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Journal ArticleDOI

Analysis of semiconductor microcavity lasers using rate equations

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TLDR
In this paper, the rate equations for a microcavity semiconductor laser are solved and the steady-state behavior of the laser and some of its dynamic characteristics are investigated, and it is shown that by manipulating the mode density and the spontaneous decay rates of the cavity modes, the threshold gain can be decreased and the modulation speed can be improved.
Abstract
The rate equations for a microcavity semiconductor laser are solved and the steady-state behavior of the laser and some of its dynamic characteristics are investigated. It is shown that by manipulating the mode density and the spontaneous decay rates of the cavity modes, the threshold gain can be decreased and the modulation speed can be improved. However, in order to fully exploit the possibilities which the modification of the spontaneous decay opens up, the active material volume in the cavity must be smaller than a certain value. Threshold current using different definitions, population inversion factor, L-I curves, linewidth, and modulation response are discussed. >

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Citations
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Journal ArticleDOI

Fabrication technologies for quantum cascade photonic-crystal microlasers

TL;DR: In this paper, the authors describe the technological and fabrication methods necessary to incorporate both photonic and electronic-band engineering in order to create novel surface-emitting quantum cascade microcavity laser sources.
Dissertation

III-V semiconductor nanocavities on silicon-on insulator waveguide : laser emission, switching and optical memory

TL;DR: In this article, the authors present a modele for fabriquer des cavites "nanobeam" de facteurs Q tres eleves, encapsulees dans un materiau bas indice.
Book ChapterDOI

Spontaneous Emission Control in Semiconductor Microcavities

TL;DR: The first to realize that stimulated emission and spontaneous emission go hand in hand, Albert Einstein this article showed that the A and B coefficients of spontaneous emission are intimately coupled and showed that spontaneous emission and stimulated emission are correlated.
Journal ArticleDOI

Optically pumped rolled-up InAs/InGaAsP quantum dash lasers at room temperature

TL;DR: In this paper, the fabrication and optical performance of free-standing rolled-up InAs/InGaAsP tube optical cavities, wherein self-organized InAs quantum dots or dashes are incorporated as the gain media, were investigated.
Journal ArticleDOI

Noise and amplitude-squeezing performance of two-polarization-mode semiconductor lasers.

TL;DR: The theoretical results confirm a recent experimental demonstration of the generation of amplitude-squeezed light with VCSEL's and demonstrate that there exists the possibility of squeezing in the two-mode regime besides sub-shot-noise emission in the well-known ideal single-mode operation regime.
References
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Journal ArticleDOI

Electric field dependence of optical absorption near the band gap of quantum-well structures.

TL;DR: Detailed calculations of the shift of exciton peaks are presented including (i) exact solutions for single particles in infinite wells, (ii) tunneling resonance calculations for finite wells, and (iii) variational calculations ofexciton binding energy in a field.
Journal ArticleDOI

Inhibited Spontaneous Emission

TL;DR: The radiative properties of an atom in a cavity differ fundamentally from the atom's radiative property in free space as mentioned in this paper. But the cavity causes slight shifts in the energies of the atom, analogous to radiative shifts.
Journal ArticleDOI

Observation of cavity-enhanced single-atom spontaneous emission

TL;DR: It has been observed that the spontaneous-emission lifetime of Rydberg atoms is shortened by a large ratio when these atoms are crossing a high-Q$ superconducting cavity tuned to resonance with a millimeter-wave transition between adjacent Ryd Berg states as mentioned in this paper.
Journal ArticleDOI

Inhibited spontaneous emission by a Rydberg atom.

TL;DR: Spontaneous radiation by an atom in a Rydberg state is inhibited by use of parallel conducting planes to eliminate the vacuum modes at the transition frequency.
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