We study resonance flourescence in a four level ladder system and illustrate some novel features due to quantum interference and atomic coherence effects. We find that under three photon resonant conditions, in some region of the parameter space of the rabi frequencies
Ω1,Ω2,Ω3, emission is dominantly by the level 4 at the line center even though there is an almost equal distribution of populations in all the levels. As one increases
Ω3 with
Ω1andΩ2 held fixed, the four level system 'dynamically collapses' to a two level system. The steady state populations and the the resonance flourescence from all the levels provide adequate evidence to this effect.
The time evolution of the antibunching and quantum beat is studied by considering the resonant interaction of two radiation fields with a cascade three-level atom. It is found that different initial atomic states and different ratios of the average photon number of two radiation fields as well as the different coupling coefficients have a remarkable influence on the antibunching and quantum beat of two radiation fields. By numerical summation and a number of figures, it is interesting to note that under certain conditions, some strange behaviour occurs in this cascade three-level atomic system. The explanation of these strange behaviours is given.
A theoretical investigation is made of the specific polarisation rotation and the intensity quantum beats of the three-level stimulated photon echoes from a gas medium in a longitudinal magnetic field. These effects are found to be due to the precession of the atomic polarisation and magnetic moment. An interesting structure of the photon echoes in a strong magnetic field (which is also referred to as quantum beats) was discovered. An analysis of various types of photon-echo quantum beats in a magnetic field is given. It is shown that the use of the optimum polarisations of the exciting pulses gives rise to photon-echo quantum beats of a simple form. The results obtained allow the g factors and the total angular momenta of resonant atomic levels to be experimentally determined.