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

Bulletin of the Russian Academy of Sciences Physics

Phase conjugation at 10.6 microns in InAs in the cavity of a CO2 laser

Valeri I. Kovalev, A. V. Platov, M. B. Suvorov

Published Feb 1, 1988• 0 citations
OpenAlex

Related papers

Phase conjugation in long pulse CO2 lasers

Eric K. Gorton, A. M. Richmond

Optics Communications•Nov 1, 1991•3 citations

Phase Conjugation of CO2 Laser Radiation and Its Applications

V E Sherstobitov

Springer eBooks•Jan 1, 1998•1 citation

Phase Conjugation of CO2 Laser Radiation in Various Media.

Hans H. Klingenberg, Wolfgang Riede, Th. Hall

•Jan 1, 1991•0 citations

Intracavity techniques for high reflectivity phase conjugation at 10.6 µm in germanium and inverted CO2

B. J. Feldman, Robert A. Fisher, Irving J. Bigio +1 more

IEEE Journal of Quantum Electronics•Sep 1, 1979•0 citations

A study of the self-induced phase conjugation of the CO2 laser emission during four-wave interaction

Alexander A. Betin, Konstantin V. Ergakov, O V Mitropol'skiĭ

Technical Physics Letters•Nov 1, 1988•0 citations

Degenerate four-wave mixing and phase conjugation of pulsed CO2 laser radiation on transient gratings inside its own inverted medium

L. A. Afanas’ev, А. А. Ионин, А. А. Котков +3 more

Degenerate four-wave mixing (DFWM) and phase conjugation (PC) of pulsed CO2 laser radiation on transient gratings inside its own laser medium have been studied both experimentally and theoretically. The operational mode of the e-beam controlled discharge CO2 laser has been chosen in such a way (CO2:N2:He equals 1:2:4, p equals 0.28 atm, tin equals 30 microsecond(s) ) that the laser pulse length ((tau) out approximately 10 - 20 microsecond(s) ) is comparable with an effective relaxation time of the upper laser level ((tau) rel approximately 15 - 30 microsecond(s) ). The time-history of the CO2 laser and PC signal pulses, and PC reflectivity have been thoroughly investigated for different cavity Q factors and specific electrical energy inputs. It has been shown, that the formation of the PC signal under the intracavity DFWM on gain (amplitude) and thermal (phase) gratings is characterized by a complicated time history that reflects the main relaxation processes taking place inside the inverted medium. A feature of the transient PC process inside the laser active medium is the dependence of the effective relaxation time of the upper laser level on the intensity of pumping waves. PC reflectivity has been obtained by numerical calculations. A comparison of the theoretical and experimental data confirms the contribution of two different mechanisms of grating formation under DFWM inside the active medium of the CO2 laser.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•Mar 29, 1996•0 citations
Degenerate four-wave mixing (DFWM) and phase conjugation (PC) of pulsed CO2 laser radiation on transient gratings inside its own laser medium have been studied both experimentally and theoretically. The operational mode of the e-beam controlled discharge CO2 laser has been chosen in such a way (CO2:N2:He equals 1:2:4, p equals 0.28 atm, tin equals 30 microsecond(s) ) that the laser pulse length ((tau) out approximately 10 - 20 microsecond(s) ) is comparable with an effective relaxation time of the upper laser level ((tau) rel approximately 15 - 30 microsecond(s) ). The time-history of the CO2 laser and PC signal pulses, and PC reflectivity have been thoroughly investigated for different cavity Q factors and specific electrical energy inputs. It has been shown, that the formation of the PC signal under the intracavity DFWM on gain (amplitude) and thermal (phase) gratings is characterized by a complicated time history that reflects the main relaxation processes taking place inside the inverted medium. A feature of the transient PC process inside the laser active medium is the dependence of the effective relaxation time of the upper laser level on the intensity of pumping waves. PC reflectivity has been obtained by numerical calculations. A comparison of the theoretical and experimental data confirms the contribution of two different mechanisms of grating formation under DFWM inside the active medium of the CO2 laser.