2009
DOI: 10.1109/jlt.2009.2029351
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Origin and Control of Sinusoidal Nonlinearities in Wavelength-Tuned Littman External Cavity Laser Diodes

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Cited by 7 publications
(3 citation statements)
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“…2), and t p1 À t v0 and t p4 À t v3 are the half periods of the sinusoidal signal; the ratios of ðt p1 À t s Þ=2ðt p1 À t v0 Þ and ðt e À t p3 Þ=2ðt p4 À t v3 Þ refer to the fractional parts of the interference fringe number. However, when the driving signal of the ECLD is linear, the optical frequency tuning rate is not a constant because the ECLD exhibits nonlinear tunability [10][11][12]. The optical frequency tðtÞ can be expressed in a nonlinear form by Taylor expansion as:…”
Section: Optical Frequency Nonlinearity Analysismentioning
confidence: 99%
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“…2), and t p1 À t v0 and t p4 À t v3 are the half periods of the sinusoidal signal; the ratios of ðt p1 À t s Þ=2ðt p1 À t v0 Þ and ðt e À t p3 Þ=2ðt p4 À t v3 Þ refer to the fractional parts of the interference fringe number. However, when the driving signal of the ECLD is linear, the optical frequency tuning rate is not a constant because the ECLD exhibits nonlinear tunability [10][11][12]. The optical frequency tðtÞ can be expressed in a nonlinear form by Taylor expansion as:…”
Section: Optical Frequency Nonlinearity Analysismentioning
confidence: 99%
“…The linearity of the optical frequency curve is changed by adjusting the parameters in Eq. (10). Accordingly, different L sim values can be obtained by using different linearities of optical frequency for the same true value L true .…”
Section: Optical Frequency Nonlinearity Analysismentioning
confidence: 99%
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