hirookinoshitaa'c'*,tetsuoharadaa'c,masatonakasujia'c ......斑010】z...
TRANSCRIPT
-
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。)
①
"
/=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.
図
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#
CD-SEMimage(“↓1m)MC/Si
畷鶴三$,醤…,
灘 鵜TaN
(BIight)瀞蒔軍1
賎I;,
鴬
Fig2・SchematicdiagramofCSMinNewSUBARU.
-
斑010】Z H・Km0shimemI./MicToeIEctmnicEngiI1ee(、988(20刀ノ2000-2003
E砿
iO1
1101010101
Ⅱ
蝿マ
1KI、!亀
rr碑偶喜晒,油畦い一篭l凸qも
.&ひろP‐
‐哨・弔鞠縄剛蜘、1瀧呼侭献霧獅#掴懇・用j聞匡〃頭■Mjr刊口勧曹P
‐盤換Ⅸ薄爵綱蕊“↓画
l‐
■l‐.
’艮割・jP.I鴇織創綱
時諦独’
30画F‐P、!
‐邸内Fも
心
録罰〆
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
瞬此IBJI可。翠里酌llp工むけ
斗鰯IF
ii;i;NF
Ⅸ
。
,ij
W
l.
旨‘L
lf
]j堤W望
11
rl
I』2
浬
ヨL
4.ComlIwgion
』諺
画、F低’
」
F1
罫零便 謬寺 r
l#
L
11.誰
蝿典Np劉裂趣
硯
J
j,、
#】填恩錘 #無爵#W
蕊’鳴 甘,ー 士&錘
‘陽、,‘瀞 *脇西暫f
『
F可 垂
(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
30000
20000
画、
ロ■
口画
/〆:息0000
5432
1111
(E匡)ロ○の即⑯E]
H■画面
⑥
40000
$〆.国
■歴BeforecompensatioI1
■H盛V
Aftercompensation夕
身〆。|‐HoVl②。⑨
⑨
110
120130140150160170180190200
C医SEMSpaceWidth(nm)
Fig.6.CDmeasurementresultsfbrCSMandCD-SEM.
;砥
HHGspectlum
Dlvergence
59th(13.5nm)
Wをlvelength
50000
I’
3.5104
31o4
2.5104
2104
1.51o4
1104
5000
0
160240320400480560640
ChanneI
IntensityProfile
Fig、7.HHGintensiwspectrum.
-
HKnloShimetqL/MiCmeIectmniCEnginee而ng88a011)2000-2003 2003
References
I11SemiconductorlndustIyAssociation,International淀chnologyRoadmapfbrSemiconductorsLithography,IntemationalSEMATECH,Austin,TX,2007.
I21H・Kinoshita,T、Haga,KHamamoto,S・mkada,N・Kazui,S・Kakunai,H,Tsubakino,T、Shoki,MEndo,T・Watanabe,J・Vac、Sci・Technol.B22(2004)264-267.
{31K.Hamamoto,Y、Tanaka,S、Y・lEe,N、Hosokawa,N,Sakaya,MHosoya,mShoki,T・Watanabe,H・Kinoshita,J・VacSci・TEchno1.23(6B)(2005)2852-2855.
I41HirooKinoshita,KazuhiroHamamoto,NobuyukiSakaya,MorioHosoya,TakeoWatanabe,Jpn.』、Appl・Phys、46(9B)(2007)6113-6117.
151H、Kinoshita,T,Yoshizumi,MOsugi,J・Kishimoto,T・Sugiyama,T・Uno,正Watanab,Microelectron.E、9.86(2009)505-508.
{61YoshitoKamaji,KeiTakase,TakahimYoshizumi,TakashiSugiyama,TbshiyukiUno,TakeoWatanabe,Jpn.』・AppLPhys、48(2009)o6FAO7.
111111'''''''''''''''''''''''''''111円033521207801
I71KHamamoto,N・Sakaya,MHosoya,M・Kureishi,R・Ohkubo,T,Shoki,O・Nagarekawa,J・Kishimoto,mWatanmabe,H・Kinoshita,J、VacSci・Technol.B27(4)(2009)1938-1942.
181K.Takase,Y・Kamaji,N・Sakagami,T・Iguchi,M、Tada,Y・YamaguChi,Y・Fukushima,T・Harada,T・Watanabe,H・Kinoshita,jpn.』、AppLPhys、49(2010)O6GDO7・
I91EJ、Takahashi,Y・Nabekawa,KMidorikawa,Appl・Phys、IEtt、84(2004)4.I101Y・Nagata,K・Furusawa,Y、Nabekawa,K、Midorikawa,OpticsI足tt、32(7)(2007).I111T、Harada,j、Kishimoto,T・Watanabe,H、Kinoshita,,.G・IEe,J・Vac・Sci、kchnol.
B27(2009)3203.
I121JMiao,P、Charalambous,J・Kirz,D、Sayre,Nature(Ipndon)400(1999)342.[131j・Miao,Y、Nishino,Y、Kohmura,B・Johnson,C・Song,S、H、Risbud,T・Ishikawa,
Phys・Rev・Lett,95(2005)085503.[141J.R,Fienup,Appl・Opt、21(1982)2758.