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

Sub-Doppler features due to double dark resonances

A. V. Sharypov, A. D. Wilson‐Gordon

Published Jun 13, 2009• 1 citation
Publisher
DOI
10.1016/j.optcom.2009.05.041

Related papers

Sub-Doppler Satellites of Dark-Line Atomic Resonances in the Case of Ordinary Vapour Cell and Extremely Thin Cell

Y. Pashayan-Leroy, David G. Sarkisyan, Armen D. Sargsyan +2 more

•Jun 7, 2006•0 citations

Dark resonances with variable Doppler sensitivity (4 pages)

Danijela Rostohar, Christian Bolkart

Physical Review A•Jan 1, 2005•0 citations

Effect of Doppler broadening on the transparency and dispersion of the generalized double dark resonance

C. Y. Ye, Alexander S. Zibrov, Yuri V. Rostovtsev

Spectroscopy of the Doppler broadened Rb atomic vapour coherently driven by two coupling fields is presented. Double dark resonances have been observed in different geometries of the coupling fields. A simple four-level model explains the basic counter-intuitive features of experimental spectra. The eigenvalues of the atom-field system distinguishing between the various geometries clarify the physics.

Journal of Modern Optics•Mar 1, 2002•10 citations

New phenomena in Doppleron resonances

R. Corbalán, Gaspar T. Orriols, L. Roso +2 more

Optics Communications•Jul 1, 1981•10 citations

Doppleron Resonances in a Three-Level System

E. Arimondo, R. Corbalán, Gaspar T. Orriols +2 more

European Conference on Atomic Physics•Jan 1, 1981•0 citations

Sub-Doppler double-resonance spectroscopy of NH_3 using a tunable-diode laser and a CO laser

W. Weber, R. W. Terhune

Results are given for a Stark-tuned double-resonance experiment, using a CO-laser pump and a diode-laser probe. The CO laser, operating on the 13-12 P(15) line at 1775.2588 cm(-1), is locked by Lamb-dip stabilization to one of the Stark components of the a(R)R(9, 9) nu(4) line of NH(3). The diode laser probes the aQ(9, 9) nu(2) line at 921.255 cm(-1), revealing a complex spectrum of sub-Doppler features, the narrowest of which are 5.3 +/- 0.3 MHz wide. As well as the resonances associated with population depletion of the common lower levels, we see line-narrowing effects that are due to two-quantum Raman-type processes and collision-induced resonances arising from state-changing collisions that preserve the molecular velocities. The zero-field a(R)R(9, 9) nu(4) line is established to be 264.1 +/- 5.0 MHz above the CO-laser line.

Optics Letters•Oct 1, 1981•15 citations
Results are given for a Stark-tuned double-resonance experiment, using a CO-laser pump and a diode-laser probe. The CO laser, operating on the 13-12 P(15) line at 1775.2588 cm(-1), is locked by Lamb-dip stabilization to one of the Stark components of the a(R)R(9, 9) nu(4) line of NH(3). The diode laser probes the aQ(9, 9) nu(2) line at 921.255 cm(-1), revealing a complex spectrum of sub-Doppler features, the narrowest of which are 5.3 +/- 0.3 MHz wide. As well as the resonances associated with population depletion of the common lower levels, we see line-narrowing effects that are due to two-quantum Raman-type processes and collision-induced resonances arising from state-changing collisions that preserve the molecular velocities. The zero-field a(R)R(9, 9) nu(4) line is established to be 264.1 +/- 5.0 MHz above the CO-laser line.