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MILLIMETER-WAVE DIGITALLYINTENSIVE FREQUENCY GENERATION INCMOS

MILLIMETER-WAVE DIGITALLYINTENSIVE FREQUENCY GENERATION INCMOS

WANGHUAWU

ROBERTBOGDANSTASZEWSKI

JOHNR.LONG

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PREFACE

Overthepastfewdecades,frequencysynthesisbasedonanalog-intensive phase-lockedloops(PLLs)hasbeenthemostpopulartechnique employedtoprovidelocaloscillatorsignalsfortheradiofrontend.With aggressivescalingandtechnologicaladvancementinsilicon-basedprocess technologies,particularlyCMOS,digitallyassistedRFsystemsarefast becomingacommonplaceinthelow-GHzbands(i.e.,below10GHz). Thekeyenablerthereisdigitalsignalprocessingemployedtoimprove theoverallsystemperformanceviacalibration,andalsotoprovidereconfigurabilityandeaseoftestability.ParticularlyintheareaofRF frequencysynthesis,manyuniversities,researchinstitutes,andcompanies havesincedemonstratedvariousall-digitalphase-lockedloop(ADPLL) implementations,andADPLLsarenowreplacingtraditionalanalogPLLs inconsumerelectronicssupportingvariouswirelessstandards,for example,2G/3Gcellular,IEEE802.11a/b/g/n/ac,andBluetooth.

Asthefrequencyspectrumbecomesincreasinglycongestedinthe low-GHzregime,millimeter-wave(mm-wave)frequencybands(i.e., above30GHz)aregainingpopularityastheyofferlargebandwidthto supportGiga-bitpersecondwirele sscommunicationwithouttheneed forcomplexmodulationschemes,thusachievinglowerrorrates andlowenergyconsumptionperbit.Uptothisdate,therehavebeen manypublishedsilicon-basedmm-waveanalogPLLs,butveryfew ADPLLsoperatingabove30GHzarere ported.Littlematerialhasbeen writtenontheADPLLdesignchallengesatmm-wavefrequencies andthedesigntechniquestoaddressthem.Moreover,testingand debuggingPLLstocorrectlyidentifyanydesignorfabricationproblems wouldbeequallychallengingdue totheclosed-loopoperationof thePLL.

Inthisbook,wedetailthesetechnicalchallenges,anddiscussthe designandimplementationofa60-GHzADPLLinaconventional widelyavailableCMOSprocess.Wefurtherelaborateoncalibration techniquesthatareespeciallyusefulatmm-wavetoimprovethesystem performance.Wealsoexplaintheimplementedtestabilityfeaturesthat

facilitatedesignfortestandcharacterization.Thisbookisorganizedas follows:

Chapters1 3goovertheintroductionandreviewofexistingliterature.Chapter1laysoutthemotivationandchallengesinbuildingan ADPLLforthemm-waveregime,whileChapter2presentsvarious existingmm-wavefrequencysynthesizerarchitectures.Chapter3 reviewsthebuildingblocksofafrequencysynthesizer,whichare commontobothanaloganddigitalimplementations.

Chapters4 6dealwiththetheory,design,andrealizationofammwaveADPLL.Chapter4coversthebasicconceptswhichareneeded tounderstandthedesignandoperationofanADPLL,andChapter5 discussesmm-wavedigitallycontrolledoscillator(DCO)designsand implementations.Chapter6addressesthedesignsofotherkeycircuit blocks,anddemonstratesa60-GHzADPLLforuseinanFMCW transmitter.

Chapter7explainsseveralcalibrationtechniquesusedtoimprovethe performanceofthe60-GHzADPLL,whileChapter8describesthe measurementchallengesofamm-wavefrequencysynthesizer,and proposesbuild-inself-testandself-characterizationtechniques. Theworkpresentedinthisbookisaculminationofseveralyears ofresearch.Wewouldliketothankandacknowledgethediscussions andhelpwereceivedfrompastandpresentcolleaguesattheDepartment ofElectronicsofDelftUniversityofTechnologyinTheNetherlands. WealsothankthestaffatElsevierfortheirsupport.

WanghuaWu

RobertBogdanStaszewski

JohnR.Long April2015

LISTOFABBREVIATIONS

ADC Analog-to-digitalconverter

ADPLL All-digitalphase-lockedloop

AM Amplitudemodulation

BiCMOS BipolarandCMOS

BISC Built-inself-characterization

BIST Build-inself-test

CB Coarse-tuningbank

CKM Modulationclock

CKR Referenceclockretimedbyoscillatorclock

CKV Oscillator(variable)outputclock

CLK Clock

CML Current-mode-logic

CMOS Complementarymetal-oxide-semiconductor

CT Center-tap

DAC Digital-to-analogconverter

DCO Digitallycontrolledoscillator

DDFS Directdigitalfrequencysynthesizer

DFC Designforcharacterization

DFT Designfortest

DNL Differentialnonlinearity

DSP Digitalsignalprocessing

EM Electromagnetic

ESD Electrostaticdischarge

EVM Errorvectormagnitude

FB Fine-tuningbank

FCC FederalCommunicationsCommission

FCW Frequencycommandword

FET Field-effecttransistor

FM Frequencymodulation

FMCW Frequency-modulatedcontinuous-wave

FREF Frequencyreference

Gb/s Gigabitpersecond

GRO Gatedringoscillator

GSM Globalsystemformobile(communications)

