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

17th Congress of the International Commission for Optics: Optics for Science and New Technology

A partial coherence resonance fluorescence analysis

Javier J. Sanchez-Mondragon

Published Sep 1, 1996• 0 citations
Publisher

Abstract

We present the resonance fluorescence spectrum produced by a partially coherent external field, described by its even order correlation. We discuss CW [1] partial coherence but the procedure is suitable for pulse excitation beams where most of recent experimental interest has arised. In our analysis we consider an stochastic driving field and the semiclassical theory of radiation in a two level atom[2].

DOI
10.1117/12.2316131

Related papers

Resonance fluorescence with squeezed light excitation

Reeta Vyas, Surendra Singh

Resonance fluorescence from a single two-level atom driven by a beam of squeezed light is studied in the weak field limit. We consider the situation where the atom is coupled to the ordinary vacuum and only a few field modes corresponding to the driving field are squeezed. The field produced by the degenerate optical parametric oscillator is used as the driving field. This driving field can be described in terms of two real independent Gaussian processes. Heisenberg equations of motion are solved in the steady-state, and analytic expressions for the fluorescent light intensity and the spectrum of fluorescent light are derived. We also consider photon statistics of fluorescent light. In particular, squeezing, antibunching, and sub-Poissonian statistics of fluorescent photons are discussed and analytic expressions for the quadrature variance and the two-time intensity correlation function are presented. Contrary to the case of coherent excitation the second-order intensity correlation function does not factorize.

Annual Meeting Optical Society of America•Jan 1, 1991•0 citations

Resonance fluorescence with squeezed-light excitation

Reeta Vyas, Surendra Singh

Resonance fluorescence from a single two-level atom driven by a beam of squeezed light is studied in the weak-field limit. We consider the situation where the atom is coupled to the ordinary vacuum and only a few field modes corresponding to the driving field are squeezed. The field produced by the degenerate optical parametric oscillator is used as the driving field. Heisenberg equations of motion are solved in the steady-state and analytic expressions for the fluorescent-light intensity and the spectrum of fluorescent light are derived. We also consider photon statistics of fluorescent light. In particular, squeezing, antibunching, and sub-Poissonian statistics of fluorescent photons are discussed, and analytic expressions for the quadrature variance and the two-time intensity correlation function are presented. Contrary to the case of coherent excitation, the second-order intensity correlation function does not factorize. This and other differences are discussed, and curves are presented to illustrate the behavior of various quantities. We also present results for thermal excitation of the atom.

Physical Review A•Jun 1, 1992•33 citations

Resonance fluorescence of a two-level atom driven by a fluctuating laser field: an application of a multiple time scale method

S. Chaturvedi, Crispin W. Gardiner

The authors review the various models of fluctuating laser fields which have been used in the past for the treatment of resonance fluorescence of a driven two-level atom. A new treatment of this problem in the case of a partially coherent laser field is given. This method extends that of Zoller (1977, 1978) to a large ratio of atomic decay constant to driving field frequency. The method is a kind of multiple time scale method, applied to a stochastic differential equation, and is of interest in its own right. It gives a systematic expansion in powers of the ratio of the atomic decay constant to driving field frequency, and can in principle be computed to arbitrary accuracy. Computations are presented to assess the effect of the high corrections determined.

Journal of Physics B Atomic and Molecular Physics•Apr 14, 1981•16 citations

Atomic Relaxation in the Presence of Intense Partially Coherent Radiation Fields

Joseph H. Eberly

I develop a nonperturbative relaxation theory appropriate for an atom subjected to strong finite-bandwidth radiation fields. The partial coherence implied by the finite bandwidth is modeled by simple phase and amplitude correlation functions. Modifications of the Mollow theory of resonance fluorescence are calculated as an example. The finite bandwidth of the applied field does not have a simply additive effect on the predicted fluorescence spectrum.

