1992
DOI: 10.1103/physreva.45.1853
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Spectral hole burning and gain saturation in short-cavity semiconductor lasers

Abstract: A coupled set of equations for carrier distributions and stimulated emission in a semiconductor laser is presented, based on a nonequilibrium Green s-function formulation. Carrier momentum-dependent dephasing caused by carrier-carrier scattering and frequency-dependent optical gain are shown to govern the interplay between carrier relaxation and stimulated recombination. Ignoring the interband Coulomb interaction, the coupled system of equations for the carrier distribution functions and the optical gain is so… Show more

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Cited by 39 publications
(27 citation statements)
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“…The small increase of the carrier distribution at the highmomentum is due to the stimulated absorbtion of photons. The similar results are also found in [9]. …”
Section: Resultssupporting
confidence: 93%
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“…The small increase of the carrier distribution at the highmomentum is due to the stimulated absorbtion of photons. The similar results are also found in [9]. …”
Section: Resultssupporting
confidence: 93%
“…Terms ∝ κ, γ and 1/T are introduced phenomenologically to include the loss and pump of lasers. In the past, the relaxation rate 1/T was calculated microscopically within a Born approximation and a dynamical random-phase approximation [12,9], where the carrier distribution and the kinetic hole are shown to be related to the rate. The self-consistent determination of the rate will be important to discuss the shape of kinetic hole quantitatively, however the detailed analysis is out of scope of the qualitative discussions here.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
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“…The phenomenological approximation shown here is called the relaxation approximation [27]. Each relaxation term suggests that the photon field a 0 decays with a rate of κ, the distribution function n e(h),k is driven to approach the Fermi distribution f e(h),k ( Fig.…”
Section: Mf Smentioning
confidence: 99%
“…When the beating frequency is in a range up to a few THz it leads to a modulation within the carrier distributions because ultrafast nonlinearities in the semiconductor (e.g. carrier heating [56] and spectral hole burning [57,58]) can still follow this modulation. This modulation of the carrier system also modulates the optical properties, e.g.…”
Section: Direct Thz Emissionmentioning
confidence: 99%