GUI Graphicaluserinterface

HVAC Heating,ventilating,andairconditioning

IC Integratedcircuit

IEEE InstituteofElectricalandElectronicsEngineers

IF Intermediatefrequency

IIR Infiniteimpulseresponse

ILFD Injection-lockedfrequencydivider

INL Integralnonlinearity

IO Input/output

IR Interconnectresistance

ISM Industrial,scientificandmedical

LF Loopfilter

LMS Leastmeansquares

LO Localoscillator

LPF Low-passfilter

LSB Leastsignificantbit

MB Mid-coarsetuningbank

MIM Metal-insulator-metal

MIMO Multiple-inputandmultiple-output

mm-wave Millimeter-wave

MoM Metal-oxide-metal

MOS Metal-oxide-semiconductor

MTBF Meantimebetweenfailures

nDCO NormalizedDCO

NMOS N-typemetal-oxide-semiconductor

NTW Normalizedtuningword

OTW Oscillatortuningword

PA Poweramplifier

PCB Printedcircuitboard

PFD Phase/frequencydetector

PHE Phaseerror

PHR Phaseoffrequencyreference

PHV Phaseofvariableoscillator

PI Proportional-integral

PLL Phase-lockedloop

PM Phasemodulation

PMOS P-typemetal-oxide-semiconductor

PN Phasenoise

PPF Poly-phasefilter

PROM Programmableread-onlymemory

PVT Process,voltageandtemperature

QAM Quadratureamplitudemodulation

Q-factor Qualityfactor

Rx Receiver

RF Radiofrequency

RFIC Radiofrequencyintegratedcircuit

rms Root-mean-square

RO Ringoscillator

SAFF Sense-amplifier-basedflip-flop

SiGe SiliconGermanium

SoC System-on-chip

SPI Serialperipheralinterface

SRAM Staticrandom-accessmemory

TDC Time-to-digitalconverter

TL Transmissionline

TR Tuningrange

TSPC Truesingle-phaseclocked

Tx Transmitter

UWB Ultra-wideband

VCO Voltage-controlledoscillator

WiGig WirelessGigabitAlliance

WiMAX WorldwideInteroperabilityforMicrowaveAccess

WLAN Wirelesslocal-areanetwork

WPAN Wirelesspersonal-areanetwork

CHAPTER1 Introduction

Contents

1.1 Motivation2

1.1.1 AdvantagesofMillimeter-WaveRadios2

1.1.2 Deep-SubmicronCMOS5

1.1.3 DigitallyIntensiveApproach7

1.2 DesignChallenges9

1.2.1 TowardAll-DigitalPLLinmm-WaveRegime9

1.2.2 WideTuningRangeandFineFrequencyResolution11

1.2.3 LinearWidebandFM12 References13

WirelesscommunicationhasevolvedremarkablysinceGuglielmoMarconi demonstratedthetransmissionandreceptionofMorse-codedmessages acrosstheAtlanticOceanintheearlytwentiethcentury.Sincethen,new wirelesscommunicationmethodsandserviceshavebeencontinuously adoptedthatrevolutionizeourlives.Today,cellular,mobile,andwireless local-areanetworks(WLANs),affordedbybreakthroughsinsemiconductor technologiesandtheircapabilityofmassproduction,areinuseworldwide. Theyenableustoshareimagesofourcherishedmomentswithfamilyand friendsanywhere,andatanytime.Thecurrenttrendstoward portablewirelessdeviceswithultra-high-speed(e.g.,gigabitpersecond) connectivitywillsoonallowustogoonlineviaournotebooks,cell phones,andtablets,simultaneouslyemailing,chattingwithfriends,web browsinganddownloadingmoviesandmusicinafractionofthetimeit takestoday.Thesedeviceswillhavetomeetaggressiveperformance specificationsinasufficientlysmallandlow-costproductatlowpower dissipation.Thishaspromptedfranticresearchintonewradiofrequency (RF)-integratedcircuits,systemarchitectures,anddesignapproaches. Thisbookexploresthefeasibility,advantages,design,andtestingof digitallyintensivefrequencysynthesisinthemillimeter-wave(mm-wave) frequencyrange.Anall-digitalphase-lockedloop(ADPLL)-basedtransmitter

demonstratorfabricatedinaproductionbulkCMOSprocessisdescribed, whichoperatesinthe60-GHzband,andachievesfractionalfrequency generationandwidebandfrequencymodulation(FM).Thisdigitally intensivedesignhasthepotentialforlowcostinvolumeproduction.It isalsoamenabletoscalinginfuturetechnologynodesasopposedto otheranalog-intensiveimplementations.Thesiliconareaandpower consumptionofsuchtransmittersmaybereducedfurtherinfutureby harnessingthepowerofdigitalsignalprocessing(DSP).

