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

Physica B+C

Collisional perturbation of resonance fluorescence from atoms in a strong monochromatic driving field

F. Schuller, Gerard Nienhuis

Published Feb 1, 1981• 6 citations
Publisher
DOI
10.1016/0378-4363(81)90145-5

Related papers

Resonance Fluorescence of Atoms in Strong Monochromatic Laser Fields

James D. Cresser, J. Häger, Gerd Leuchs +2 more

Topics in current physics•Jan 1, 1982•47 citations

Resonance fluorescence in a strong monochromatic field

E. V. Baklanov

Journal of Experimental and Theoretical Physics•Jun 1, 1974•0 citations

Resonance fluorescence of N entangled atoms in a strong driving field

Chui‐Ping Yang, Guang‐Can Guo

Physica A Statistical Mechanics and its Applications•Nov 1, 1999•11 citations

Radiative transition rates of collisionally perturbed atoms in an intense monochromatic field

F. Schuller, Gerard Nienhuis

Physica B+C•Jun 1, 1983•2 citations

Collisional broadening of saturated resonance fluorescence spectra by two-state atoms irradiated by monochromatic light

Gerard Nienhuis, F Schuller

The authors derive an expression for the spectrum of fluorescence by a two-state atom in a perturber gas irradiated by nearly resonant monochromatic light of arbitrary intensity. The result is fully expressed in terms of the absorption profile that would be measured in a conventional low-intensity absorption experiment and of the rate of radiative and collisional transitions. The present result generalises previous work and the authors demonstrate that expressions obtained before in special cases are recovered by taking the appropriate limits.

Journal of Physics B Atomic and Molecular Physics•Jun 14, 1980•12 citations

Canonical transformation for single-atom resonance fluorescence: The strong-driving-field limit

G. Compagno, Franco Persico

A canonical transformation, which diagonalizes the single-mode radiation Hamiltonian in the rotating wave approximation, is exploited to dress a two-level atom by the strong monochromatic driving field in the resonance fluorescence phenomenon. Langevin equations of motion are obtained for dressed atomic operators, and their solutions yield the amplitude of waves scattered into the fluorescence field. The power spectrum of the scattered field is obtained from the first-order correlation functions between dressed atomic operators. The results of the present treatment are compared with others, and advantages and disadvantages of the present method are discussed.

Physical Review A•Nov 1, 1980•15 citations
The authors derive an expression for the spectrum of fluorescence by a two-state atom in a perturber gas irradiated by nearly resonant monochromatic light of arbitrary intensity. The result is fully expressed in terms of the absorption profile that would be measured in a conventional low-intensity absorption experiment and of the rate of radiative and collisional transitions. The present result generalises previous work and the authors demonstrate that expressions obtained before in special cases are recovered by taking the appropriate limits.
A canonical transformation, which diagonalizes the single-mode radiation Hamiltonian in the rotating wave approximation, is exploited to dress a two-level atom by the strong monochromatic driving field in the resonance fluorescence phenomenon. Langevin equations of motion are obtained for dressed atomic operators, and their solutions yield the amplitude of waves scattered into the fluorescence field. The power spectrum of the scattered field is obtained from the first-order correlation functions between dressed atomic operators. The results of the present treatment are compared with others, and advantages and disadvantages of the present method are discussed.