Z. Ficek et Hs. Freedhoff, RESONANCE-FLUORESCENCE AND ABSORPTION-SPECTRA OF A 2-LEVEL ATOM DRIVEN BY A STRONG BICHROMATIC FIELD, Physical review. A, 48(4), 1993, pp. 3092-3104
We examine the radiative properties of a two-level atom driven by a st
rong bichromatic field with frequencies omega1=omega0-delta1 and omega
2=omega0+delta2, which can be asymmetrically placed about the atomic t
ransition frequency omega0 and can have different Rabi frequencies OME
GA1 and OMEGA2. Applying the optical Bloch equations for the bichromat
ic excitation, we derive an infinite set of equations of motion for th
e time evolution of the atomic variables. The equations are solved num
erically by matrix inversion and Laplace transforms. Using the quantum
regression theorem, we then solve for the steady-state total fluoresc
ence intensity, and the resonance-fluorescence and absorption spectra.
The spectra are found to depend on the frequency difference 2delta=de
lta1+delta2, the average detuning DELTA=omega0- 1/2(omega1+omega2), an
d the Rabi frequencies of the driving fields. For OMEGA1=OMEGA2=OMEGA,
the total fluorescent intensity displays a series of maxima for DELTA
=+/-ndelta-/+OMEGA2/4delta, where the n are the odd integers. The inte
nsity-dependent shift from the resonances ndelta is explained as an an
alog pf the generalized Bloch-Siegert shift. The resonance-fluorescenc
e spectrum for DELTA not-equal O appears to contain more peaks than th
at for DELTA=0. This is due to the splitting of the central peak and t
he even sidebands into doublets. The absorption spectrum of a weak-pro
be beam for DELTA=0 and equal Rabi frequencies consists of a symmetric
series of dispersionlike sidebands separated from omega0 by integer m
ultiples of delta2 together with a central absorption peak at omega0,
whose amplitude oscillates with OMEGA. For DELTA not-equal O and/or OM
EGA1 not-equal OMEGA2, the odd sidebands remain dispersionlike, while
the central peak and the even sidebands split into absorption-emission
doublets. A simple physical interpretation of the spectral features i
s given in terms of the dressed-atom model.