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Raphael Bouskila,Raphael Bouskila, Martin RochetteMartin Rochette
Photonic Systems GroupPhotonic Systems Group
McGill University, Montréal QCMcGill University, Montréal QC
Three-wavelength self-pulsatingThree-wavelength self-pulsating
fiber sourcefiber source
09/24/1309/24/13 22
OutlineOutline
 IntroductionIntroduction
 3-wavelength ring configuration3-wavelength ring configuration
 3-wavelength polarization-based3-wavelength polarization-based
recirculating configurationrecirculating configuration
– ResultsResults
 ConclusionConclusion
09/24/1309/24/13 33
IntroductionIntroduction
 Self-pulsating fiber source based on 2R opticalSelf-pulsating fiber source based on 2R optical
regeneratorregenerator
09/24/1309/24/13 44
IntroductionIntroduction
 Self-pulsation arises in ring configurationSelf-pulsation arises in ring configuration
09/24/1309/24/13 55
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
09/24/1309/24/13 66
Three-wavelength sourceThree-wavelength source
09/24/1309/24/13 77
Polarization-based setupPolarization-based setup
 Fewer EDFAs, lengths of HNLF requiredFewer EDFAs, lengths of HNLF required
 Functionally similarFunctionally similar
09/24/1309/24/13 88
Optical spectraOptical spectra
-60
-55
-50
-45
-40
-35
-30
-25
-20
-15
1520 1525 1530 1535 1540 1545 1550
Wavelength (nm)
Power(dBm)
Lambda1 unfiltered Lambda1 filtered Lambda2 filtered Lambda3 filtered
09/24/1309/24/13 99
RF spectrumRF spectrum
-130
-120
-110
-100
-90
-80
-70
-60
-50
0 50 100 150 200 250
Frequency (kHz)
Power(dBm)
48 kHz  4.31 km
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

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Three-wavelength self-pulsating fiber source

Editor's Notes

  1. [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
  2. 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
  3. We have implemented and tested this source; it produces
  4. 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