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

秋の分科会講演予稿集

13a-P-3 Light Modulation in the Optical Pumping Experiment(2)

滋 安東, 清人 大川, 高啓 久保

Published Oct 12, 1967• 0 citations
OpenAlex

Related papers

4a-E-2 Light Modulation in Optical Pumping Experiment

高啓 久保, 清人 大川

日本物理学会年会講演予稿集•Apr 2, 1967•0 citations

Transverse optical pumping with polarization-modulated light

Harald Klepel, Dieter Suter

Optics Communications•Jun 1, 1992•18 citations

4He optical pumping with polarization modulated light

H. Gilles, Bernard Cheron, J. Hamel

Optics Communications•Mar 1, 1991•13 citations

Spin Exchange and Light Modulation in Optically Pumped Sodium.

George A. Ruff

•Jan 1, 1967•0 citations

Theory of the modulation of light in optical pumping experiments

George William Series

The absorption of light by optically pumped atoms undergoing magnetic resonance is calculated from expressions based on a simplification of Barrat and Cohen-Tannoudji's theory of optical pumping. The density matrix for the system is first derived in orders of approximation which correspond to successive cycles of pumping. The off-diagonal elements of the matrix, and consequently the absorption of light, are modulated. The amplitudes of modulation are resonance functions which are, in general, more complicated than solutions of the Bloch equations. The selection rules for electric dipole radiation limit the possible frequencies of modulation to ω0 and 2ω0 for primary interactions (ω0 is the applied frequency), but modulation at higher frequencies can arise through the circulation of coherence in optical pumping cycles. The functions which represent the amplitude of modulation at 4ω0 are derived in first and second order, for comparison with experiment.

Proceedings of the Physical Society•Aug 1, 1966•17 citations

Dressed-atom model for optical pumping with modulated light

Krystyna Kolwas, M. Kolwas

Optics Communications•May 1, 1976•6 citations
The absorption of light by optically pumped atoms undergoing magnetic resonance is calculated from expressions based on a simplification of Barrat and Cohen-Tannoudji's theory of optical pumping. The density matrix for the system is first derived in orders of approximation which correspond to successive cycles of pumping. The off-diagonal elements of the matrix, and consequently the absorption of light, are modulated. The amplitudes of modulation are resonance functions which are, in general, more complicated than solutions of the Bloch equations. The selection rules for electric dipole radiation limit the possible frequencies of modulation to ω0 and 2ω0 for primary interactions (ω0 is the applied frequency), but modulation at higher frequencies can arise through the circulation of coherence in optical pumping cycles. The functions which represent the amplitude of modulation at 4ω0 are derived in first and second order, for comparison with experiment.