hirookinoshitaa'c'*,tetsuoharadaa'c,masatonakasujia'c ......斑010】z...

4
MicroelectroniCEngineering88(2011)2000-2003 ContentsIistsavaiIabIeatScienceDirect MicroelectronicEngineering FISEVIERjournaIhomepage:www・elsevier,com/Iocate/mee Developmentofcoherentscatterometrymicroscope HirooKinoshitaa'c'*,TetsuoHaradaa'c,MasatoNakasUjia'c,YutakaNagatab,c,TakeoWatanabea,c aUnive応ityQfHyqgo,mbomtolyqfAdwmcedS℃ie"cE〔md泥cfmoIQgWbrIndusny,1-1-2KOutOKtImjgouriAko弓gun,HyOgoP7Ef678-1205,ノロPqn bRike〃2-1HimsawqWtIko,SditqmqP7Ef351-0198,J《Ipan cJSTCREST5-3B(mCho,dliyoda,7bkyOlO2-00方,JnP〔、 ARTICLEINFO ABSTRACT ArtidehiStD1y: Availableonlinel2FebruaIy2011 KEywordS: EUVL DefEctinspection CDmeasurement Mask HighharmoniclasersourEe AnewmaskinspectionsystemfbrEUVLisbeingdeveloped・Theresolutionofpreviouslydevelopedacti- nicinspectionsystems,whichemployIZPorSchwarzschildoptics,islimitedto60nm、Thispromptedus todevelopanewunorthodoxmaskinspectionsystem:alenslessmicroscopeⅧthacoherentlight source・ThissystemcandetectdefEctsonlyafewnanometerswide,anditenablesCDmeasurementswith a3ぴaccuracyofO32nm. ◎2011ElsevierB.V・Allrightsreselved. 1.Intmduction Acriticalissueinextremeultravioletlithography,whichisex- pectedtobeusedfbrtheproductionofsemiconductordevicesat the32-nmnode,isthefabricationofdefect-freemasks・AnEUVL maskconsistsofanabsorberpattemandamultilayeronaglass substrateAMoSimultilayerexhibitsahighreflectivityof70%at theworkingwavelength(13.5,m)ofEUVlithography,According tothelTRSI11,defEctsmustbelessthan20nmwideatthe 32-nmnode・EUVLmaskshavetwotypesofdefects:amplitude defEcts,whichareeitherparticlesononeofthelayersofthe multilayerorflawsinthemultilayer;andphasedefEcts,which arecreatedwhenthemultilayerisdepositedoverabumporpit ontheglasssubstrate・ WehavedevelopedanEUVmicroscopethatemploysSchwarzs- childopticsandanX-rayzoomingtubeI2-8landhaveinstalledit attheNewSUBARUsynchrotronfacility、IthasahighNAofO、3,a magnificationof30×,andalaIgefieldwithadiameterof 1.5mm・TheX-rayzoomingtubehaselectromagneticlenses・It magnifiesapmjectedmaskimagebylO-200×;sothetotalmagni‐ ficationofthemicroscopeis300-6000×・Thissystemenables observationoffinishedmaskpattemslessthanlOOnminsize andpit-typephasedefEctslessthan20nmwide・However,when areflectiveobjectiveisused,thefigureoferrorofthemirrors andthealignmentaccuracyoftheopticsmustbeexceptionally *Correspondingauthorat:UniversityofHyogo,IaboratoryofAdvancedScience andTeChnologyfbrlndustry,1-1-2KoutoKamigouriAko-gun,HyogoPref678- 1205,Japan、泥1.:+81791582546;fax:+81791582504. E-mqiIqddress:kinosita@lasti・u-hyogo、acjp(H、Kinoshita). 0167-9317/$‐seefmntmatter◎2011ElsevierB.V・AllrightsreseIved・ doi:10.10161j,mee,2011.02.060 high・ThismakesitverydifYiculttodesignandfabricatereflective opticswithahighNAfbrEUVlight・ Thus,anewinspectionmethodthatdoesnotemployaconven- tionalobjectiveisbeingdevelopedfbrtheinspectionofEUVL masksfbrthehp-22-nmnode・Itshouldbeabletodetectpattem defectslessthan20nmwideandmeasuretheCDtoanaccuracy oflessthan0.01,m・ThesystemisbasedonX-raydiffraction microscopyandconsistsofacoherent13.5-nmsource,amask andmaskstage,andanEUVcharge-coupled-device(CCD)camera・ ItrequiresnoobjectiveandusesonlycoherentEUVlight・Thelight sourceisahigh-harmonic-generatio、(HHG)beamwithawave‐ lengthof13.5nmproducedbyintensefemtosecondlaserpulses I9,101. 2.Experiments Thecoherentscatterometrymicroscope(CSM)wearedevelop‐ ing(Fig.1)consistsofanHHGEUVsource,amaskstage,anX-ray CCDcamera,andacomputingsystem・Thissystemprovidesaberra- tion-free,diffraction-limitedimagingwithahighNAbyusingthe cameratorecordcoherentEUVlightdiffractedfromamaskI111・ WithanimagingsetupbasedonFraunhofErdiffraction,the objectivecollectsbothphaseandamplitudeinfbrmationfroma sample・Incontrast,theCSMrecordsonlydiffractionintensity; andthustheimagesitproducescontainonlyamplitudeinfbrma- tion・ThemissingphaseinfOrmationisretrievedbyusingahybrid input-output(HIO)algorithm[12-14],whichiterativelycalculates theFouriertransfbrmandtheinverseFouriertransfbrm,subjectto constraints・Thisenablesacompleteimageofasampletobe reconstructed.