1.1MOTIVATION

Toachievegigabitpersecond(i.e.,Gb/s)transferrates,Wi-Fitechnology (IEEE802.11acinthe5-GHzband) [1] hasbeendevelopedinrecent years.MultistationWLANthroughputofatleast1Gb/s,andasinglelink throughputofatleast500Mb/sisspecified.ItemploysRFbandwidthsof upto160MHz,multiple-inputandmultiple-output(MIMO)array transmitter/receiverstreams(upto8),multi-userMIMO,andupto 256-QAM(quadratureamplitudemodulation)schemesinordertoachieve thatlevelofperformance.Themm-wavefrequencybands,bycontrast,are lesscrowdedthanthelow-gigahertzradiocommunicationbandsand,more attractively,havewiderlicense-freeRFbandwidthavailable(e.g.,7GHz bandwidthinthe60-GHzband).Thiswillenablethegigabit-per-second short-rangecommunicationforconsumermultimediaproductsandsupport thedevelopmentofemergingshort-rangewirelessnetworkinginmany importantareas,forexample,commerce,manufacturing,transport,etc., andthusprovidesignificantgrowthpotentialinnewinternetapplications inprice-sensitivecommunicationmarkets.

Inthefollowingsections,theadvantagesandchallengesofmm-wave transceiverdesigninCMOStechnologywillbeexamined.Thefocusis onmm-wavefrequencysynthesis.

1.1.1AdvantagesofMillimeter-WaveRadios

Themm-wavefrequencybandisdefinedas30 300GHzwithawavelengthbetween1and10mmintheair [2].Therearevariousaspectsof mm-wavebandsthatmakeitattractiveforshort-rangeapplications.One majoradvantageisthebandwidthavailabletocarryinformation.Tokeep operatingcostslow,regulatorylicensedbandsshouldbeavoided,thus callingfortheexploitationoftheunlicensedortheindustrial,scientific, andmedical(ISM)radiobands. Figure1.1 plotstheavailablebandwidth 2

Figure1.1 BandwidthallocationfortheISMandunlicensedbandsbelow100GHz bytheFCC(intheUnitedStates) [3].

(indicatedinGHzatthetopofeachcolumn)forISMandunlicensed bandsbelow100GHzintheUnitedStates [3].Below25GHz,theRF spectrumiscongestedduetofrequencyslotsreservedformilitary,civil, andpersonalcommunicationservices.Forreference,mostcommercial productsoperateinbandsbelow10GHz,forexample,theglobalsystem formobilecommunicationsoperatesat900and1,800MHz(inEurope), and850and1,900MHz(intheUnitedStates),andultra-wideband (UWB)radiosarepermittedtooperatefrom3.1to10.6GHz [4].Less than1GHzofbandwidthintotalhasbeenallocatedforthelicense-free ISMbandsat2.45,5.8,and24GHz.Onthecontrary,thereis7GHzof bandwidthinthe60-GHzspectrumbandallocatedforlicense-freeuse, whichisthelargesteverallocatedbytheFederalCommunications Commission(FCC)intheUnitedStatesbelow100GHz.Withsuchwide bandwidthavailable,mm-wavewirelesslinkscanachievecapacitiesashigh as7Gb/sfullduplex,whichisunlikelytobematchedbyanyoftheRF wirelesstechnologiesatlowerfrequencies.TheFCChasalsorecently approvedanotherunlicensedband(92 95GHz)tomeetthegrowing demandforpoint-to-pointhigh-bandwidthcommunicationlinks [5]

Foragivenantennasize,thebeamwidthcanbemadefinerbyincreasing thefrequency.Anotherbenefitofthemm-waveradioisanarrowerbeam duetotheshorterwavelength(λ 5 c/fc ,where c isthespeedoflightand fc isthecarrierfrequency),whichallowsfordeploymentofmultiple, independentlinksincloseproximity.Themainlimitationofmm-wave radioisthephysicalrange.Duetoabsorptionbyatmosphericoxygenand

Figure1.2 Averageatmosphericattenuationofradiowavespropagatingthrough freespaceversusfrequency [6]

watervapor,signalstrengthdropsoffrapidlywithdistancecomparedto otherbands. Figure1.2 illustratesthegeneraltrendofincreasingthe attenuationofradiowaveswithfrequency(dueonlytoatmosphericlosses; freespacepathlossisnotaccountedfor) [6].Atmosphericabsorptionby oxygencausesmorethan15dB/kmofattenuation.Thelossofalink budgetat60GHzisthereforeunacceptableforlong-distancecommunication(e.g., . 1km),butcanbeusedtoanadvantageinshort-rangeindoor communicationsbecausethelimitedrangeandnarrowbeamwidthsprevent interferencebetweenneighboringlinks.Theseattributeshaveledtogreatly reducedregulatoryburdensformm-wavecommunications.

Duetoitspotentialforshort-range,gigabit-per-secondcommunications, severalstandardsinthe60-GHzbandhavebeenestablishedinrecent years.TheIEEE802.15.3cstandardwasapprovedin2009forwireless personal-areanetwork [7].AsimilarstandardforEurope(ECMA-387 [8]) waspublishedin2008.TheWirelessHDconsortiumhasreleasedaspecificationversion1.0aforregulatingthetransmissionofhigh-definitionvideoin thisunlicensedband [9].Mostrecently,theIEEE802.11adstandard(known asWiGig) [10] wasadoptedin2013.Itprovidesdataratesupto7Gb/s,or morethan10 3 themaximumspeedpreviouslysupportedbytheIEEE 802.11standard.IEEE802.11adalsoaddsa“fastsessiontransfer”feature,

whichenableswirelessdevicestoseamlesslytransitionbetweenthe60-GHz frequencybandandlegacybandsat2.4and5GHzinordertooptimizelink performanceandrangecriteria.

