optoelectronics circuits systems lab ocdma optical source development april 16, 2005 jason chou,...

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Optoelectronics Circuits & Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California, Los Angeles

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Optoelectronics Circuits & Systems Lab SC-enhanced Mode Locked Source MLL EDFA DS Fiber Requires only a few longitudinal modes from the mode locked laser Simplifies design Extend the spectrum to create a broad comb of frequencies of multi-THz bandwidth by super-broadening Decouples the laser design from the spectrum requirement of OCDMA Filter

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Page 1: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

OCDMA Optical Source Development

April 16, 2005Jason Chou, Ozdal Boyraz, and Bahram Jalali

University of California, Los Angeles

Page 2: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

Goal Conventional supercontinuum source

produces broadband spectrum, where only small portion is used

Goal is to create spectrum only where it is needed

Approaches:• Broadband comb generations • Asymmetric comb generation

Page 3: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

SC-enhanced Mode Locked Source

MLL

EDFADS Fiber

• Requires only a few longitudinal modes from the mode locked laser• Simplifies design

• Extend the spectrum to create a broad comb of frequencies of multi-THz bandwidth by super-broadening• Decouples the laser design from the spectrum requirement of OCDMA

Filter

Page 4: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

Broadband Spectral Comb Generation

MLLaser

Line SelectionFilter

EDFA

p p p

DS Fiber

•Desired lines are selected from MLL spectrum•Act as seed for generating desired spectral lines•Generation achieved using SPM and FWM in nonlinear media

Page 5: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

Asymmetric Broadband Spectral Comb Generation

SeedPulse AWG

EDFA DS Fibers

DSF1 DSF3DSF2

p p p

•Spectrum location is optimized using dispersion slope engineering

Page 6: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

Numerical SimulationStarting Spectrum After FWM in single mode fiber

Optical Frequency

Asymmetry

•Asymmetry in spectrum can be induced through dispersion slope•Effect is modest in standard single mode fiber•Can be drastic in dispersion engineered media

Optical Frequency

Page 7: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

Experimental Demonstration

•Independent control of channel separation and total bandwidth•Power is concentrated in discrete OCDMA channels •>25nm bandwidth•Promising approach

-40

-30

-20

-10

0

10

20

30

40

1525 1530 1535 1540 1545 1550 1555 1560 1565 1570 1575

Wavelength [nm]

Pow

er [d

Bm

/nm

]

Output Spectrum

InputSeed

PC

=1300nm =1490nm =1561nm

BPF

MLL EDFA

Modulator

Input RF Signal

Chirped Optical Pulse

DispersionWav

elen

gth

Time

Optical BW

Stretched RF Signal

PDSCSource

Dispersion

Fiber L1 Fiber L2

1500 1520 1540 1560 1580 1600 1620-30

-25

-20

-15

-10

Ampl

itude

(a.u

.)

Wavelength (nm)

PC

=1300nm =1490nm =1561nm

BPF

MLL EDFA

PC

=1300nm =1490nm =1561nm

BPF

MLL EDFA

Modulator

Input RF Signal

Chirped Optical Pulse

DispersionWav

elen

gth

Time

Optical BW

Stretched RF Signal

PDSCSource

Dispersion

Fiber L1 Fiber L2

1500 1520 1540 1560 1580 1600 1620-30

-25

-20

-15

-10

Ampl

itude

(a.u

.)

Wavelength (nm)

1500 1520 1540 1560 1580 1600 1620-30

-25

-20

-15

-10

Ampl

itude

(a.u

.)

Wavelength (nm)

Conventional SupercontinuumGeneration

Page 8: Optoelectronics Circuits  Systems Lab OCDMA Optical Source Development April 16, 2005 Jason Chou, Ozdal Boyraz, and Bahram Jalali University of California,

Optoelectronics Circuits & Systems Lab

Next Steps Dispersion engineering will be investigated by cascading

fibers with dispersion tailored profiles to improve efficiency and flatten channel profile.

Dynamic range per channel is limited by ASE-FWM beating effect which can be mitigated by adding narrowband optical filters to suppress EDFA noise background.

Alternative approach to improve FWM efficiency and reduce noise is to filter and overlap MLL pulses before passing through dispersion engineered fibers.