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FiberOpticNetworkDesignX.Wu,M.Y.Li,H.M.YanDept.ofOpt.Engr.,ZJU2011Class6
OpticalAmplificationEDFAStructureParametersSelectionGainflatteningExerciseAnopticalamplifierisadevicewhichamplifiestheopticalsignaldirectlywithouteverchangingittoelectricity.Thelightitselfisamplified.
Reasonstousetheopticalamplifiers:
ReliabilityFlexibilityWavelengthDivisionMultiplexing(WDM)LowCostVarietyofopticalamplifiertypesexists,including:SemiconductorOpticalAmplifiers(SOAs)ErbiumDopedFiberAmplifiers(EDFAs)TraditionalOpticalCommunicationSystemLosscompensation:Repeatersatevery20-50kmOptically
AmplifiedSystemsEDFA=ErbiumDopedFiberAmplifierVarietyofopticalamplifiertypesexist,including:SemiconductoropticalamplifiersOpticalfibreamplifiers(ErbiumDopedFibreAmplifiers)Distributedfibreamplifiers(RamanAmplifiers)OpticalfibreamplifiersarenowthemostcommontypeOneofthemostsuccessfulopticalprocessingfunctionsAlsousedasabuildingblockinDWDMsystemsSource:Master7_5OpticalAmplificationErbiumdopedfiberamplifiersAmplifierapplicationsIssues:GainflatteningandNoiseOverviewBasicEDFAmplifierDesignErbium-dopedfiberamplifier(EDFA)mostcommonCommerciallyavailablesincetheearly1990’sWorksbestintherange1530to1565nmGainupto30dB(1000photonsoutperphotonin!)
Opticallytransparent“Unlimited”RFbandwidthWavelengthtransparentInput1480or980nmPumpLaserErbiumDopedFiberOutputIsolatorCouplerPumpSourceWDMErbiumDopedFibreIsolatorIsolator
=FusionSpliceInputOutputApumpopticalsignalisaddedtoaninputsignalbyaWDMcouplerWithinalengthofdopedfiberpartofthepumpenergyistransferredtotheinputsignalbystimulatedemissionForoperation~1550nmthefiberdopantisErbiumPumpwavelengthiseither980nmor1480nm,pumppower~50mWGainsof30-40dBpossibleErbiumDopedFiberAmplifierFibreinput/outputErbiumdopedfibreloopPumplaserWDMFibrecouplerSource:Master7_5InteriorofanErbiumDopedFibreAmplfier(EDFA)PumpSourceWDMErbiumDopedFibreIsolatorIsolator
=FusionSpliceInputOutput980nmsignal1550nmdatasignalPowerlevel980nmsignal1550nmdatasignalPowerlevelPowerinterchangebetweenpumpanddatasignalsOperationofanEDFAPhysicsofanEDFAErbium:rareelementwithphosphorescentpropertiesPhotonsat1480or980nmactivate
electronsintoametastablestateElectronsfallingbackemitlightin
the1550nmrange
SpontaneousemissionOccursrandomly(timeconstant~1ms)StimulatedemissionByelectromagneticwaveEmittedwavelength&phaseare
identicaltoincidentoneErbiumProperties1480980820540670GroundstateMetastablestateErbiumDopedFibreAmplifiersFiberlength:typicallytenmetresorsoDoping:asmallcontrolledamountoftherareearthelementerbiumaddedtotheglassintheformofanion(Er3+).LDpower:between10and200mW
WavelengthsLightateither980or1,480nm.)
