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Photonic-chip-based RF
spectrum analyzer
Raphael BouskilaRaphael Bouskila
09/24/1309/24/13 R. BouskilaR. Bouskila 22
OutlineOutline
 IntroductionIntroduction
 WaveguideWaveguide
 RF spectrum analyzerRF spectrum analyzer
 ConclusionConclusion
09/24/1309/24/13 R. BouskilaR. Bouskila 33
IntroductionIntroduction
09/24/1309/24/13 R. BouskilaR. Bouskila 44
WaveguideWaveguide
 Amount of nonlinearity dependent onAmount of nonlinearity dependent on
intensity:intensity:
 Fiber core diameter: ~8-10Fiber core diameter: ~8-10 μμmm
– Effective area: ~50-80Effective area: ~50-80 μμmm22
2
eff
2 n
A
π
γ
λ
=
09/24/1309/24/13 R. BouskilaR. Bouskila 55
WaveguideWaveguide
 Second problem: DispersionSecond problem: Dispersion
– N.B.N.B. DD == DDWGWG ++ DDmatmat
09/24/1309/24/13 R. BouskilaR. Bouskila 66
WaveguideWaveguide
 What to do?What to do?
 Solution: Ridge (or rib) waveguideSolution: Ridge (or rib) waveguide
09/24/1309/24/13 R. BouskilaR. Bouskila 77
WaveguideWaveguide
 High nonlinearityHigh nonlinearity
achieved via extremelyachieved via extremely
high mode confinementhigh mode confinement
– AAeffeff: 2.61: 2.61 μμmm22
 Low dispersionLow dispersion
achieved byachieved by
compensatingcompensating DDmatmat withwith
DDWGWG
09/24/1309/24/13 R. BouskilaR. Bouskila 88
WaveguideWaveguide
 When they say “wide bandwidth,” theyWhen they say “wide bandwidth,” they
aren’t kidding:aren’t kidding:
09/24/1309/24/13 R. BouskilaR. Bouskila 99
RF spectrum analyzerRF spectrum analyzer
 Regular PSD:Regular PSD:
 RF spectrum:RF spectrum:
 Used to characterize sources andUsed to characterize sources and
components; provides information aboutcomponents; provides information about
distortions and nonidealitiesdistortions and nonidealities
2
( ) ( ) i t
S E t e dtω
ω = ∫
22
( ) ( ) i t
RFS E t e dtω
ω = ∫
09/24/1309/24/13 R. BouskilaR. Bouskila 1010
RF spectrum analyzerRF spectrum analyzer
 Typically done using expensiveTypically done using expensive
electronicselectronics
 All-optical method preferred!All-optical method preferred!
09/24/1309/24/13 R. BouskilaR. Bouskila 1111
RF spectrum analyzerRF spectrum analyzer
09/24/1309/24/13 R. BouskilaR. Bouskila 1212
RF spectrum analyzerRF spectrum analyzer
09/24/1309/24/13 R. BouskilaR. Bouskila 1313
ConclusionConclusion
 Advantages:Advantages:
– Ultrawide bandwidthUltrawide bandwidth
– Record-setting nonlinearityRecord-setting nonlinearity
– Low dispersionLow dispersion
 Limitations:Limitations:
– Material and fabrication costsMaterial and fabrication costs
– Dispersion could be minimized furtherDispersion could be minimized further
09/24/1309/24/13 R. BouskilaR. Bouskila 1414
ReferencesReferences
 [1] M. Pelusi[1] M. Pelusi et al.et al. Photonic-chip-based radio-Photonic-chip-based radio-
frequency spectrum analyser with terahertzfrequency spectrum analyser with terahertz
bandwidth.bandwidth. Nature PhotonicsNature Photonics 33, 139-143 (March, 139-143 (March
2009).2009).
 [2] B. E. A. Saleh & M. C. Teich. Fundamentals[2] B. E. A. Saleh & M. C. Teich. Fundamentals
of Photonics, 2nd ed. Wiley, 2007.of Photonics, 2nd ed. Wiley, 2007.
 [3] G. P. Agrawal. Nonlinear Fibre Optics, 4th[3] G. P. Agrawal. Nonlinear Fibre Optics, 4th
ed. Academic Press, 2006.ed. Academic Press, 2006.
 [4] M. R. E. Lamont[4] M. R. E. Lamont et al.et al. Dispersion engineeringDispersion engineering
of highly nonlinear As2S3 waveguides forof highly nonlinear As2S3 waveguides for
parametric gain and wavelength conversion.parametric gain and wavelength conversion.
Opt. ExpressOpt. Express 1515, 9458–9463 (2007)., 9458–9463 (2007).