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  • MicroelectroniCEngineering88(2011)2000-2003

    ContentsIistsavaiIabIeatScienceDirect

    MicroelectronicEngineering

    FISEVIERjournaIhomepage:www・elsevier,com/Iocate/mee

    Developmentofcoherentscatterometrymicroscope

    HirooKinoshitaa'c'*,TetsuoHaradaa'c,MasatoNakasUjia'c,YutakaNagatab,c,TakeoWatanabea,caUnive応ityQfHyqgo,mbomtolyqfAdwmcedS℃ie"cE〔md泥cfmoIQgWbrIndusny,1-1-2KOutOKtImjgouriAko弓gun,HyOgoP7Ef678-1205,ノロPqnbRike〃2-1HimsawqWtIko,SditqmqP7Ef351-0198,J《Ipan

    cJSTCREST5-3B(mCho,dliyoda,7bkyOlO2-00方,JnP〔、

    ARTICLEINFO ABSTRACT

    ArtidehiStD1y:

    Availableonlinel2FebruaIy2011

    KEywordS:EUVL

    DefEctinspectionCDmeasurement

    Mask

    HighharmoniclasersourEe

    AnewmaskinspectionsystemfbrEUVLisbeingdeveloped・Theresolutionofpreviouslydevelopedacti-nicinspectionsystems,whichemployIZPorSchwarzschildoptics,islimitedto60nm、Thispromptedustodevelopanewunorthodoxmaskinspectionsystem:alenslessmicroscopeⅧthacoherentlightsource・ThissystemcandetectdefEctsonlyafewnanometerswide,anditenablesCDmeasurementswitha3ぴaccuracyofO32nm.

    ◎2011ElsevierB.V・Allrightsreselved.

    1.Intmduction

    Acriticalissueinextremeultravioletlithography,whichisex-

    pectedtobeusedfbrtheproductionofsemiconductordevicesatthe32-nmnode,isthefabricationofdefect-freemasks・AnEUVL

    maskconsistsofanabsorberpattemandamultilayeronaglasssubstrateAMoSimultilayerexhibitsahighreflectivityof70%attheworkingwavelength(13.5,m)ofEUVlithography,AccordingtothelTRSI11,defEctsmustbelessthan20nmwideatthe32-nmnode・EUVLmaskshavetwotypesofdefects:amplitude

    defEcts,whichareeitherparticlesononeofthelayersofthe

    multilayerorflawsinthemultilayer;andphasedefEcts,whicharecreatedwhenthemultilayerisdepositedoverabumporpit

    ontheglasssubstrate・

    WehavedevelopedanEUVmicroscopethatemploysSchwarzs-childopticsandanX-rayzoomingtubeI2-8landhaveinstalleditattheNewSUBARUsynchrotronfacility、IthasahighNAofO、3,amagnificationof30×,andalaIgefieldwithadiameterof1.5mm・TheX-rayzoomingtubehaselectromagneticlenses・ItmagnifiesapmjectedmaskimagebylO-200×;sothetotalmagni‐ficationofthemicroscopeis300-6000×・ThissystemenablesobservationoffinishedmaskpattemslessthanlOOnminsizeandpit-typephasedefEctslessthan20nmwide・However,whenareflectiveobjectiveisused,thefigureoferrorofthemirrorsandthealignmentaccuracyoftheopticsmustbeexceptionally

    *Correspondingauthorat:UniversityofHyogo,IaboratoryofAdvancedScienceandTeChnologyfbrlndustry,1-1-2KoutoKamigouriAko-gun,HyogoPref678-1205,Japan、泥1.:+81791582546;fax:+81791582504.