Question#1:Whynotincreasedopinglevelanddecreaselength?Question#2:What’stheadvantageofpumping1480nm?Er+3EnergyLevelsPump:980or1480nmPumppower>5mWEmission:1.52-1.57mLonglivingupperstate(10ms)Gain30dBEDFAOperationA(relatively)high-poweredbeamoflightismixedwiththeinputsignalusingawavelengthselectivecoupler.Themixedlightisguidedintoasectionoffiberwitherbiumionsincludedinthecore.Thishigh-poweredlightbeamexcitestheerbiumionstotheirhigher-energystate.Whenthephotonsbelongingtothesignal(atadifferentwavelengthfromthepumplight)meettheexcitederbiumatoms,theerbiumatomsgiveupsomeoftheirenergytothesignalandreturntotheirlower-energystate.Asignificantpointisthattheerbiumgivesupitsenergyintheformofadditionalphotonswhichareexactlyinthesamephaseanddirectionasthesignalbeingamplified.Thereisusuallyanisolatorplacedattheoutputtopreventreflectionsreturningfromtheattachedfiber.Suchreflectionsdisruptamplifieroperationandintheextremecasecancausetheamplifiertobecomealaser!TechnicalCharacteristicsofEDFAEDFAshaveanumberof
attractivetechnical
characteristics:EfficientpumpingMinimalpolarisationsensitivityLowinsertionlossHighoutputpower(thisisnotgainbutrawamountofpossibleoutputpower)LownoiseVeryhighsensitivityLowdistortionandminimalinterchannelcrosstalkAmplifiedSpontaneousEmissionAmplifiedspontaneousemission(ASE)Randomspontaneousemission(SE)AmplificationalongfiberErbiumrandomlyemitsphotonsbetween1520and1570nmSpontaneousemission(SE)isnotpolarizedorcoherentLikeanyphoton,SEstimulatesemissionofotherphotonsWithnoinputsignal,eventuallyallopticalenergyisconsumedintoamplifiedspontaneousemissionInputsignal(s)consumemetastableelectronsmuchlessASEGainversusAmplifierlengthGainversuspumplevelNoiseSourcesEDFAEDFAhasrevolutionizedopticalcommunicationsAllopticalandfibercompatibleWidebandwidth,20~70nmHighgain,20~40dBHighoutputpower,>200mWBitrate,modulationformat,powerandwavelengthinsensitiveLowdistortionandlownoise(NF<5dB)PumpSource980nmlowASE,lownoiseamplifier1480nmhigherpowerpumplaserhighoutputpowernotasefficientdegreeofpopulationinversionislowerEDFABehaviouratGainSaturationTherearetwomaindifferencesbetweenthebehaviourofelectronicamplifiersandof
EDFAsingainsaturation:1)
As
inputpowerisincreasedontheEDFAthetotalgainoftheamplifierincreasesslowly.Anelectronicamplifieroperatesrelativelylinearlyuntilits
gainsaturatesandthenitjustproducesallitcan.Thismeansthatan
electronicamplifieroperatednearsaturationintroducessignificantdistortions
intothesignal(itjustclipsthepeaksoff).2)Anerbiumamplifieratsaturationsimplyapplieslessgaintoallofitsinput
regardlessoftheinstantaneoussignallevel.Thusitdoesnotdistortthesignal.
ThereislittleornocrosstalkbetweenWDMchannelseveninsaturation.
Totaloutputpower:Amplifiedsignal+Noise(AmplifiedSpontaneousEmissionASE)EDFAisinsaturationifalmostallErbiumionsareconsumedforamplificationTotaloutputpowerremainsalmostconstant,regardlessofinputpowerchanges
Pin(dBm)TotalPout-3dBMax-20-30-10GainSaturationinEDFAsGainCompressionTotaloutputpower:
Amplifiedsignal+ASEEDFAisinsaturationifalmostallErbiumionsareconsumedforamplificationTotaloutputpowerremainsalmostconstantLowestnoisefigure
Preferredoperatingpoint
PowerlevelsinlinkstabilizeautomaticallyPin(dBm)TotalPout-3dBMax-20-30-10GainAmplifierLengthAsthesignaltravelsalongthelengthoftheamplifieritbecomesstrongerdueto
amplification.Asthepumppowertravelsthroughtheamplifieritsleveldecreases
duetoabsorption.Thus,boththesignalpowerlevelandthepumppowerlevel
varyalongthelengthoftheamplifier.Atanypointwecanhaveonlyafinite
numberoferbiumionsandthereforewecanonlyachieveafinitegain(andafinite
maximumpower)perunitlengthoftheamplifier.
