Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physica B+C

Third-order nonlinear spectra of a strong bichromatic field interacting with a three-level atom in a “V” configuration. II numerical results

D.A. Hutchinson, K.J. Woloschuk, Constantine Mavroyannis

Published Feb 1, 1984• 1 citation
Publisher
DOI
10.1016/0378-4363(84)90108-6

Related papers

Third-order nonlinear spectra of a strong bichromatic field interacting with a three-level atom in a “V” configuration. I

D.A. Hutchinson, K.J. Woloschuk, Constantine Mavroyannis

Physica B+C•Oct 1, 1983•1 citation

Third-order optical mixing of frequencies of a strong bichromatic field interacting with a three-level atom in the “Lambda” configuration

Constantine Mavroyannis

Optics Communications•Jul 1, 1983•4 citations

Two-photon interference spectra at the sum-frequency generation of a bichromatic field interacting with a three-level atom

Constantine Mavroyannis

Applied Physics B•Jul 1, 2003•0 citations

Interference spectra induced by a bichromatic field in the excited state of a three-level atom

Constantine Mavroyannis

Journal of Quantitative Spectroscopy and Radiative Transfer•Jun 1, 1998•0 citations

Sum third order frequency mixing of a strong bichromatic field interacting with a three-level atom

K.J. Woloschuk, S. Hontzeas, D.A. Hutchinson +1 more

We have considered the excitation spectra of three-photon processes arising from the interaction of a three-level atom, in the cascade configuration, with two strong electromagnetic fields whose initially populated modes ω a and ω b are near resonance with the atomic transition frequencies ω21 and ω32, respectively. In the limit of high photon densities, expressions for the Green's functions are derived in a closed form describing third order nonlinear processes in the region of frequencies ω = ω a + 2ω b and ω = ω b + 2ω a , respectively. Numerical calculations are then performed and the computed spectra are presented graphically for different values of the Rabi frequencies Ω a and Ω b , and detunings ζ a and ζ b , respectively. The excitation spectrum near ω = ω a + 2ω b is calculated as a function of the parameters η a = Ω a /γ0, η b = Ω b /γ0, ζ a = (ω21 - ω a )/γ0 and ζ b = (ω32 - ω b )/γ0 where γ0 is the spontaneous transition probability. With no detuning the spectral intensities vary slowly with respect to variations of the Rabi frequencies and are shifted by amounts governed by the field strengths η a and η b . In the presence of detunings, asymmetries, characteristics of such off-resonance situations, arise enhancing certain spectral peaks while diminishing the intensity of others.

Molecular Physics•Oct 10, 1983•2 citations

Nonlinear resonances in polarization spectrum of three-level atom, interacting with weak polychromatic fields

Вера Ивановна Яковлева, I.K. Korshok, A. G. Antipov +4 more

•Jan 1, 2018•0 citations
We have considered the excitation spectra of three-photon processes arising from the interaction of a three-level atom, in the cascade configuration, with two strong electromagnetic fields whose initially populated modes ω a and ω b are near resonance with the atomic transition frequencies ω21 and ω32, respectively. In the limit of high photon densities, expressions for the Green's functions are derived in a closed form describing third order nonlinear processes in the region of frequencies ω = ω a + 2ω b and ω = ω b + 2ω a , respectively. Numerical calculations are then performed and the computed spectra are presented graphically for different values of the Rabi frequencies Ω a and Ω b , and detunings ζ a and ζ b , respectively. The excitation spectrum near ω = ω a + 2ω b is calculated as a function of the parameters η a = Ω a /γ0, η b = Ω b /γ0, ζ a = (ω21 - ω a )/γ0 and ζ b = (ω32 - ω b )/γ0 where γ0 is the spontaneous transition probability. With no detuning the spectral intensities vary slowly with respect to variations of the Rabi frequencies and are shifted by amounts governed by the field strengths η a and η b . In the presence of detunings, asymmetries, characteristics of such off-resonance situations, arise enhancing certain spectral peaks while diminishing the intensity of others.