Publication | Open Access
Dicke Narrowing Reduction of the Doppler Contribution to a Line Width
13
Citations
4
References
1981
Year
Numerical AnalysisEngineeringFluid MechanicsLine WidthRarefied FlowNumerical SimulationTransport PhenomenaKinetics (Physics)Anomalous DiffusionApproximation TheoryBiophysicsApproximate Line ShapePhysicsSpectral Line WidthDicke Narrowing ReductionInverse ProblemsCollisional NarrowingMultiphase FlowSignal ProcessingRadarDoppler ContributionNatural SciencesApplied PhysicsDiffusion ProcessContinuum ModelingMultiscale Modeling
In the simplest kinetic models of collisional narrowing or reduction of the Doppler contribution to a spectral line width, the narrowing process is related to the usual diffusion constant of transport theory. Dicke narrowing requires a correlation between the pre- and post-collisional absorber or emitter electric dipole moment. Pressure broadening on the other hand results from at least a partial destruction of this correlation so that in general pressure broadening and Dicke narrowing are statistically dependent on and correlated with each other. It follows that a spectroscopic diffusion constant is required. A classical phase description (which is easily converted to a semiclassical one) is used here to derive a kinetic equation for which the approximate line shape is obtained by It velocity moment method. The spectroscopic diffusion constant closely resembles the Chapman-Enskog first approximation for the diffusion constant but has mixed in an extra function (the memory) which represents the correlation between collision-induced changes of the dipole moment and velocity changes and the correlation between the pre- and post-collision electric dipole moment. Dicke narrowing can be used to obtain information about the line broadening amplitude SB(b, w) for strong velocity-changing collisions. The Galatry ('weak' collision) and 'strong' collision line-shape functions are obtained as different cutoff approximations in the velocity moment analysis. The present analysis, however, is not limited to specifically weak or strong collisions. The two line-shape formulae are shown to be virtually identical sufficiently far from the line centre and at sufficiently high densities. Convenient, approximate analytical formulae for the half-width are obtained using two different definitions.
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