Fiberlength=F(signalpower,pumppower,Erconcentration,gainrequired)Inanamplifierdesignedformultiwavelengthoperationthereisanotherconsideration-theflatnessofthegaincurveovertherangeofamplified
wavelengths.Withacarefuldesignandoptimisationoftheamplifier'slengthwecanproduceanearlyflatamplifiergaincurve.OpticalGain(G)G=SOutput/SInput
SOutput:outputsignal(withoutnoisefromamplifier)
SInput: inputsignal
InputsignaldependentOperatingpoint(saturation)of
EDFAstronglydependson
powerandwavelengthof
incomingsignalWavelength(nm)Gain(dB)154015601580101520204030-5dBm-20dBm-10dBmPInput:-30dBmSeveralattractivefeaturesfornetworkuse:RelativelysimpleconstructionReliable,duetothenumberofpassivecomponentsAllowseasyconnectiontoexternalfibersBroadbandoperation>20nmBitratetransparentIdeallysuitedtolongspansystemsIntegralpartofDWDMsystemsUnderseaapplicationsforOFAsarenowcommonOFAsintheNetworkIn-lineAmplifierPowerAmplifierPreamplifierFibreLinkTransmitterTransmitterTransmitterOpticalAmplifiersOpticalAmplifierFibreLinkOpticalAmplifierFibreLinkOpticalReceiverOpticalReceiverOpticalReceiverOpticalAmplifierApplicationsAmplifierApplicationsPreamplifiersverylowalownoisecharacteristicisessentialonlyamoderategainfigureTypicallyapreamplifierwillnothavefeedbackcontrolasitcanberunwellbelowsaturation.PoweramplifiersMostDFBlasersoutput:2mW,Afiber:aggregatepowerlevelsofupto100to200mWbeforenonlineareffectsstarttooccur.TypicalEDFApoweramplifiershaveanoutputofaround100mWLineamplifiersReplacesarepeaterwithinalong
communicationlinehighgainattheinputandhighpoweroutputaverylownoisefigure.Thisisreallyapreamplifiercascaded
withapoweramplifier.Sophisticatedlineamplifierstodaytendtobemade
justthisway-asamulti-sectionamplifierseparatedbyanisolator.EDFACategoriesIn-lineamplifiersInstalledevery30to70kmalongalinkGoodnoisefigure,mediumoutputpowerPowerboostersUpto+17dBmpower,amplifiestransmitteroutputAlsousedincableTVsystemsbeforeastarcouplerPre-amplifiersLownoiseamplifierinfrontofreceiverRemotelypumpedElectronicfreeextendinglinksupto200kmandmore
(oftenfoundinsubmarineapplications)RXPumpTXPumpBestusedforsinglechannelsystemsinthe1550nmregion,Systemsaredesignedforuseasboosters,in-lineamplifiersorpreamplifiers.BandwidthisnotwideenoughforDWDM,specialEDFAneededExample:ConventionalEDFASource:Master7_5Gainflatnessisnowwithin1dBfrom1530-1560nmITU-TDWDMCbandis1530to1567nmGainFlattenedEDFAforDWDMTypeGainMaximumOutputpowerNoisefigurePowerAmplifierHighgainHighoutputpowerNotveryimportantIn-lineMediumgainMediumoutputpowerGoodnoisefigurePreamplifierLowgainLowoutputpowerLowvalue<5dBessentialSelectingAmplifiersPumpingDirectionsAdditionalpumpingoptionsMultistageEDFAsSomenewEDFAdesignsconcatenatetwooreventhreeamplifierstages.An
amplifier“stage”isconsideredtoconsistofanyunbrokensectionoferbiumdoped
fibre.Multistageamplifiersarebuiltforanumberofreasons:1.Toincreasethepoweroutputwhileretaininglownoise2.Toflattenthetotalamplifiergainresponse3.Toreduceamplifiedstimulatedemissionnoise
Two-StageEDFALineAmplifierwithSharedPump.Pumppowerwould