    E-mqiIqddress:kinosita@lasti・u-hyogo、acjp(H、Kinoshita).

    0167-9317/$‐seefmntmatter◎2011ElsevierB.V・AllrightsreseIved・doi:10.10161j,mee,2011.02.060

    high・ThismakesitverydifYiculttodesignandfabricatereflectiveopticswithahighNAfbrEUVlight・

    Thus,anewinspectionmethodthatdoesnotemployaconven-tionalobjectiveisbeingdevelopedfbrtheinspectionofEUVLmasksfbrthehp-22-nmnode・Itshouldbeabletodetectpattemdefectslessthan20nmwideandmeasuretheCDtoanaccuracy

    oflessthan0.01,m・ThesystemisbasedonX-raydiffraction

    microscopyandconsistsofacoherent13.5-nmsource,amaskandmaskstage,andanEUVcharge-coupled-device(CCD)camera・ItrequiresnoobjectiveandusesonlycoherentEUVlight・Thelightsourceisahigh-harmonic-generatio、(HHG)beamwithawave‐lengthof13.5nmproducedbyintensefemtosecondlaserpulsesI9,101.

    2.Experiments

    Thecoherentscatterometrymicroscope(CSM)wearedevelop‐

    ing(Fig.1)consistsofanHHGEUVsource,amaskstage,anX-rayCCDcamera,andacomputingsystem・Thissystemprovidesaberra-tion-free,diffraction-limitedimagingwithahighNAbyusingthe

    cameratorecordcoherentEUVlightdiffractedfromamaskI111・

    WithanimagingsetupbasedonFraunhofErdiffraction,theobjectivecollectsbothphaseandamplitudeinfbrmationfromasample・Incontrast,theCSMrecordsonlydiffractionintensity;andthustheimagesitproducescontainonlyamplitudeinfbrma-tion・ThemissingphaseinfOrmationisretrievedbyusingahybridinput-output(HIO)algorithm[12-14],whichiterativelycalculatestheFouriertransfbrmandtheinverseFouriertransfbrm,subjectto

    constraints・Thisenablesacompleteimageofasampletobereconstructed.

  • H・KinosI1itqetqI./MicroeIec"OnicE唾neemlg88(20刀ノ2000-2003 2001

    蕊議慰

    CSM

    Coherent

    Source(13.5-nmHHG)

    PinhoIe

    X-rayCCD

    CompLIting

    systenlGasceIlfbrionization

    I monochromatizesthebeam・ThepinholeprovidesaspatialcoherencelargeenoughfbrobservationswiththeCSMNext,a

    concavesphericalmirrorreflectsthebeam(incidentangle:3。)

    "

    /=雲琴雲凋 LMonochromatoI。

    6025XYStage

    Vacu而而1泊illber

    59-orderEUVIight

    Fig、1.Comgurationofcoherentscatterometrymlcroscope.

    Twoorfburcopiesofthesamepattemareusuallymadeonamask、Amaskinspectionsystemcomparestwoofthemtodeter-mlnewhetherornottheycontainanydefEcts、

    WithFraunhoferdiffraction,thediffractionimageofarepeatedpattemisdeterminedbythepitchofthepattem・Forthisreason,thepattemwidthisestimatedfromtheratiooftheintensitiesof

    theOth-orderand±1st宮orderdiffractedlight、Thecriticaldimension(CD)requiresanaccuracyoflessthan

    26nmfbrthe32-nmnode[11.Toachievethatlevelofaccuracy,itisnecessarytobeabletoprecise1ydeterminethelinewidthofamaskpattem、Thus,at-wavelengthobservationwithanEUVmicroscopeisessentialfbrestimatingtheactinicCDoftherenec-tionprofile.

    3.Resultsanddiscussion

    ToexaminethefEasibiliwofdefEctinspectionandCDmeasure-mentwiththeCSM,theCSMwasinstalledontheBL-3Cbeamline

    oftheNewSUBARUsynchrotronfacility,whichhasabending-mag-netsource

    Figs、2and3showaschematicandaphotograph,respectively,oftheCSMattheendstationoftheBL-3CTheopticalpathintheCSMchamberbeginswitha5-mm-diameterpinholeanda200-nm-thickZrfilter,whichreducesthebeamdiameterandpartially

    Fig.3.PhotographofCSM.

    hp88nm

    Fig、4.DetectionimageofundersizedefEct.

