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

Optics Communications

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

Constantine Mavroyannis

Published Jul 1, 1983• 4 citations
Publisher
DOI
10.1016/0030-4018(83)90013-5

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 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

Physica B+C•Feb 1, 1984•1 citation

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

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

Stimulated emission at the sum-frequency generation of a bichromatic field interacting with a three-level atom

Constantine Mavroyannis

Zeitschrift für Physik D Atoms Molecules and Clusters•Dec 1, 1996•2 citations

Stimulated emission at the difference-frequency generation of a bichromatic field interacting with a three-level atom

Constantine Mavroyannis

The author considers the stimulated emission process that occurs at the difference-frequency generation of a bichromatic field interacting with a three-level atom in the Lambda configuration. In the low-intensity limit of both laser fields and at finite detunings, there are two induced excitations whose lifetimes are much longer in comparison to those of excitations spontaneously emitted by the excited states of the atom. Conditions are established under which the two-photon stimulated emission prevails, indicating that significant amplification is likely to occur at the difference-frequency generation.

Quantum Optics Journal of the European Optical Society Part B•Jun 1, 1993•4 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.
The author considers the stimulated emission process that occurs at the difference-frequency generation of a bichromatic field interacting with a three-level atom in the Lambda configuration. In the low-intensity limit of both laser fields and at finite detunings, there are two induced excitations whose lifetimes are much longer in comparison to those of excitations spontaneously emitted by the excited states of the atom. Conditions are established under which the two-photon stimulated emission prevails, indicating that significant amplification is likely to occur at the difference-frequency generation.