Inadditiontothegigabit-per-secondcommunication,the60-GHz unlicensedbandalsoholdspromiseforintegratingwirelesssensors. Frequency-modulatedcontinuous-wave(FMCW)radarsmaybeutilized forpresencedetectionandrangingat60-GHzapplications,where high-frequencyresolutionisrequired [11].Thisisalsotheintended applicationfortherealizedADPLLfrequencysynthesizerthatisfully describedinthisbook.AsanexampleofsuchFMCWapplicationisa gesturerecognitionsystemforcars,wherethedrivergestures(e.g., noddingthehead)withouttakingtheeyesofftheroadwheninterfacing withapplicationssuchasnavigation,phone,HVAC(heating,ventilating, andairconditioning)controls,etc.Thetargeteddetectionrangeis from0.3to10mandtherangeresolutionisbelow5cm.Alow-cost implementationofshort-rangeradarsystemswillenablenumerous applicationsinsecurity,searchandrescue,imaging,logistics,quality control,tonamejustafew.

Figure1.3 illustratestheoperatingprincipleofanFMCWradar transceiver.Thecarriersignalismodulatedasshownin Figure1.3b, resultinginasignalwhoseinstantaneousfrequencyvarieslinearlywith time,i.e.,alinearchirp [12].Thislinearchirpistransmittedtowarda target,andthereceivedechoisconvolvedwithaportionofthetransmittedsignaltodeterminetheround-trippropagationtime, τ .InanFMCW radar,theachievablerangeresolution(Δr)isdeterminedby

where c isthespeedoflight,andBW(Figure1.3b)isthemodulation rangeofthetransmitsignal [12].Whenthefull7GHzofbandwidthat 60GHzisutilized,arangeresolutionasfineas2cmcanbeachieved.

1.1.2Deep-SubmicronCMOS

Silicontechnologies(e.g.,CMOSandSiGe-BiCMOS)aremainstreamintegratedcircuit(IC)processesdrivenlargelybymassproductionofICsusedin digitalcomputers(e.g.,desktopsandnotebooks)andotherelectronicdevices (e.g.,cellphones,gameconsoles,andtablets).Thedemandforahigherintegrationlevelandlowercostinvolumeproductionhasdrivenmm-wave electronicsdevelopmentinsiliconCMOStechnology.With65-nmbulk

Figure1.3 (a)SimplifiedblockdiagramofanFMCWradartransceiver;(b)transmittedandreceivedlinearFMCWsignal.

CMOStechnologiesinproductionofferingpeaktransitfrequency(fT)and maximumfrequencyofoscillation(fmax)closeto200GHz(simulatedusing baselinetransistors) [13],severalexperimental60-GHztransceivershave beenreportedthatachievedataratesabove4Gb/sacrossa2-mlink [14 16].TheseprototypesdemonstratethepotentialtouseCMOSfor RF/basebandco-integration,andrevealthedesignchallengesandopportunitiesforimprovedRFperformance(e.g.,higherRFoutputpower,lower oscillatorphasenoise(PN),etc.)andlowerpowerconsumption. Nevertheless,III-Vprocessesstillhaveanicheinpoweramplifiersand antennaswitchesformobilephones/basestations,andultra-high-frequency, high-powerelectronicsformilitaryandspaceapplications.

Abetterunderstandingofthepropertiesofdeep-submicronCMOS technologiesiscrucialinordertoimplementhigh-performance mm-waveICs.Severalkeypropertiesaresummarizedhere,whichshould betakenintoaccountwhendecidingonthepreferredarchitecturesand designapproaches.

•Lowsupplyvoltage:comparedtoIII-Vandbipolartechnology,which relyonalargersupplyvoltage(3.3and2.5V),deep-submicron CMOSfeaturesanominalsupplyvoltageof B1V.

•Duetotheaforementionedlowsupplyvoltageofdeep-submicron CMOSandrelativelyhighthresholdvoltage(0.5Vandoftenhigher, duetothebodyeffect),theavailablevoltageheadroomisquitesmall. Thus,themarginbetweentechnologyperformanceanddesign requirementsappearslargerinthetimedomainthaninthevoltage domain [17]

•ExcellentswitchingcharacteristicsofMOStransistors—bothrise andfalltimesareontheorderoftensofpicosecondsorlessfor deep-submicronCMOStechnologies.

•Rapidpaceofprocessscaling—eachnewdigitalCMOSprocessnode occursroughlyevery18months,resultinginanincreaseinthedigital gatedensitybyafactorof2(knownasMoore’slaw [18]).

•Multiplemetallayersarecommonlyavailableforinterconnectioninlargescaledigitalcircuitry,whichalsoprovidehigh-densitymetal-oxide-metal capacitors.

