Figure 1 - Schematic of the 'dressing' of electron energy levels by a strong coupling beam9.


From the following article

Gain without inversion in semiconductor nanostructures

M. D. Frogley, J. F. Dynes, M. Beck, J. Faist and C. C. Phillips

Nature Materials 5, 175 - 178 (2006)

doi:10.1038/nmat1586

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a, When driven at h strokeomegacapproxE12, a two-level system evolves into two doublets, each split by the Rabi energy, h strokeOmegaRabi, denoted by the red arrows, which itself increases monotonically with the coupling beam intensity. b, The three-level system whose 'bare' transition energies are denoted by the solid black arrows. Most (approx80%) of the electrons remaining in state |1right fence and the gain arising from coherences appearing in the upper two states, which have been split into Rabi doublets by the off-resonant coupling beam. Upward green arrows represent the coupling photons, the downward dashed arrows are the transitions generating the optical gain and the blue arrows denote the frequency, h strokeomega0, where extra loss appears.

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