Physical Review Letters•Nov 22, 1976•203 citations

Intensity correlations in resonance fluorescence from coupled two-level atoms

Marco Wiegand

The normalised intensity correlation function of resonance fluorescence radiation from two-level atoms is studied in various respects. In the first part of the paper the author discusses only interference effects for several uncoupled, linearly arranged, atoms. It is shown that, depending on the distance between the atoms, the direction of observation and the strength of the driving field, an antibunching effect as well as a very big bunching effect may be observed. In the second part of the paper he studies for the case of two atoms and weak external fields the influence of the interaction between the atoms by means of a perturbation theory. It is shown that the coupling between the atoms strongly modifies the normalised intensity correlation function in comparison with the case of uncoupled atoms. He takes as the driving field a coherent external field as well as laser light and thermal light.

Journal of Physics B Atomic and Molecular Physics•Apr 14, 1983•10 citations

Collective resonance fluorescence in an intense laser field with phase and amplitude fluctuations

A.S. Shumovsky, R. Tanaś, Tran Quang

The collective resonance fluorescence from a system of two-level atoms resonantly driven by a strong laser field with the phase and amplitude fluctuations is considered. The effect of the laser field fluctuations on the spectrum as well as the degrees of the second-order coherence of the fluorescent field is discussed in detail for the off-resonance case.

Journal de physique•Jan 1, 1988•3 citations
We present the resonance fluorescence spectrum produced by a partially coherent external field, described by its even order correlation. We discuss CW [1] partial coherence but the procedure is suitable for pulse excitation beams where most of recent experimental interest has arised. In our analysis we consider an stochastic driving field and the semiclassical theory of radiation in a two level atom[2].
Resonance fluorescence from a single two-level atom driven by a beam of squeezed light is studied in the weak field limit. We consider the situation where the atom is coupled to the ordinary vacuum and only a few field modes corresponding to the driving field are squeezed. The field produced by the degenerate optical parametric oscillator is used as the driving field. This driving field can be described in terms of two real independent Gaussian processes. Heisenberg equations of motion are solved in the steady-state, and analytic expressions for the fluorescent light intensity and the spectrum of fluorescent light are derived. We also consider photon statistics of fluorescent light. In particular, squeezing, antibunching, and sub-Poissonian statistics of fluorescent photons are discussed and analytic expressions for the quadrature variance and the two-time intensity correlation function are presented. Contrary to the case of coherent excitation the second-order intensity correlation function does not factorize.
Resonance fluorescence from a single two-level atom driven by a beam of squeezed light is studied in the weak-field limit. We consider the situation where the atom is coupled to the ordinary vacuum and only a few field modes corresponding to the driving field are squeezed. The field produced by the degenerate optical parametric oscillator is used as the driving field. Heisenberg equations of motion are solved in the steady-state and analytic expressions for the fluorescent-light intensity and the spectrum of fluorescent light are derived. We also consider photon statistics of fluorescent light. In particular, squeezing, antibunching, and sub-Poissonian statistics of fluorescent photons are discussed, and analytic expressions for the quadrature variance and the two-time intensity correlation function are presented. Contrary to the case of coherent excitation, the second-order intensity correlation function does not factorize. This and other differences are discussed, and curves are presented to illustrate the behavior of various quantities. We also present results for thermal excitation of the atom.
The authors review the various models of fluctuating laser fields which have been used in the past for the treatment of resonance fluorescence of a driven two-level atom. A new treatment of this problem in the case of a partially coherent laser field is given. This method extends that of Zoller (1977, 1978) to a large ratio of atomic decay constant to driving field frequency. The method is a kind of multiple time scale method, applied to a stochastic differential equation, and is of interest in its own right. It gives a systematic expansion in powers of the ratio of the atomic decay constant to driving field frequency, and can in principle be computed to arbitrary accuracy. Computations are presented to assess the effect of the high corrections determined.
The normalised intensity correlation function of resonance fluorescence radiation from two-level atoms is studied in various respects. In the first part of the paper the author discusses only interference effects for several uncoupled, linearly arranged, atoms. It is shown that, depending on the distance between the atoms, the direction of observation and the strength of the driving field, an antibunching effect as well as a very big bunching effect may be observed. In the second part of the paper he studies for the case of two atoms and weak external fields the influence of the interaction between the atoms by means of a perturbation theory. It is shown that the coupling between the atoms strongly modifies the normalised intensity correlation function in comparison with the case of uncoupled atoms. He takes as the driving field a coherent external field as well as laser light and thermal light.