Resonant emission in four-wave mixing for a cycling transition Fg = 1 ↔ Fe = 0
Four-wave mixing (FWM) in a cycling transition F g =1 ↔ F e =0 is investigated. Subject to a linearly polarized pump field with frequency ω c and a magnetic field, and simultaneously saturated and probed by the circularly polarized fields (σ ± ) with frequencies ω s and ω p , three kinds of FWM fiel...
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Published in | Journal of modern optics Vol. 53; no. 11; pp. 1663 - 1673 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
London
Taylor & Francis Group
20.07.2006
Taylor & Francis |
Subjects | |
Online Access | Get full text |
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Summary: | Four-wave mixing (FWM) in a cycling transition F
g
=1 ↔ F
e
=0 is investigated. Subject to a linearly polarized pump field with frequency ω
c
and a magnetic field, and simultaneously saturated and probed by the circularly polarized fields (σ
±
) with frequencies ω
s
and ω
p
, three kinds of FWM fields with frequencies: 2ω
s
− ω
p
, ω
c
+ω
s
− ω
p
and ω
c
− ω
s
+ω
p
, emit. The multi-peaked structure of FWM spectra is obtained and explained as the resonant emission between the 'virtual states' in the dressed picture. The generated FMW signals have high quantum efficiency for a wide range of drive Rabi frequency and saturation Rabi frequency. Finally, the emitted fields ω
c
+ ω
s
− ω
p
and ω
c
− ω
s
+ω
p
have about the same intensity for the well matching among the Zeeman splitting, drive Rabi frequency and saturation Rabi frequency. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0950-0340 1362-3044 |
DOI: | 10.1080/09500340600590083 |