1996
DOI: 10.1063/1.2807693
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Physics of Optoelectronic Devices

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Cited by 765 publications
(889 citation statements)
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“…In order to estimate how much material gain was achieved from nanoresonators under electrical injection, we fit EL spectra using well-known equations 48 for material gain g and spontaneous emission r sp , as shown inequations (1-4). Supplementary Table 1 defines the variables in the equations.…”
Section: Methodsmentioning
confidence: 99%
“…In order to estimate how much material gain was achieved from nanoresonators under electrical injection, we fit EL spectra using well-known equations 48 for material gain g and spontaneous emission r sp , as shown inequations (1-4). Supplementary Table 1 defines the variables in the equations.…”
Section: Methodsmentioning
confidence: 99%
“…Particularly for direct electrical modulation, which will be important for communication applications, factors like non-linear gain compression restrict the modulation bandwidth before the  p limit is reached 23 . Small laser cavities have also been shown to significantly modify the rate of spontaneous emission 17,19,20 which can enhance the modulation bandwidth, particularly if the cavity is used as a light emitting diode rather than a laser [23][24][25][26] . In optical signal processing applications however, optical modulation bandwidth could approach the photon lifetime limit 27 .…”
Section: Limits On Laser Sizementioning
confidence: 99%
“…In applications where a constant output power is required, strong damping of the relaxation oscillations is therefore favorable. The relaxation-oscillation frequency is important for modulation applications, as a modulation of the laser with a frequency near ω RO can resonantly excite relaxation oscillations and lead to unwanted nonuniform laser responses [CHU95], as will be discussed in Sec. 3.4.…”
Section: Laser Dynamics -Relaxation Oscillationsmentioning
confidence: 99%