1.1.3DigitallyIntensiveApproach

Duetotheaforementionedpropertiesofdeep-submicronCMOS technologies,especiallythestrengthincircuitspeedanddensity,digitally assistedanddigitallyintensiveRFsystemsarebecomingattractivefor mm-wavetransceiverICs.WhenthedesignedRFsystememploysdigital logicandsignalprocessingextensivelytoobtainbetterRFperformance, itiscalled digitallyintensive.Comparedto analog-intensive architectures,the numberofpurelyanalogcircuitfunctionsinadigitallyintensive mm-wavetransceiverisreduced,whichresultsinadvantagesthat conventionaldigitaldesignflowshaveoveranalogdesignmethodologies. Amongthemare:reduceddesigncycletimesusingautomateddigital implementationtoolsandflow,easeoftestabilityviabuilt-inselftest, on-chipDSP,high-densitymemory,andautomaticfunctionaltesting withgoodfaultcoverage.Moreover,digitallyintensivearchitectureshave lowersensitivitytoprocess/deviceparametervariabilitycomparedtothe analogintensivesystems.Inaddition,digitalcircuitsprovidereconfigurabilitytocontroltheoperationmodeandimprovesystemperformance viapowerfulon-chipcalibrationtechniques,whichmayreducesilicon areaandpowerdissipationoftheSoC.

Notethatthe“digitallyintensive”termdoesn’timplythatanalog/RF designtechniquesarenotimportant.Onthecontrary,theyareascrucial asbefore.Theoverallsystemperformanceisusuallydominatedbyafew keyanalogcircuitblocks.Theessenceofthedigitallyintensiveapproach istomaketheinputs/outputs(IOs)oftheRF/analogbuildingblocks digitalsothatthesystemcanbemodeledandanalyzedusingthedigital designflow,withitsmanyadvantagesfordesignthroughputandyield. Consequently,itrequiresRF/analogdesignerstobeconversantwith digitalcircuitsandsystemdesign,toanalyzethesystemfrombothanalog anddigitalperspectives,andtocollaboratewithdigitaldesigners.

AgoodexampleofadigitallyintensivearchitectureisADPLL synthesizershownin Figure1.4.Itcontainsadigitallycontrolledoscillator, whichmayoscillateinthegigahertzrangeandiscontrolledbyadigital oscillatortuningword(OTW).ThegigahertzDCOoutput(usually followedbyaninvert-basedbuffer)hassharprising/fallingedgeswhen implementedindeep-submicronCMOStechnologieswith fT above 100GHz,thusbehavinglikeadigitalclock.Thetime-to-digitalconverter (TDC)measuresandquantizesthetimedifferencebetweenthereference andDCOclocktransitionedges.Thenthedigitizedphaseerrorisfiltered byadigitalloopfilter(LF)andeventuallyconvertedtotheOTWinorder totunetheoscillatortothedesiredfrequency.AlthoughtheDCOand TDCarebothanaloginnature,allbuildingblocksintheADPLLare definedasdigitalattheI/Olevel,andthereforetheloopcontrolcircuitry isimplementedinafullydigitalmanner,asillustratedin Figure1.4.

ThisADPLLarchitecturehasbeenusedinmassproductionfor RFconnectivityand2G/3Gmobilecommunications [17].Withthe improvedRFcapabilityof65-nmCMOStechnology,digitallyintensive frequencysynthesiscouldbeexploredinthemm-waverange,which isover10 3 thepreviouslyprovenfrequencyrange.Suchmm-wave

Figure1.4 SimplifiedblockdiagramofanADPLL.

ADPLLincreasesthereconfigurabilityoffrequencygenerationina mm-wavetransceiver.Moreover,FMcanbeincorporatedtheretoforma digitaltransmitterwiththepotentialforsuperiormodulationqualityand lowercostinmassproduction.

1.2DESIGNCHALLENGES

Torealizelow-cost,yethigh-performancemm-wavetransceiversinCMOS technology,newconceptsinICimplementationsforultra-widebandsignal generationandmm-wavefront-endsarenecessary.Thisbookfocuseson frequencysynthesis,whichiscriticaltomanymoderncommunication systems.Duetothehighoperatingfrequency,finefrequencyresolution,and widebandlinearFMrequirements,afullyintegratedmm-wavefrequency synthesizerhasvariousdesignchallengesthatarediscussedinthefollowing sections.

1.2.1TowardAll-DigitalPLLinmm-WaveRegime

Beforethisvery60-GHzall-digitalphase-lockedloop(PLL)thatwillbe elaboratedinthisbook,therehadbeennootherreportedsuccessful fractional-Nsynthesizerimplementationsabove10GHzforwireless applicationsthatwouldemployanall-digitalapproach.Therewere, however,tworeportsofdigitalPLLsynthesizers [19,20] operatingat20 and40GHz,respectively,usedforhigh-speedserialwirelineapplications, andnumeroussuccessfulADPLLdemonstratorsoperatingbelow10GHz forvariouswirelessapplications,forexample,bluetooth,cellular,WLAN, WiMAX,etc. [21 24].Forlow-gigahertzapplications,anLCoscillator isnormallyusedtosatisfystringentPNrequirements,inwhichthe tuningoftheoscillationfrequencyisachievedviadigitalcontrolofan arrayofMOSvaractorsthatoperateinflatregionsoftheir C V curve.It iswell-knownthatthePNofanLCoscillatorintheupconverted thermalnoiseor 1/f 2 regime(i.e.,outsidetheloopbandwidthofaPLL synthesizer)isinverselyproportionaltothesquareofthetankquality factor Q [25].Thetank Q-factorbelow10GHzisdominatedbythe Q-factoroftheinductor,whilethevaractor Q-factorisnormallymuch higher(e.g., B100at2GHz)ina65-nmCMOStechnology.