    CSMCCDImage

    L1s1orderl.刈ぴhorderl |÷1割order|

    一汐

    300hm

    Back-

    iIIuminated

    CCDcameraPinhoIc

    ,/Undersizedefect

    弘総識鰯

    鯖#

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    畷鶴三$,醤…,

    灘 鵜TaN

    (BIight)瀞蒔軍1

    賎I;,

    Fig2・SchematicdiagramofCSMinNewSUBARU.

  • 斑010】Z H・Km0shimemI./MicToeIEctmnicEngiI1ee(、988(20刀ノ2000-2003

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    1

    AcoherentscatterometrymicroscopeisbeingdevelopedfbrthedefEctinspectionandCDmeasurementof22-nm-nodeEUVmasks、

    AnundersizedefEctinaline-and‐spacepattemwasclearlyob-served;andtheCDofaperiodicL&Spattemwasaccuratelymea-sured・The3ぴCDaccuracyisO、32,m,whichsatisfIesthelTRS

    specificationsfbrthehp-22-nmnode・Furthermore,a13.5-nm

    HHGsourcebasedonacommercial30-fSlasersystem(SpectraPhysics)hasalreadybeenbuilt,ExperlmentalresultsobtainedwiththissourcewillbereportedinthenearfUture

    FL

    宝峰陥r‐h』が仇

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    ‘陽、,‘瀞 *脇西暫f

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    (a)SEMimage (b)CSMimage

    Fig、5.Exampleofreconstructedimageof28-nm-nodebitlinemaskpattem.

    andElplanarmirrorreflectsit(incidentangle:39。)ontoanEUV

    maskThetwomirrorsarecoatedwith40pairsofMoSilayers,whichhaveElpeakreflectiviwof43%at入=13.4,mand52%at

    ノl=13.5,m.TheZrfilterandthethreeMoSimultilayersofthebranchingmirrorandthetwomirrorsoftheCSMmonochromatize

    thewhitelight,yieldingalargetemporalcoherence、Fig.4showsdefEctinspectionresultsfbranundersizedefect

    (width:30,m)inanhp-88-nmline-and-spacepattemonamask:

    (a)CSMCCDimage(diffTactionpattern)and(b)CD-SEMimage・Inthediffractionpattem,thiswpeofdefEctappearsasalmeperpen-diculartotheL8zSpattem・

    Fig.5showsdefEctinspectionresultsfbranhp-112-nmbitlinemaSkpattemobtainedwith(a)anSEMand(b)theCSM、TheHIO

    algorithmfaithfilllyreconstructsthepattem・Fromthisimage,thedefEctresolutionwasestimatedtobelessthan30nm・

    WhentheCSMisusedtoestimatetheCD,theresultsaccuratelyrenecttheshadowmgoftheabsorberpattembecausetheangleofincidencefbranEUVmaskis6o,whichisthesameasthatfbrtwo

    alphaEUVexposuretools,theADT(ASML)andtheEUV1(Nikon).

    Fig.6showsresultsfbrCDmeasurementsofamaskfbrthehp-32-nmnodethatwasfabricatedattheUniversiwofHyogo・Thewidthofspacesvariesfroml28tol80nm・Thesevaluesinclude

    theeffEctsofthevariationinilluminationintensityduringthemeasurements・Aftercompensationfbrthisvariatio、,theresults

    arelinear,Acomparisonofvaluesfbrthehorizontalandvertical

    directionsrevealedanalmostl8-nmdiffErenceduetoShadowing・Thisagreeswellwiththetheoreticalvaluefbranabsorberthick-nessof70nm・

    Fig.7showsrecentresultsobtainedwith13.5-nmHHGpro=ducedusiI1g30-fSlaserpulsesfromacommerciall-kHzTi:sap-phirelasersystem(SpectraPhysics)withalasingwavelengthof800nmandanoutputpowerof6W・Theresultsarebetterthan

    anticipated,TheaverageintensityofthesourceislOOOtimeshigh-erthanthatoftheBL-3beamline.

    170

    160

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    120130140150160170180190200

    C医SEMSpaceWidth(nm)

    Fig.6.CDmeasurementresultsfbrCSMandCD-SEM.

    ;砥

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    59th(13.5nm)

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    50000

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    ChanneI

    IntensityProfile

    Fig、7.HHGintensiwspectrum.

  • HKnloShimetqL/MiCmeIectmniCEnginee而ng88a011)2000-2003 2003

    References

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