Local field effect as a function of pulse duration
arXiv:1008.2587 · doi:10.1103/PhysRevA.82.015802
Abstract
In this note we give semiclassical consideration of the role of pulse duration in observation of local field effects in the regime of optical switching. We show that the main parameter governing local field influence is the ratio of peak Rabi frequency corresponding to medium inversion and Lorentz frequency of the medium. To obtain significant local field effect, this parameter should be near unity that is valid only for long enough pulses. We also discuss the role of relaxation and pulse shape in this processes.
4 pages, 3 figures
References in corpus (6)
- Quantum field theory of cooperative atom response: Low light intensity
- Radiative atom-atom interactions in optically dense media: Quantum corrections to the Lorentz-Lorenz formula
- Lorentz-Lorenz shift in a Bose-Einstein condensate
- Spontaneous emission and level shifts in absorbing disordered dielectrics and dense atomic gases: A Green's function approach
- Single-cycle gap soliton in a subwavelength structure
- Compression of an intensive light pulse in a dense resonant medium and photonic-band-gap structures containing it
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