Resonance fluorescence with bichromatic excitation and nonresonant squeezed reservoir: iterative approach

2012 ◽  
Vol 90 (5) ◽  
pp. 449-460 ◽  
Author(s):  
S.S. Hassan ◽  
R.A. Alharbey

An iterative approach, not restricted to field strength nor to resonance conditions, is used to solve the nonautonomous Bloch equations modeling the interaction of a bichromatically driven two-level atom in the presence of an off-resonant broadband squeezed vacuum (SV) radiation reservoir. The system parameters are chosen such that the absolute difference between the iterative and (exact) numerical solutions is [Formula: see text](10−2) or less. For some limiting cases, range of validity of the iterative procedure is estimated analytically. The derived analytical solutions are used to calculate the transient fluorescent spectrum. Some previously obtained results (both experimental and theoretical) in the normal vacuum case are recovered. In the SV case, with strong resonant (off-resonant) bichromatic field strength, the transient spectrum shows many symmetrical (asymmetrical) resonances of weights and locations dependent on the SV detuning parameter.

1990 ◽  
Vol 41 (11) ◽  
pp. 6013-6022 ◽  
Author(s):  
Helen Freedhoff ◽  
Zhidang Chen

1980 ◽  
Vol 58 (11) ◽  
pp. 1570-1579 ◽  
Author(s):  
M. P. Sharma ◽  
A. Balbin Villaverde ◽  
Constantine Mavroyannis

We have studied the fluorescence spectra arising from the interaction of a three-level atom with two strong electromagnetic fields whose initially populated modes are equal to the two atomic transition frequencies, respectively. The Green's function formalism has been used to calculate the excitation spectrum of the system. An expression for the spectral function describing the excitation spectrum of the system has been derived in a closed form in the limit of high photon densities. Numerical computation of the expression for the spectral function indicates that at each transition frequency there may exist either one pair or two pairs or three pairs of sidebands, in addition to the central peak, depending upon the relative strength of the Rabi frequencies involved.


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