However,thisisoppositetothesituationatmm-wavefrequencies. Figure1.5 plotsthe Q-factorandcapacitance(Cv)versusbiasvoltagefor n 1 /n-wellandp 1 /p-wellaccumulationmodevaractorsina65-nm CMOStechnologyatminimumgatelength [26]. Q-factorvarieswith

Figure1.5 Capacitanceand Q-factorat60GHzversusgatevoltageforminimum length,thin-oxideaccumulationmodevaractors(65-nmCMOS) [26]

bias(duetochanging Cv)andisapproximately20or5intheflatregions. Whiletheinductor Q-factor(QL)increaseswithincreasingfrequency, the Q-factorofcapacitorsandvaractors(QC)isinverselyproportionalto frequency.Therefore, Q ofthetankcapacitance(varactorplusparasitics) becomestheprimaryfactorlimitingthequalityoftunableon-chip resonators,andthePNperformanceofmm-waveoscillators.Power consumptionoftheoscillatormustthereforebeincreasedinorderto maintainsignalswingandcompensateforgreaterlossesintheLCtank.

Inaddition,afrequencydividerchainisnecessarytobringthecarrier frequencydowntoafewGHzforfurtherprocessingbythedigitalphase detector.Therearestrongtrade-offsbetweenpower,chiparea(inductors), maximumoperatingfrequency,andoperatingrangeinthedividerchain design,whichnormallydissipatesmorethan50%ofthetotalpowerina mm-waveanalogPLL [27].Moreover,thedivider’soperatingrangeshould bealignedwiththeDCOfrequencytuningrangeinthepresenceof process,voltage,andtemperature(PVT)variations.Thedividerchain introducesextradelayintheloopandmayaffectthestabilityofthePLL. Allthesebringextrachallengestothedesignofmm-waveADPLLs.

AlthoughthedigitallyintensivenatureoftheADPLLpermitsthefast system-levelsimulationandverificationbyanevent-drivensimulator,the transistorsizingandphysicallayoutofthekey“analog-nature”building blocks,suchasDCO,dividerchain,andTDChavetobe“handcrafted” accordingtothedesignspecifications,andthenmodeledatthebehavioral levelfortheclosed-loopsimulations.Comparedtodesignforlow-GHz

applications,theinterconnectionsbetweenmm-wavefrequencybuilding blocksaffectsthesystemperformanceduetoparasiticcapacitance,losses, andunwantedcapacitiveandmagneticcouplingeffects.Therefore,intensiveelectromagneticsimulationisalsorequiredforasuccessfulADPLL designinthemm-waveregime.

1.2.2WideTuningRangeandFineFrequencyResolution

Asmentionedearlier,onemajorbenefitofthe60-GHzbandisthe7-GHz worthofunlicensedbandwidth.Whenthe7-GHzbandwidthisfully employed,the60-GHzFMCWradar,asshownin Figure1.3,cantheoreticallyachievearangeresolutionasfineas2cm.SincePVTvariationsmust beaccommodatedbythetuningrangeoftheoscillator,awiderthan9-GHz tuningrangeisdesiredtoensurefullcoverageoftheentire60-GHzband. However,atuningrangelessthan5%istypicallyexpectedforanLC voltage-controlledoscillator(VCO)operatingatthesefrequencies [26]

Thetank Q-factorandfractionaltuningbandwidthfortanks optimizedateachfrequencyareplottedin Figure1.6 (schematicshown inset),usingsimulationsinthesame65-nmRF-CMOStechnologyas Figure1.5[26].Inordertoconstructthetuningrangecurve,wefirst

Figure1.6 Optimumtank Q-factorandfractionaltuningrangeforresonatorsin 65-nmRF-CMOSfromsimulation(basedonsimulationswith Cfixed 5 20fF) [26]

selectaninductorthathasthehighestpeak Q-factorwhendriven differentiallyateachfrequency(f0).Thefixedandvariablevaractor capacitances(Cfixed 5 20fFandn 1 /n-wellthickoxidevaractorwith L 5 0.4 μm)arethenaddedtosettheresonanceat f0.Thefixedportion ofthetankcapacitance(Cfixed)accountsforwiringinterconnectsand transistorparasitics.Forexample,thetunablecapacitance ΔC willbe 21fFofthe70.4-fFtotaltankcapacitance(C0),ifa100-pHtank inductor(L0)resonantat60GHzisassumed.Itcanbeseenthatthe oscillatortuningrangedropsto B5%athigherfrequencies.Tuningrange maybeimprovedbysacrificingthetank Q-factor,i.e.,usingsmaller inductorvaluesandlargervaractors.However,thepowerconsumptionof theoscillatororthesizeofcoretransistorneedtobeincreasedforPN performance,which,inthelattercase,canintroducemore Cfixed,thus limitingtheachievabletuningrangebythistradeoff.

