2016
DOI: 10.1016/j.optcom.2016.03.017
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Effects of quantum noise on the nonlinear dynamics of a semiconductor laser subject to two spectrally filtered, time-delayed optical feedbacks

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Cited by 5 publications
(3 citation statements)
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References 27 publications
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“…[29][30][31], which confirms our new results and expectations. From the results, under OFB in the weak region and when the LD is operating in the CW or PO region, we found that although the decrease/increase in the LEF/SEF causes an enhancement/reduction in the laser stability/noise, as presented in Figure 5, it causes considerable shifts in the lasing frequency and corrupts the LD efficiency in applications [32].…”
Section: Discussionmentioning
confidence: 88%
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“…[29][30][31], which confirms our new results and expectations. From the results, under OFB in the weak region and when the LD is operating in the CW or PO region, we found that although the decrease/increase in the LEF/SEF causes an enhancement/reduction in the laser stability/noise, as presented in Figure 5, it causes considerable shifts in the lasing frequency and corrupts the LD efficiency in applications [32].…”
Section: Discussionmentioning
confidence: 88%
“…[2 which confirms our new results and expectations. From the results, under OFB weak region and when the LD is operating in the CW or PO region, we found th hough the decrease/increase in the LEF/SEF causes an enhancement/reduction in t ser stability/noise, as presented in Figure 5, it causes considerable shifts in the frequency and corrupts the LD efficiency in applications [32]. By transmitting to the PO state, when the LEF α = 1 and the SEF C = 10 −4 , 10 −5 , and 10 −6 , the peak value of the RIN with OFB is enhanced to higher values (four orders of magnitude) (dashed line) compared with the solitary laser RIN (solid line) at the relaxation frequency f r , as shown in Figure 4(a1-a3).…”
Section: Rin Spectra Of Ld For Various Statesmentioning
confidence: 94%
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