Even degenerate levels of doping imply low concentrations of impurities with respect to the base semiconductor.
2.
This quantity always vanishes for non-degenerate levels of atoms, because these are eigenstates of the parity operator.
3.
You can have an atom with two almost degenerate levels ( the energy eigenvalues are almost identical ) and a transition between the two levels is possible.
4.
At the rising part of the pulse ( a ) the excited state ( with two degenerate levels 1 and 2 ) are not in multiphoton resonance with the ground state.
5.
As the doping concentration is increased, electrons populate states within the conduction band which pushes the Fermi level higher in energy and in the case of degenerate level of doping, the Fermi level lies inside the conduction band.
6.
Under subsequent action of the same pulse, due to interference in the transition amplitudes of the lambda system, the field cannot ionize the population completely and a fraction of the population will be trapped in a coherent superposition of the quasi degenerate levels.
7.
In general the strength of the trapping will be determined by the strength of the two photon coupling between the quasi-degenerate levels via the continuum . In 1996, using the very stable laser and by minimizing the masking effects of the focal region expansion with increasing intensity, Talebpour et al . observed structures on the curves of singly charged ions of Xe, Kr and Ar.
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