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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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Citations
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Journal ArticleDOI

Spotlight on Plasmon Lasers

TL;DR: A plasmonics-based design approach is enabling coherent light sources to be built at the nanometer scale, enabling scaling down of photonic devices, similar to the trend in electronics.
Journal ArticleDOI

Quantum Plasmonic Circuits

TL;DR: A survey of recent progress in controlling emission from quantum emitters using plasmonic structures, as well as efforts to engineer surface Plasmon propagation and design plasmanic circuits using these elements can be found in this article.
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Finite-difference time-domain calculation of the spontaneous emission coupling factor in optical microcavities

TL;DR: In this article, the authors presented a general method for the /spl beta/ factor calculation in optical microcavities based on the classical model for atomic transitions in a semiconductor active medium, which is used to evolve the electromagnetic fields of the system and calculate the total radiated energy, as well as the energy radiated into the mode of interest.
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Emission from quantum-dot high-β microcavities: transition from spontaneous emission to lasing and the effects of superradiant emitter coupling

TL;DR: This paper demonstrates that the usual criterion for lasing with a conventional cavity, that is, a sharp non-linearity in the input–output curve accompanied by noticeable linewidth narrowing, has to be reinforced by the equal-time second-order photon autocorrelation function to confirm lasing.
Journal ArticleDOI

Surface plasmon lasers: sources of nanoscopic light

TL;DR: In this paper, a review outlines the science of surface plasmon confinement and the techniques necessary to integrate semiconductors with metal nanostructures for surface plasmons amplification.
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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