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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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Journal ArticleDOI

Photonic crystals and microdisk cavities based on GaInAsP-InP system

TL;DR: In this paper, the authors presented a preliminary guide to realize microcavity semiconductor lasers exhibiting spontaneous emission control effects, which includes theoretical consideration on the effects; processing techniques for semiconductor micro-cavities; and some demonstrations of photonic crystal and microdisk cavity.
Journal ArticleDOI

Lasing oscillation in a three-dimensional photonic crystal nanocavity with a complete bandgap

TL;DR: In this article, the first laser was constructed by coupling a cavity mode exhibiting the highest quality factor yet achieved (∼38,500) with quantum dots, achieving the first lasing oscillation in a three-dimensional photonic crystal nanocavity.
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Room temperature continuous-wave lasing in photonic crystal nanocavity

TL;DR: Three-dimensional carrier confinement and a low transparent carrier density due to volume effect in a quantum dot system play important roles in the cw laser operation at room temperature as well as a high quality factor photonic crystal nanocavity.
Journal ArticleDOI

Coherent Control of Spontaneous Emission near a Photonic Band Edge: A Single-Atom Optical Memory Device

TL;DR: In this article, coherent control of spontaneous emission from a three-level atom with one resonant frequency near the edge of a photonic band gap was demonstrated, where spontaneous emission can be totally suppressed or strongly enhanced depending on the relative phase between the control and pump laser fields.
Journal ArticleDOI

Ten years of spasers and plasmonic nanolasers.

TL;DR: An international team of researchers has conducted a comprehensive review of the evolution spasers, from their first experimental demonstrations through to technological advances in the field and future research and new applications.
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.
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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.
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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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