Inadditiontotheaforementioneddifficultiesinachievingawide tuningrangeforamm-waveLCoscillator,itisalsochallengingtorealize finefrequencytuningunderdigitalcontrol.Amm-waveDCOisthe heartofamm-waveADPLL.Itprovidesthemeanstoconvertdigital controlwordsintooutputfrequencies.Thelackofahigh-resolution DCOhashinderedtheADPLLfromreachingmm-wavefrequenciesin thepast.Theminimum-sizedNMOSvaractorina65-nmCMOS processgeneratesa ΔC of B40aF,whichresultsinafrequency resolutionof B17MHzfora60-GHzcarrier(i.e.,

,assuming

analysisinRef. [17],thiscorrespondstoaquantizationnoise of 62.2dBc/Hzat1-MHzoffset(referenceclockis40MHz),whichis 28dBhigherthanthenaturalPNofa60-GHzDCO(e.g., 90dBc/Hz at1-MHzoffset).Moreover,minimum-sizeddevicesdonottracklarger deviceswell,resultinginamismatcheffectinsidethetuningbankarray. Therefore,newdigitalfine-tuningtechniquesneedtobedevelopedfor mm-waveDCOstoachievearawfrequencyresolutionontheorderof 1MHz. ΣΔ ditheringoftheleastsignificantbitsintheDCOtuning bankcanbeemployedtoimprovethefrequencyresolutionfurther [17]

1.2.3LinearWidebandFM

Tomaximallyexploittheavailablebandwidth(e.g.,7GHzinthe 60-GHzband)allocatedatmm-wavefrequenciesforhighdatarate communicationsandhigh-precisionradars,mm-wavetransceiversshould

providelinearwidebandFMcapability.Forexample,ina60-GHz FMCWradartransceivershownin Figure1.3,thefrequencyofthe transmitsignalislinearlyrampingupanddownacross5-GHzrange. Theradarrangeresolutionisdeterminedby Eq.(1.1) anddegradeswith thesweepnonlinearity [12].However,inpractice,theDCOtuningmust besegmentedintocoarse-andfine-tuningbanks,eachwithdifferent tuningstep, KDCO (definedasfrequencychangeperbit)torealizehigh resolutionandawidetuningrangesimultaneously.Consequently,the widebandtriangularmodulation,asshownin Figure1.3a hastotraverse throughvarioustuningbanksandrelyonlinearized KDCO acrossmultiple banks.Moreover,thetuningstepmismatchesinsideeachbankalso introducenonlinearitiesintheFM.Dummystructurescanbeaddedin thephysicallayouttoimprovethematchingperformancebuttheymay notbepossibleatmm-wavefrequenciesduetotheincreasedparasitics andreducedoveralltuningrange.Alternatively,digitalcalibrationand compensationtechniquesshouldbedevelopedandappliedtoimplement thewidebandtriangularmodulation.Inaddition,sincethe Q-factorof thetankalsovariesfrom20to5acrossthemodulationrange (Figure1.5),theoutputswingoftheoscillatormayvarybymorethan 3dB.Theoutputbuffermustcompensateforthesignalpowerfluctuation acrossthemodulationrangeandproduceachirpwithaflatoutputpower (e.g., 6 dB)attheFMCWtransmitteroutput.

Toaddresstheaforementionedconcernsandissuesforhighperformancefrequencysynthesisatmm-wavefrequencies,somenew circuitsandsystemarchitecturesarrangementshavetobediscovered.In thisbook,alternativedesignapproachesandarchitectureformm-wave PLLsareexplored.Weusea60-GHzall-digitalPLLforFMCWradar applicationasadesignexample.ThePLLarchitecture,mm-wavecircuit design,andtheDSPtechniquesdevelopedinthisparticularworkcanbe universallyappliedtoothermm-waveapplicationsthatfocusonhigh performanceandlowcost.

REFERENCES

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[4]FederalCommunicationsCommission.Revisionofpart15ofthecommission’s rulesregardingultra-widebandtransmissionsystems,April22,2002[online]. Available: , http://transition.fcc.gov/Bureaus/Engineering_Technology/Orders/ 2002/fcc02048.pdf .

[5]InternationalTechnologyRoadmapforSemiconductors.Radiofrequencyand analog/mixed-signaltechnologiesforwirelesscommunications,2009[online]. Available: , http://www.itrs.net/Links/2009ITRS/2009Chapters_2009Tables/ 2009_Wireless.pdf .

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[10]IEEE802.11ad.Part11:wirelessLANmediumaccesscontrol(MAC)andphysical layer(PHY)specificationsamendment3:enhancementsforveryhighthroughputin the60GHzband,2012.

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[14] A.Tomkins,R.A.Aroca,T.Yamamoto,S.T.Nicolson,Y.Doi,S.P.Voinigescu,A zero-IF60GHz65nmCMOStransceiverwithdirectBPSKmodulation demonstratingupto6Gb/sdataratesovera2mwirelesslink,IEEEJ.Solid-State Circuits44(8)(2009)2085 2099.

[15] K.Okada,N.Li,K.Matsushita,K.Bunsen,R.Murakami,A.Musa,etal.,A 60-GHz16QAM/8PSK/QPSK/BPSKdirect-conversiontransceiverfor IEEE802.15.3c,IEEEJ.Solid-StateCircuits46(12)(2011)2988 3004.

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high-speedserialcommunicationapplications,in:IEEEInternationalSolid-State CircuitsConferenceDigestofTechnicalPapers,February2009,pp.94 95,95a.

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[24] G.Marzin,S.Levantino,C.Samori,A.L.Lacaita,A20Mb/sphasemodulatorbased ona3.6GHzdigitalPLLwith 36dBEVMat5mWpower,IEEEJ.Solid-State Circuits47(12)(2012)2974 2988.

