1988
DOI: 10.1063/1.99646
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Effect of low-frequency intensity noise on high-frequency direct modulation of semiconductor injection lasers

Abstract: It was experimentally observed that low-frequency intensity noise in 1.3 μm semiconductor lasers can be translated to high frequencies through beating with a high-frequency modulation signal, thus imposing a maximum achievable signal/noise ratio. An analysis of this effect using a formalism developed for treating intermodulation distortion yields good agreement with the experimental results.

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Cited by 36 publications
(10 citation statements)
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“…The modulated laser signal was found to be either continuous or pulsing; each has period doubling or is superposed by relaxation oscillations depending on the modulation conditions. Similar experimental results were also reported [9,10].…”
supporting
confidence: 80%
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“…The modulated laser signal was found to be either continuous or pulsing; each has period doubling or is superposed by relaxation oscillations depending on the modulation conditions. Similar experimental results were also reported [9,10].…”
supporting
confidence: 80%
“…It was observed in experiments that the modulated signal of the laser has nonlinear forms with different degrees of signal distortion and noise levels in both regimes of low and high modulation frequencies [10,11]. Explanation of such effects in modulated laser diodes that support more than one mode oscillations and in the deploying fiber links was given phenomenologically in terms of the laser nonlinearity and mode competition [9]. Trustworthy analyses, however, of these frequency domain properties should correlate them with the time-domain characteristics of competition among the oscillating modes.…”
mentioning
confidence: 99%
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“…Recent measurements show that the low frequency relative intensity noise (RIN) can be substantially enhanced for multimode as well as single mode lasers [1]. This effect, which has important systems implications, is not predicted by conventional single mode rate equation modeling of the lasers RIN.…”
Section: Relative Intensity Noisementioning
confidence: 97%
“…1 s h o w the RF spectrum of a directly modulated bulk 1.3 pm-wavelength Fabry-Perot laser. The wings of the RF spectrum surrounding the peak at 3 GHz (modulation frequency) are caused by translatilm of the low-frequency intensity noise to the subcarrier frequency [6]. The different RF spectra are paired with different optical emission spectra (inserts) arising from small changes in the current (.<2 mA) and temperature (5 degrees) at constant power.…”
mentioning
confidence: 99%