1985
DOI: 10.1049/el:19850714
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Measurement of Rayleigh backscatter-induced linewidth reduction

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Cited by 37 publications
(6 citation statements)
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“…For this measurement the external-cavity laser was operating 5 mA above its 17 mA threshold, and the output power, as a zeroth-order reflection from the grating, was 0.8 mW. Two possible fits, using the standard expression for the self-heterodyne spectrum of coherent laser light with white FM noise superimposed [see ( 5 ) ] , are plotted as curves (1) and (2). The integrated spectral intensity of these fits is calibrated using the area theorem and is taken equal to that of the measured spectrum.…”
Section: Resultsmentioning
confidence: 99%
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“…For this measurement the external-cavity laser was operating 5 mA above its 17 mA threshold, and the output power, as a zeroth-order reflection from the grating, was 0.8 mW. Two possible fits, using the standard expression for the self-heterodyne spectrum of coherent laser light with white FM noise superimposed [see ( 5 ) ] , are plotted as curves (1) and (2). The integrated spectral intensity of these fits is calibrated using the area theorem and is taken equal to that of the measured spectrum.…”
Section: Resultsmentioning
confidence: 99%
“…1. This is because for short delays the delayed optical field is almost a replica of the original and the interference has a strong coherent component, as follows from (5). For short delays, the strength of the selfheterodyne spectrum is proportional to the square of the delay time [see (5) or (6)].…”
Section: Discussed Belowmentioning
confidence: 99%
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“…However, the models developed so far describing the effects produced by optical feedback under laser current modulation, are not referred to RB, since they consider only the reflection coming from a single external cavity [19]- [21], typically put on the back-facet of the laser. At the same time, the effects produced by RB feedback have been considered only with reference to the linewidth reduction [22] and optical frequency shift and hopping [23], [24], in all cases for continuous-wave operation, without considering the presence of a modulating current.…”
mentioning
confidence: 99%
“…The common mean of the linewidth narrowing and wavelength tuning is the employment of frequency-selective optical feedback. 1,2 The optical feedback can be formed by resonant reflection from a confocal cavity 3 and by the Rayleigh backscattering which emerged in a fiber 4,5 or in a microsphere resonator. 6 In general, all these frequency-selective elements have a free spectrum range less than that of a DL cavity, and these determine the lasing wavelength at scales of up to several gigahertz.…”
mentioning
confidence: 99%