typicallybesplitinaratiodifferentfrom50:50.CommercialDesignsInputEDFOutputIsolatorTelemetry&RemoteControlPumpLasersOutputMonitorEDFInputMonitorIsolatorSecurity/SafetyFeaturesInputpowermonitorTurningontheinputsignalcancausehighoutputpowerspikesthatcandamagetheamplifierorfollowingsystemsControlelectronicsturnthepumplaser(s)downiftheinputsignalstaysbelowagiventhresholdformorethanabout2to20μs
BackreflectionmonitorOpenconnectorattheoutputcanbealasersafetyhazardStraightconnectorstypicallyreflect4%ofthelightbackBackreflectionmonitorshutstheamplifierdownifbackreflectedlightexceedscertainlimitsOutputSpectraASEspectrumwhennoinputsignalispresentAmplifiedsignalspectrum(inputsignalsaturatestheopticalamplifier)1575nm-40dBm1525nm+10dBmErbiumcanprovideabout40-50nmofbandwidth,from1520to1570nmGainspectrumdependsontheglassused,eg.silicaorzblanglassGainspectrumisnotflat,significantgainvariationsWavelength(nm)
152015301540155015603020100Gain(dB)EDFAgainspectrumEDFAGainSpectrumGainCharacteristicsofEDFAGain(amplifier)-istheratioindecibelsofinputpowertooutputpower.Gain
at1560nmissome3dBhigherthangainat1540nm(thisistwiceasmuch).In
mostapplications(ifthereisonlyasinglechannelorifthereareonlyafew
amplifiersinthecircuit)thisisnottoomuchofalimitation.WDM
systemsusemanywavelengthswithintheamplifiedband.Ifwehaveaverylong
WDMlinkwithmanyamplifiers
thedifferenceinresponseinvariouschannelsaddsup.FlatteningoftheGainCurveTechniquesOperatingthedeviceat77°K->amuchflattergain,notallthatpractical.Introducingotherdopantmaterials(suchasaluminiumorytterbium)alongwith
theerbiumintothefibrecore.Amplifierlengthisanotherfactorinfluencingtheflatnessofthegaincurve.Controllingthepumppower(throughafeedbackloop)isroutinetoreduceamplifiedspontaneousemission.AddinganextraWDMchannellocallyattheamplifier(“gainclamping”).Manipulatingtheshapeofthefiberwaveguidewithintheamplifier.Atthesystemslevelthereareotherthingsthatcanbedonetocompensate:Using“blazed”fiberBragggratingsasfilterstoreducethepeaksinthe
responsecurve.TotransmitdifferentWDMchannelsatdifferentpowerlevelstocompensatefor
lateramplifiergaincharacteristics.GainFlatteningConceptUsedtoreducevariationinamplifiergainwithwavelength,usedinDWDMsystemsThegainequalisationisrealisedbyinsertingtaperedlongperiodgratingswithintheerbiumdopedfibre.DesignedtohaveapproximatelytheoppositespectralresponsetothatofanEDFAInlineDicongainflatteningfilterInlineDicongainflatteningfilterspectralresponseGainFlatteningFilters(Equalizers)SpectralHoleBurning(SHB)GaindepressionaroundsaturatingsignalStrongsignalsreduceaverageionpopulationHolewidth3to10nmHoledepth0.1to0.4dB1530nmregionmoresensitive
toSHBthan1550nmregion
ImplicationsUsuallynotanissueintransmission
systems(singlelorDWDM)Canaffectaccuracyofsome
lightwavemeasurements1545155015601540Wavelength(nm)7nm0.36dBPolarizationHoleBurning(PHB)PolarizationDependentGain(PDG)Gainofsmallsignalpolarizedorthogonaltosaturatingsignal0.05to0.3dBgreaterthanthelargesignalgainEffectindependentofthestateofpolarizationofthelargesignalPDGrecoverytimeconstantrelativelyslow
ASEpoweraccumulationASEpowerisminimallypolarizedASEperpendiculartosignalexperienceshighergainPHBeffectscanbereducedeffectivelybyquicklyscramblingthestateofpolarization(SOP)ofthein
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