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 inJournal of modern optics Vol. 53; no. 11; pp. 1663 - 1673
Main Authors Sun, Qingqing, Gu, Ying, Gong, Qihuang
Format Journal Article
LanguageEnglish
Published London Taylor & Francis Group 20.07.2006
Taylor & Francis
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ISSN0950-0340
1362-3044
DOI10.1080/09500340600590083

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Abstract 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.
AbstractList Four-wave mixing (FWM) in a cycling transition Fg=1 Fe=0 is investigated. Subject to a linearly polarized pump field with frequency omegac and a magnetic field, and simultaneously saturated and probed by the circularly polarized fields (sigma+/-) with frequencies omegas and omegap, three kinds of FWM fields with frequencies: 2omegas - omegap, omegac+omegas - omegap and omegac - omegas+omegap, 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 omegac + omegas - omegap and omegac - omegas+omegap have about the same intensity for the well matching among the Zeeman splitting, drive Rabi frequency and saturation Rabi frequency.
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.
Author Gu, Ying
Gong, Qihuang
Sun, Qingqing
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  organization: State Key Laboratory for Mesoscopic Physics , Department of Physics , Peking University
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Keywords Dressed states
Zeeman effect
Four-wave mixing
Quantum optics
Linear polarization
Rabi splitting
Quantum yield
Nonlinear optics
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Snippet 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...
Four-wave mixing (FWM) in a cycling transition Fg=1 Fe=0 is investigated. Subject to a linearly polarized pump field with frequency omegac and a magnetic...
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SubjectTerms Exact sciences and technology
Fundamental areas of phenomenology (including applications)
Nonlinear optics
Optics
Phase conjugation, optical mixing; photorefractive and kerr effects
Physics
Title Resonant emission in four-wave mixing for a cycling transition Fg  = 1 ↔ Fe  = 0
URI https://www.tandfonline.com/doi/abs/10.1080/09500340600590083
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Volume 53
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