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CHAPTER2

Millimeter-WaveFrequency Synthesizers

Contents

2.1 FrequencySynthesizerFundamentals17

2.1.1 PNinOscillators18

2.1.2 FrequencySynthesizerinaRadioTransceiver20

2.1.3 MethodsforFrequencySynthesis21

2.2 Phase-LockedLoop23

2.2.1 Charge-PumpPLL24

2.2.2 All-DigitalPLL26

2.3 Millimeter-WavePLLArchitectures28

2.3.1 PLLwithaFundamentalOscillator28

2.3.2 PLL-BasedHarmonicGeneration29

2.4 Summary32 References33

2.1FREQUENCYSYNTHESIZERFUNDAMENTALS

Alocaloscillator(LO)isrequiredinhigh-performanceradiotransceiversirrespectiveofthearchitecture.ItisemployedtotranslatetheRF signaldowntoanintermediatefrequencyorbasebandinreceivers, andviceversaintransmitters.TheLOhastobetunableacrosstheRF bandandthefrequencyresolutionhastobeatleastequaltothe channelspacing.AfrequencysynthesizeristypicallyusedastheLOin RFtransceiverstoovercomethedriftsinoscillatorfrequencydueto temperaturevariations.ThesynthesizerprovidesastableRFcarrier withhighspectralpurity,ideallyacrossawidefrequencyspan. RFfrequencysynthesizersremainoneofthemostchallengingblocks inmanywirelesssystems(e.g.,mobilecommunications).Thechoiceof frequencysynthesisapproachdependsonfactorssuchasphasenoise (PN),permissiblespuriousoutputlevels,switchingrate,frequency resolution,cost,andcomplexity.

2.1.1PNinOscillators

AnidealLOoperatingatangularfrequency ω c ,producesasinusoidal outputversustimeoftheform yðt Þ 5 AUcosðω c t 1 ϕÞ,where A isthe amplitudeand ϕ isanarbitraryandfixedphase.Thezero-crossingsoccur atintegermultiplesoftheperiod, Tc 5 2π=ω c .Inthefrequencydomain, allofitspowerisconcentratedatasinglefrequency, ω c ,asshownin Figure2.1a.However,noisesourcesinsidepracticaloscillatorcircuits (e.g.,fromtransistors)perturbthezerocrossingsrandomly.Therefore, boththeamplitudeandphasevaryrandomlywithtime.Inmostcases, thechangeinamplitudeisremovedbyalimitingbuffercircuit,and thereforeonlytherandomdeviationofthephasemustbeconsidered:

where ϕn ðt Þ isasmall,randomphasequantitythatcausesthezerocrossingstodeviatefromintegermultiplesof Tc .Consequently,theoscillator frequencyspectrumspreadsaround ω c (Figure2.1b).Thephasefunction ϕn ðt Þ inthetimedomainisobservedasspectralspreadinginthe frequencydomainandiscalledPN [1]

PNofRFoscillatorsisnormallycharacterizedinthefrequency domain.Forasmallvalueofthephasefluctuation, jϕn ðt Þj{1radian, Eq.(2.1) canbesimplifiedto

whichmeansthatthespectrumof ϕn ðt Þ isfrequency-translatedto 6 ω c . Thus,thedecliningskirtsin Figure2.1b areduetothephasefluctuation ϕn ðt Þ

Figure2.1 Outputspectrumof(a)idealand(b)practicaloscillators.

ThisPNcanbequantifiedbyconsideringa1-Hzbandwidthatanoffset Δω fromthecarrier,calculatingthenoisepower,anddividingthatresult bythecarrierpower [2].

L ðΔω Þ 5 10log10 noisepowerina1-Hzbandwidthat ω c 1 Δω carrierpower : (2.3)

Thisisthesingle-sidedspectralnoisedensity,usuallyexpressedin decibels,withrespecttothecarrierperhertzbandwidth(i.e.,dBc/Hz). Thesingle-sidedPNof Eq.(2.3) isone-halfofthePNspectrum,which containsbothupper-andlower-frequencycomponents( ω c 6 Δω ).

Inpractice,thePNreachesaconstantflooratlargefrequencyoffsets (e.g., Δω largerthanafewtensofmegahertzinatypicalRFoscillator). Theregionnearthecarrieriscalled“close-in”PNandtheregionfar fromthecarrieriscalled“far-out”PN,althoughtheborderbetween thetwoisvague.Inthisbook,“far-out”PNreferstooffsetsgreater than20MHzfromthecarrier.

Figure2.2 showsaPNspectrumofatypicaloscillator.Inthis log-logplot,thePNindBc/Hzisplottedagainsttheoffset Δω from thecarrierfrequency ω c .ThePNprofiletraversesthrough1=ω 3 ,1=ω 2 , and1=ω 0 sloperegions.Theregion1=ω 2 isgenerallyreferredtoasthe thermalnoiseregionbecauseitiscausedbywhiteoruncorrelated timingfluctuationsintheperiodofoscillation.The1/ f flickernoiseof electronicdevicesisalsosubstantialforloweroffsetfrequencies.Itgets up-convertedandcreatesthe1=ω 3 region.Finally,the1=ω 0 regionis typicallydominatedbythethermalnoiseaddedoutsidetheoscillator proper,suchasinanoutputbuffer.

Inaddition,anundesired,systematicfluctuationintheoscillatorPN givesrisetoaspurioustone.Thiscanbesimplyexplainedbyconsidering

Figure2.2 PNspectrumofatypicaloscillator.

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