2002
DOI: 10.1109/lpt.2002.1021995
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Symmetric highly efficient (/spl sim/0 dB) wavelength conversion based on four-wave mixing in quantum dot optical amplifiers

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Cited by 122 publications
(51 citation statements)
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“…When a linear amplification of the input signal is required, the flat section of the gain characteristics should extend towards as high input power as possible, leading to a distortion-free amplification of arbitrarily strong optical signals [LAE06a]. On the other hand, optical signals with powers in the nonlinear regime induce a nonlinear response of the amplifier, which can be used, e.g., for wavelength conversion via four-wave-mixing [AKI02,QAS04,MAJ11a,SCH12e] or cross-gain-modulation [KIM09a,MEU10].…”
Section: Gain Saturationmentioning
confidence: 99%
See 1 more Smart Citation
“…When a linear amplification of the input signal is required, the flat section of the gain characteristics should extend towards as high input power as possible, leading to a distortion-free amplification of arbitrarily strong optical signals [LAE06a]. On the other hand, optical signals with powers in the nonlinear regime induce a nonlinear response of the amplifier, which can be used, e.g., for wavelength conversion via four-wave-mixing [AKI02,QAS04,MAJ11a,SCH12e] or cross-gain-modulation [KIM09a,MEU10].…”
Section: Gain Saturationmentioning
confidence: 99%
“…Here, a linear amplification with a low noise figure is required, to ensure low distortion of the input signal [AKI03,BER04,USK05]. On the other hand, nonlinear optical applications, such as four-wave-mixing [AKI02,QAS04,MAJ11a,SCH12e] and cross-gain modulation [KIM09a,MEU10,CON10] for wavelength conversion, as well as regenerative amplification, require a nonlinear response of the optical amplifier. In the nonlinear amplification regime the amplifier response is input-power dependent and will thus lead to signal distortions, which can be utilized, e.g., for pulse shaping…”
Section: Introductionmentioning
confidence: 99%
“…First the bound conduction band states of the QD, which we assume known at this point, are fitted with a parabolic band (similar to a bulk DOS) with the curvature determined by the effective electron mass. Two equations determining the effective conduction bandedge , and the effective single dot volume, , are obtained by integrating over the bulk-like DOS from to the bound energy of either the GS or ES, multiplying by the effective volume of a single dot , and equating it with either the number of states including spin of the GS , or that of the combined GS and ES (19) From these we find (21) and (22) If we now assume , where is the relative bandgap difference between the two materials, originating from the conduction band, we can determine the effective valence bandedge . The contribution to the total effective DOS of the valence band from all dots in the device , can now be written as (23) with being the Heaviside step function and the total number of dots in each dot population.…”
Section: A Hole Occupation Probabilitiesmentioning
confidence: 99%
“…Recently, also QD SOAs have received some attention, mainly focused on their nonlinear properties. Main results include the demonstration of ultrafast gain recovery [17], signal processing and pattern free amplification up to 40 Gbit/s [18] and unique four-wave mixing properties [19]. With respect to their application as linear amplifiers, QD SOAs were predicted to exhibit low noise figure and high saturation power [20], [21].…”
Section: Introductionmentioning
confidence: 99%
“…46-49. Wavelength switching experiments employing ultrashort pulses were published in refs. [50][51][52]. In this paper, we investigate nonlinear carrier dynamics in a MQW-SOA in the context of ultrafast all-optical logic.…”
Section: Introductionmentioning
confidence: 99%