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 and Spectroscopy

Nonlinear waves in a dispersing medium with two-photon resonant transition

Guram T. Adamashvili

Published Mar 1, 1994• 0 citations
OpenAlex

Related papers

Nonlinear wave in a medium with a two-photon resonance transition

Guram T. Adamashvili

Physics Letters A•Apr 1, 1992•4 citations

Optical breather in a dispersive medium with a two-photon resonant transition

Guram T. Adamashvili

Optics and Spectroscopy•Jun 1, 1992•0 citations

Negative group velocities in quasi-phase-matched second-order nonlinear optical interactions

Stefano Longhi, P. Laporta, Marcello Marano

The existence of anomalous, i.e. superluminal or negative, group velocities [1] provides one of the most amazing phenomenon of wave propagation which is compatible with, and even a consequence of, causality [2]. Anomalous wave propagation generally relies on the resonant interaction of light with an atomic medium, i.e. it exploits the dispersive properties of absorptive [3] or inverted [4,5] atomic media near resonances. Evanescent wave propagation across photonic barriers [1] provides the other wide framework where anomalous group velocities have been observed, however in such cases the achievement of a negative group velocity seems unlikely. By exploiting the dispersive properties of a gain doublet, a narrow spectral region of transparent anomalous dispersion around the dip center of two Lorentzian gain lines, leading to negative transit times and no pulse attenuation, can be created [4]. A recent demonstration thereof has been indeed reported in an experiment by Wang and coworkers using Cs vapor [5].

Nonlinear Guided Waves and Their Applications•Jan 1, 2002•0 citations

Nonlinear polarizability of a two-isotope active medium in a ring laser in the presence of interisotope resonance photon exchange

A. Birman, A. F. Savushkin

The resonance radiation trapping operators are constructed for a two-isotope excited atom ensemble allowing for interisotope resonance photon exchange. The nonlinear polarizability of a ring-laser medium is calculated using the strong collision model and an expression is obtained which relates the exchange parameter with the isotope shift due to the resonance transition and with the trapping parameter. Relationships are derived and analyzed for the nonlinear self-interaction and interaction parameters of the opposite waves under complete exchange conditions by accurately solving a system of kinetic equations.

Soviet Journal of Quantum Electronics•May 31, 1979•0 citations

Periodic nonlinear waves in degenerate two-photon interaction in a two-level medium

Alexander A. Zabolotskii

Optics and Spectroscopy•Sep 1, 1996•0 citations

Propagation of waves in a two-photon absorbing medium

Jick H. Yee, H.H. Chau

Physics Letters A•Aug 1, 1970•1 citation
The existence of anomalous, i.e. superluminal or negative, group velocities [1] provides one of the most amazing phenomenon of wave propagation which is compatible with, and even a consequence of, causality [2]. Anomalous wave propagation generally relies on the resonant interaction of light with an atomic medium, i.e. it exploits the dispersive properties of absorptive [3] or inverted [4,5] atomic media near resonances. Evanescent wave propagation across photonic barriers [1] provides the other wide framework where anomalous group velocities have been observed, however in such cases the achievement of a negative group velocity seems unlikely. By exploiting the dispersive properties of a gain doublet, a narrow spectral region of transparent anomalous dispersion around the dip center of two Lorentzian gain lines, leading to negative transit times and no pulse attenuation, can be created [4]. A recent demonstration thereof has been indeed reported in an experiment by Wang and coworkers using Cs vapor [5].
The resonance radiation trapping operators are constructed for a two-isotope excited atom ensemble allowing for interisotope resonance photon exchange. The nonlinear polarizability of a ring-laser medium is calculated using the strong collision model and an expression is obtained which relates the exchange parameter with the isotope shift due to the resonance transition and with the trapping parameter. Relationships are derived and analyzed for the nonlinear self-interaction and interaction parameters of the opposite waves under complete exchange conditions by accurately solving a system of kinetic equations.