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

KvanE

Asymmetry of light amplification in optically thick active media

S. G. Voloshenyuk, L. V. Vovk, E I Zabello, Eugene A. Tikhonov

Published May 1, 1989• 0 citations
OpenAlex

Related papers

Asymmetry of stimulated emission in active dye media

Eugene A. Tikhonov, N M Narovlyanskaya

•Jan 1, 1979•0 citations

Frequency conversion light waves in optically active media

B. V. Bokut', Anatoly N. Serdyukov

Journal of Applied Spectroscopy•Jan 1, 1970•0 citations

Coherent amplification, reflection, and induced superradiance in activated media.

Aleksandr M Leontovich, A. M. Mozharovskiǐ, Evgenii Dmitrievich Trifonov

Soviet Physics Uspekhi•Nov 30, 1986•2 citations

Asymmetry of the amplification of light in optically dense active media

S. G. Voloshenyuk, L. V. Vovk, E I Zabello +1 more

An asymmetry effect in the amplification and efficiency of an optically dense amplifier is predicted theoretically and confirmed experimentally for opposite and concurrent collinear signal and pump paths. The effect is due to a difference in the losses as a result of the two-stage absorption of pump radiation in a system of luminescing centers described by a model of three energy levels. Calculations are made of various characteristics of this type of amplifier using the quasisteady-state approximation.

Soviet Journal of Quantum Electronics•May 31, 1989•2 citations

Influence of optical Stark effect on the amplification of intense light pulses in resonance media

Vladimir D Taranukhin, M. Yu. Pogosbekyan

The amplification of intense light pulses in resonance active media with an optical Stark effect and coherence effects is examined theoretically. In the course of the amplification, the pulse may go through a stage of an incoherent Stark quasisoliton. The envelope of this quasisoliton has an approximately constant, highly asymmetric shape. The energy of the quasisoliton is approximately constant. Upon further amplification, the Stark quasisoliton "breaks up" into a train of shorter pulses. Over a sufficiently long amplification distance, a true soliton may form in the active medium. In general, this true soliton is not the same as a standard π pulse in a medium without a Stark effect.

Quantum Electronics•Aug 31, 1993•1 citation

Nonlinear Optical Phenomena in Active Media

George C. Baldwin

Springer eBooks•Jan 1, 1969•1 citation
An asymmetry effect in the amplification and efficiency of an optically dense amplifier is predicted theoretically and confirmed experimentally for opposite and concurrent collinear signal and pump paths. The effect is due to a difference in the losses as a result of the two-stage absorption of pump radiation in a system of luminescing centers described by a model of three energy levels. Calculations are made of various characteristics of this type of amplifier using the quasisteady-state approximation.
The amplification of intense light pulses in resonance active media with an optical Stark effect and coherence effects is examined theoretically. In the course of the amplification, the pulse may go through a stage of an incoherent Stark quasisoliton. The envelope of this quasisoliton has an approximately constant, highly asymmetric shape. The energy of the quasisoliton is approximately constant. Upon further amplification, the Stark quasisoliton "breaks up" into a train of shorter pulses. Over a sufficiently long amplification distance, a true soliton may form in the active medium. In general, this true soliton is not the same as a standard π pulse in a medium without a Stark effect.