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Photonic chip-based RF spectrum analyzer

  • 2. 09/24/1309/24/13 R. BouskilaR. Bouskila 22 OutlineOutline  IntroductionIntroduction  WaveguideWaveguide  RF spectrum analyzerRF spectrum analyzer  ConclusionConclusion
  • 3. 09/24/1309/24/13 R. BouskilaR. Bouskila 33 IntroductionIntroduction
  • 4. 09/24/1309/24/13 R. BouskilaR. Bouskila 44 WaveguideWaveguide  Amount of nonlinearity dependent onAmount of nonlinearity dependent on intensity:intensity:  Fiber core diameter: ~8-10Fiber core diameter: ~8-10 μμmm – Effective area: ~50-80Effective area: ~50-80 μμmm22 2 eff 2 n A π γ λ =
  • 5. 09/24/1309/24/13 R. BouskilaR. Bouskila 55 WaveguideWaveguide  Second problem: DispersionSecond problem: Dispersion – N.B.N.B. DD == DDWGWG ++ DDmatmat
  • 6. 09/24/1309/24/13 R. BouskilaR. Bouskila 66 WaveguideWaveguide  What to do?What to do?  Solution: Ridge (or rib) waveguideSolution: Ridge (or rib) waveguide
  • 7. 09/24/1309/24/13 R. BouskilaR. Bouskila 77 WaveguideWaveguide  High nonlinearityHigh nonlinearity achieved via extremelyachieved via extremely high mode confinementhigh mode confinement – AAeffeff: 2.61: 2.61 μμmm22  Low dispersionLow dispersion achieved byachieved by compensatingcompensating DDmatmat withwith DDWGWG
  • 8. 09/24/1309/24/13 R. BouskilaR. Bouskila 88 WaveguideWaveguide  When they say “wide bandwidth,” theyWhen they say “wide bandwidth,” they aren’t kidding:aren’t kidding:
  • 9. 09/24/1309/24/13 R. BouskilaR. Bouskila 99 RF spectrum analyzerRF spectrum analyzer  Regular PSD:Regular PSD:  RF spectrum:RF spectrum:  Used to characterize sources andUsed to characterize sources and components; provides information aboutcomponents; provides information about distortions and nonidealitiesdistortions and nonidealities 2 ( ) ( ) i t S E t e dtω ω = ∫ 22 ( ) ( ) i t RFS E t e dtω ω = ∫
  • 10. 09/24/1309/24/13 R. BouskilaR. Bouskila 1010 RF spectrum analyzerRF spectrum analyzer  Typically done using expensiveTypically done using expensive electronicselectronics  All-optical method preferred!All-optical method preferred!
  • 11. 09/24/1309/24/13 R. BouskilaR. Bouskila 1111 RF spectrum analyzerRF spectrum analyzer
  • 12. 09/24/1309/24/13 R. BouskilaR. Bouskila 1212 RF spectrum analyzerRF spectrum analyzer
  • 13. 09/24/1309/24/13 R. BouskilaR. Bouskila 1313 ConclusionConclusion  Advantages:Advantages: – Ultrawide bandwidthUltrawide bandwidth – Record-setting nonlinearityRecord-setting nonlinearity – Low dispersionLow dispersion  Limitations:Limitations: – Material and fabrication costsMaterial and fabrication costs – Dispersion could be minimized furtherDispersion could be minimized further
  • 14. 09/24/1309/24/13 R. BouskilaR. Bouskila 1414 ReferencesReferences  [1] M. Pelusi[1] M. Pelusi et al.et al. Photonic-chip-based radio-Photonic-chip-based radio- frequency spectrum analyser with terahertzfrequency spectrum analyser with terahertz bandwidth.bandwidth. Nature PhotonicsNature Photonics 33, 139-143 (March, 139-143 (March 2009).2009).  [2] B. E. A. Saleh & M. C. Teich. Fundamentals[2] B. E. A. Saleh & M. C. Teich. Fundamentals of Photonics, 2nd ed. Wiley, 2007.of Photonics, 2nd ed. Wiley, 2007.  [3] G. P. Agrawal. Nonlinear Fibre Optics, 4th[3] G. P. Agrawal. Nonlinear Fibre Optics, 4th ed. Academic Press, 2006.ed. Academic Press, 2006.  [4] M. R. E. Lamont[4] M. R. E. Lamont et al.et al. Dispersion engineeringDispersion engineering of highly nonlinear As2S3 waveguides forof highly nonlinear As2S3 waveguides for parametric gain and wavelength conversion.parametric gain and wavelength conversion. Opt. ExpressOpt. Express 1515, 9458–9463 (2007)., 9458–9463 (2007).

Editor's Notes

  1. Note Brit spelling of analyzer
  2. 4 um ridge Squares 1530 Circles 1569
  3. time divisions of the multiplexer were deliberately misaligned, causing a time-dependent amplitude modulation
  4. Next, the experimenters tried introducing a variable group velocity dispersion to the signal components by routing them through various lengths of silica fibre. They also (separately) induced a polarization-dependent group delay (differential group delay) by splitting the signal into a TM and a TE mode and applying a separate group delay to each.