FLUORESCENCE AND ABSORPTION BY A 2-LEVEL ATOM IN A BICHROMATIC FIELD WITH ONE STRONG AND ONE WEAK COMPONENT

Citation
Z. Ficek et Hs. Freedhoff, FLUORESCENCE AND ABSORPTION BY A 2-LEVEL ATOM IN A BICHROMATIC FIELD WITH ONE STRONG AND ONE WEAK COMPONENT, Physical review. A, 53(6), 1996, pp. 4275-4287
Citations number
38
Categorie Soggetti
Physics
Journal title
ISSN journal
10502947
Volume
53
Issue
6
Year of publication
1996
Pages
4275 - 4287
Database
ISI
SICI code
1050-2947(1996)53:6<4275:FAABA2>2.0.ZU;2-T
Abstract
We analyze the fluorescence and absorption spectra of a two-level atom driven by a bichromatic field with frequencies omega(1) and omega(2), separated by omega(2)-omega(1) = 2 delta and Rabi frequencies (at res onance) 2 Omega(1) and 2 Omega(2) such that their ratio alpha = Ohm(2) /Ohm(1)<1. We focus on the case of omega(1) close to the atomic freque ncy omega(0) and omega(2) near the Rabi sideband frequency omega(1) 2 Ohm(1); the detunings are denoted by Delta(1) = omega(0)-omega(1) an d Delta(2) = omega(1) + 2 Ohm(1)-omega(2). We find that the spectra de pend critically on the detuning Delta(2): For large Delta(2), the fluo rescence spectrum consists of the well known Mellow triplet, centered at omega(1); for smaller (but nonzero) Delta(2), the spectrum is compo sed of a triplet at omega(1) together with doublets near the sideband frequencies omega(1) +/- 2 Ohm(1). However, when Delta(2) = 0 (and alp ha much less than 1), the spectrum consists of a doublet centered at o mega(1) and triplets at omega(1)+/-2 Ohm(1):there is then no fluoresce nce at omega(1). As alpha increases, additional triplet structures app ear in the spectrum at frequencies omega(1) +/- 2n Ohm(1) with intensi ties proportional to alpha(2(n-1)), n>1, and a line reappears at omega (1), with intensity proportional to alpha(4). The absorption by the sy stem of a weak probe beam is also strongly dependent on the detuning, and the spectrum is composed of emission-dispersion-absorption feature s located near omega(1) and omega(1) +/- 2n Ohm(1). An analysis in the dressed-atom pic ture is presented which explains the physical origin of all these features, in both fluorescence and absorption.