Abstract

We study the collective scattering of radiation by a large ensemble of Na≫1 atoms, in the presence of a pump field. We use the wave-kinetic approach where the center-of-mass position of the moving atoms is described by a microscopic discrete distribution, or alternatively, by a Wigner distribution. This approach can include thermal effects and quantum recoil in a natural way, and even consider atomic ensembles out of equilibrium. We assume two-level atoms with atomic transition frequency ωa very different from the frequency ω0 of the pump field. We consider both the quasi-classical and quantum descriptions of the center-of-mass motion. In both cases, we establish the unstable regimes where coherent emission of radiation can take place.

Highlights

  • Collective atomic processes between atoms and radiation are of fundamental importance in several areas of physics, with relevance for laser cooling [1], Bose–Einstein condensation [2], free-electron lasers [3], or super-radiant photon emission and scattering [4,5]

  • They first used a quasi-classical description, which was extended to include the quantum recoil associated with photon emission and absorption [8,9]

  • We start with the equations describing the evolution of an ensemble of two-level atoms coupled with radiation, when the atoms are submitted to an intense pump field

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Summary

Introduction

Collective atomic processes between atoms and radiation are of fundamental importance in several areas of physics, with relevance for laser cooling [1], Bose–Einstein condensation [2], free-electron lasers [3], or super-radiant photon emission and scattering [4,5]. Bonifacio and collaborators in 1994 [6,7], as the atomic physics equivalent of a free-electron laser, where the electron beams are replaced by moving atoms They first used a quasi-classical description, which was extended to include the quantum recoil associated with photon emission and absorption [8,9]. The wave-kinetic approach followed here can partly be considered an extension of our previous kinetic model for the free-electron laser [11], when electrons in a relativistic beam are replaced by slowly moving atoms.

Basic Equations
Radiation Instability
Quantum Recoil
Conclusions
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