-1, have been observed. Emissions are seen to be due to both degenerate stimulated four-photon mixing, which provides simultaneous amplification proportional to the square of the pump intensity for Stokes and anti-Stokes generation from noise, and parametric three-wave mixing in which already generated Stokes and anti-Stokes fields are mixed with a strong pump field to produce the newly generated field. Both the 1500 cm-1and the 150 cm-1fundamental anti-Stokes shifts associated with the LP
. The value of the shifts are such as to have compensation of the bulk material phase mismatch K
and
modes. On the other hand. the 1000 cm-1shift of the mixed-mode excitation of the LP
, and has a value such that the phase mismatch due to the mode dispersion K
. Three-wave mixing due to the diagonal component has been seen previously, as has stimulated four-photon mixing due to both the diagonal and off-diagonal components.Keywords
Optical fibers; Optical mixers; Birefringence; Fiber nonlinear optics; Frequency; Noise generators; Optical fibers; Optical mixing; Optical pumping; Polarization; Silicon compounds; Stimulated emission;
fLanguage
English
Journal_Title
Quantum Electronics, IEEE Journal of
Publisher
ieee
ISSN
0018-9197
Type
jour
DOI
10.1109/JQE.1985.1072550
Filename
1072550
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