optical network components
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OPTICAL NETWORKOPTICAL NETWORK
COMPONENTSCOMPONENTS
: . ,redit Dr V Nagarajan.rofessor in dept of
,CE SSNCE
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Couplers, Splitters, Isolators,Circulators
Filters, Gratings, Multiplexors
Optical Amplifiers, Regenerators
Light Sources, Tunable Lasers,Detectors
Modulators
Overview
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Couplers and FiltersCouplers and Filters
What do they do?Combine wavelengths from many separatefibers into single fiber
Coupler
Separate wavelengths from single fiber tomany separate fibers
Decoupler
Highlights:
Completely passive devicesResponse is not linear across all wavelengthsripple
Some light power is lost wavelengths passthrough filters
Hard & expensive to manufacture demand
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Couplers, SplittersCouplers, Splitters
Coupler Splitter
DWDM System use Coupler + Splitter
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Optical CouplersOptical Couplers
Combines & splits signalsWavelength independent or selectiveFabricated using waveguides in integratedoptics = coupling ratio
Power(Output1) = Power(Input1)Power(Output2) = (1- ) Power(Input1)
Power splitter if =1/2: 3-dB coupler
Tap if close to 1
-selective if depends upon (used in EDFAs)
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CouplersCouplers (contd)(contd)
Light couples from one waveguide to aclosely placed waveguide because thepropagation mode overlaps the twowaveguides
Identical waveguides => complete couplingand back periodically (coupled modetheory)
Conservation of energy constraint:Possible that electric fields at two outputs havesame magnitude, but will be 90 deg out ofphase!
Lossless combining is not possible
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8x88x8 StarStar CouplerCoupler
Power fromall inputs equallysplit amongoutputs
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CouplersCouplers (Contd)(Contd)
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Optical CouplersOptical CouplersMultiplex and demultiplex optical channels into and outof a single fiber
One port for each DWDM channel common port to thefiber plant (outside)
Incorporates:
Monitoring taps for maintenance and troubleshooting
Variable Optical Attenuators (VOA) for received poweradjustment
Expansion ports for upgrades to add more wavelengths to asystemx1x2
.
.
Rx4x5RxN
Rx1x2Rx3
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Tx4x5TxN
Tx3
1 , 2 . . . N
Tx1x2
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Tx1x2TxN
Rx1x2RxN
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Rx1x2RxN
TxN
1 , 2 . . . N
Unidirectionnidirectionall Bidirectionaidirectional
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Example: 16 DWDM CouplerExample: 16 DWDM CouplerArchitectureArchitecture
TxTx
Tx
RxRx
Rx
Tx
Coupler
Tx
and Splitting or Combining Coupler
idirectional AmplifierRxRxRx
TxTx
Tx
xpansion Ports
Coupler
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8-port Splitter Made by Cascading Y-8-port Splitter Made by Cascading Y-CouplersCouplers
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Isolators and CirculatorsIsolators and CirculatorsExtension of coupler concept
Non-reciprocal=> will not work same way ifinputs and outputs reversed
Isolator: allow transmission in one direction, butblock all transmission (eg: reflection) in the other
Circulator: similar to isolator, but with multipleports.
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:ecall Polarization:Polarization Time course of the direction of the electric fiel
vector
, , , -Linear Elliptical Circular Non polar
Polarization plays an important role in the interaction of ligwith matter
Amount of light reflected at the boundary between twomaterials
, ,Light Absorption Scattering Rotation
Refractive index of anisotropic materials depends on( )polarization Brewster s law
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Polarizing FiltersPolarizing Filters
SOP change Done using crystals called dichroics
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Rotating PolarizationsRotating Polarizations
Crystals called Faraday Rotators can rotate thepolarization
without loss!
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ptical Isolator
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Polarization-dependentPolarization-dependentIsolatorsIsolators
Limitation: Requires a particular SOP for input light signal
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o ar za on- n epen en-IsolatorsIsolators
SWP: Spatial Walk-off Polarizer (using birefringent crystals)Splits signal into orthogonally polarized components
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Multiplexers, Filters,Multiplexers, Filters,
GratingsGratings
Wavelength selection technologies
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ApplicationsApplicationsWavelength (band) selection,
Static wavelength crossconnects (WXCs)Equalization of gainFiltering of noise Ideas used in laser operation
Dispersion compensation modules
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Low insertion (input-to-output) loss
Loss independent of SOP:geometry of waveguides
Filter passband independentof temperature
Flat passbands
Sharp skirts on thepassband & crosstalkrejection
Cost: integrated opticwaveguide manufacture
Usually based uponinterference or diffraction
Characteristics of FiltersCharacteristics of Filters
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Device using
interference amongoptical signals fromsame source, but withdiff. relative phaseshifts
(i.e. different pathlengths)
Constructive
interference atwavelength andgrating pitch, a, if
a[sin(i) - sin(d)] =m
m = order of the grating
GratingsGratings
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Transmission vs ReflectionTransmission vs ReflectionGratingGrating
Note: etalon is a device where multipleoptical signals generated by repeatedtraversals of a single cavity
N arrow( )slits txvs narrow
re fle ctio nsurfaces
( )rx M a jo rity o f
d e v ice sa re la tte r( )typ e rx
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Diffraction GratingsDiffraction Gratings
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Grating principles (contd)Grating principles (contd)
Blazing: concentrating the refractedenergies at a different maxima other thanzero-th order
Reflecting slits are inclined at an angle to
the grating plane.
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Periodic perturbation (eg: of RI) written in thepropagation medium
Bragg condition: Energy is coupled from incident toscattered wave if wavelength is
0 = 2 neffwhere is period of grating If incident wave has wavelength 0, this wavelength is
reflected by Bragg grating
Bragg GratingsBragg Gratings
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Bragg Grating PrinciplesBragg Grating Principles
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Bragg Gratings (contd)Bragg Gratings (contd)
Uniform vs apodizedindex profile
Apodized: side lobes cutoff, but width of mainlobe increased
Reflection spectrum isthe F-transform of RI-
distribution
B/w of grating (1 nm)inversely proportionalto grating length (few
mm) Note: Lasers use Bragg
gratings to achieve asingle frequencyoperation
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Fiber GratingsFiber GratingsVery low-cost, low loss, ease of coupling (to
other fibers), polarization insensitivity, lowtemp coeff and simple packaging
Writing Fiber Gratings: Usephotosensitivityof certain types of fibers (eg: Silica
doped with Ge, hit with UV light => RI change) Use a phase mask (diffractive optical element)
Short-period(aka Bragg, 0.5 m) or long-periodgratings (upto a few mm) Short-period (Fiber Bragg): low loss (0.1dB), -accuracy
(0.05nm)
Long-period fiber gratings used in EDFAs to provide gaincompensation
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Fiber Bragg GratingFiber Bragg Grating
OADM El i h F BOADM El t ith F B
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OADM Elements with F-BOADM Elements with F-BGratingsGratings
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Fiber BraggFiber Bragg ChirpedChirpedGratingGrating
(U se d in d isp e rsio n co m p e n sa tio n it)tig h te n s th e p u lse w id th
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Long-period Fiber GratingsLong-period Fiber Gratings
Prin cip le o f o p e ra tio n slig h tly d iffe re n t fro m fib e rBragg
E n e rg y a fte r g ra tin g in te ra ctio n is co u p lin g in to otherfo rw ard p ro p a g a tin g m o d e s in th e cla d d in gin ste a d o f b e in g fu lly re fle cte d a s in Fib e r B ra g g
C la d d in g m o d e s ve ry lo ssy a n d q u icklyattenuated=> Couple energy O U Tof a desired wavelength band