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IntroductionIntroduction
We would likeWe would like
– More wavelengthsMore wavelengths
– Fewer expensive components (HNLF,Fewer expensive components (HNLF,
EDFAs)EDFAs)
We will deal with each issue in turnWe will deal with each issue in turn
10. 09/24/1309/24/13 1010
ConclusionConclusion
We have demonstrated an SPM-basedWe have demonstrated an SPM-based
self-pulsating source that isself-pulsating source that is
– MultiwavelengthMultiwavelength
– EconomicalEconomical
– FlexibleFlexible
– Simple in designSimple in design
Editor's Notes
[1] P. V. Mamyshev, “All-optical data regeneration based on self-phase modulation effect,” in Proc. Eur. Conf. Optical Communication (ECOC) , 1998, pp. 475–476
This source has been previously simulated and experimentally tested by other researchers [2] M. Rochette, L. R. Chen, K. Sun, and J. Hernández-Cordero, “Multiwavelength and Tunable Self-Pulsating Fiber Cavity Based on Regenerative SPM Spectral Broadening and Filtering”, IEEE Photonics Technology Letters, Vol. 20, No. 17, September 1, 2008 [3] K. Sun, M. Rochette, and L. R. Chen, “Output characterization of a self-pulsating and aperiodic optical fiber source based on cascaded regeneration” Optics Express Vol. 17, No. 12, 10419, 8 June 2009
We have implemented and tested this source; it produces
These peaks have a spacing of 48 kHz, which is the repetition rate of the pulse train. Due to the relationship L = cT = c0/(n/\f) where is the cavity length travelled by the pulse, n is the refractive index and /\nu is the frequency spacing between peaks, this indicates a cavity length of 4.31 km