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Chapman & Hall/CRC eBooks

Difference Equations for Photon-Number Distribution in the Stationary Regime of a Random Laser

Vlasta Peřinová, A. Lukš

Published Apr 29, 2005• 0 citations
Publisher
DOI
10.1201/9781420034905.ch25

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Difference Equations for Photon-Number Distribution in the Stationary Regime of a Random Laser

Abstract The theory of a laser has provided many semiclassical and quantum models of the laser. Differential-difference equations play a prominent role in the description of the dynamics of the laser. Investigation of the steady state leads to a simplification of these equations to the difference equations. Recent studies of random lasers have aroused interest in the description of traditional lasers.

Chapman & Hall/CRC eBooks•Apr 29, 2005•0 citations

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Approximate photon distribution in lasers

P. P. Jauho, D.O. Riska, Stig Stenholm

Physics Letters A•Apr 1, 1970•3 citations
In the present work the model of a single-atom laser generating in the regime when incoherent pumping rate coincides with the cavity decay rate is theoretically investigated. Using the stationary equation for phase averaged Glauber P function the analytical expressions for mean number of photons and its dispersion are obtained. In the limiting case of the strong-coupling regime the exact expression for the photon number distribution function is derived. Obtained results describe the sub-Poissonian photon statistics and show an increase in mean number of photons to non-zero value when the pumping tends to zero.
We derive the photon-number probability distribution and the resulting degree of second-order optical coherence for light emission from a uniformly distributed active species within a multiple-light-scattering medium. This is obtained from a master equation describing the probability distribution for photons in the vicinity of position r, traveling with a wave vector k, related, in turn, to a coarse-grained average of the optical Wigner coherence function. Using a simple model for isotropic, spatially uncorrelated scatterers, this reduces to a generalization of the master equation of a conventional laser in which the medium behaves like a random collection of low-quality factor cavities that are coupled by photon diffusion between a given cavity and its neighbors. Laserlike coherence, on average, is obtained in the random laser above a specific pumping threshold. Photon-number statistics above and below the lasing threshold are computed by first assuming that the atomic response to the local electromagnetic fields is nearly instantaneous. Corrections to this simple model, arising from nonadiabatic atomic dynamics, are then estimated. The dependence of the photon statistics on scatterer density, gain concentration, and position within a sample reveal that, on average, increase of the scattering strength (decrease of the photon transport mean free path) in the medium leads to a sharper peak in the local photon-number distribution, characteristic of increased local coherence in the optical field. We also evaluate the coherence of the output field at points outside the random-laser medium. This is a weighted average of radiation emitted at different positions in the sample, exhibiting varying degrees of coherence due to variations in the local pumping intensity.