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TRANSCRIPT
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Characterizationofa0.14m
SubmicronNMOSwith
SilvacoTCADSimulatorYeapKimHo1*,IbrahimAhmad2andMuhammadSuhaimiSulong3
1DepartmentofPhysicalSciences,ElectricalandElectronics,
UniversitiTunkuAbdulRahman.2DepartmentofElectrical,Electronics,andSystemsEngineering,
UniversitiKebangsaanMalaysia.3FacultyofElectricalandElectronicsEngineering,
UniversitiTunHusseinOnnMalaysia.
*Corresponding email: [email protected]
Abstract
A0.14mNMOSwassimulatedusingATHENAandATLASmodulesfrom
TCADsimulator.Theelectricalcharacteristicsofthesubmicrondevicewere
studied.Constanteldscalingwasappliedtothefollowingparameters:the
effective channel length, the density of the ion implantation for threshold
voltage(VTH)adjustment,andthegateoxidethickness(TOX).Additional
techniquesimplementedtoavoidshortchanneleffectsinsubmicrondeviceswereshallowtrenchisolation(STI),sidewallspacerdeposition,lightlydoped
drain(LDD)implantation,andretrogradewellimplantation.Theresultsshow
thatretrogradewellimplantationallowedthehighestdensityofthedopantto
fallbelowthesurfaceofthesubstrate.Withtheapplicationofsidewallspac-
erandLDDimplantation,alighterdopedregionwascreatedbeyondthen+
drain/sourcejunction.Asthelayersofmetallizationincreases,itwasobserved
thatdraincurrent(ID)increasedaswell.TheimportantparametersforNMOS
weremeasuredandvalidated.
Keywords:sidewallspacer,LDD,retrogradewell,metallization
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1 INTRODUCTION
ThedensityofachipinMOSVLSI(VeryLargeScaleIntegration)hasbeen
growingtremendously for thepastfewdecades. Oneofthereasonsis due
mainlytosizereductionofatransistor.
Startingoffwith50minthe1960s,thegatechannelofatransistor
hasshrunktolessthan0.18min2000(HongXiao2001).Inthispaper,a
0.14mNMOSwassimulatedand studied.Thedevice fabricationprocess
wasrstsimulatedusingtheATHENAmodulefromtheSilvacoVirtualWafer
Fab(VWF)TCADtools.Theelectricalpropertieswerethenvalidatedwiththe
ATLASmodule.
The performance of a 0.14 m NMOS, which falls within thesubmicronregimes,maybeseverelyaffectedbyshortchanneleffects.Thus,
besidesapplyingconstanteld scalingon theeffectivechannel length(Lg),
gateoxidethickness(TOX),andthresholdvoltage(VTH)adjustimplantation,
additional fabrication techniques have been implemented. Shallow Trench
Isolation (STI), sidewall spacer deposition, Lightly Doped Drain (LDD)
implantation,andretrogradewellimplantationweresomeofthetechniques
appliedtoensureproperoperationofthedevice(Slisheretal.2006).
2 SIMULATION PROCESS WALKTHROUGH
Thesimulationprocesscanbeclassiedinto5differentphases.Theyarewell
formation,deviceisolation,transistormaking,andinterconnection(HongXiao
2001). Initially,apwellistobeformedinthep-typesinglecrystalsilicon
(Si)wafer. Screen oxideis grownon the surfaceofthe substrate. This is
followedbyahighenergyimplantation.Thewaferistiltedandrotatedwhen
theimplantationprocessisperformed.
Theobjectiveofgrowingalayerofscreenoxideandtiltingthewafer
istominimizechannelingeffect;whereas,rotatingthewaferistominimize
shadowing effect. Soon after p well is formed, annealing and drive-in is
performedtorepairthelatticedamage(HongXiao2001).
Next,STIisemployedtoisolateneighbouringdevices.Alayerofpad
oxideisrstgrownviadryoxidation.SiliconNitride(Si3N4)isthendeposited
usingLiquidPlasmaChemicalVaporDeposition(LPCVD).Padoxideactsas
astressbufferwhichavoidscracksonSi3N4;whereas,Si3N4actsasamaskforetching.Photoresistisdepositedandphotolithographyisappliedtodene
theactiveregionofthedevice.Subsequently,Si3N4andpadoxideareetched.
Afterthephotoresistisstripped,ReactiveIonEtching(RIE)is implemented
toform trenchesat the2sidesof the active region. Athinlayerofbarrier
oxideis grownin the trenches.Thetrenches are lledupwithoxideusing
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Tetra-Ethyl-Oxy-Silane (TEOS)CVD process. The layerof barrier oxide
prevents impurities from diffusing into the substrate during TEOS CVD
process(HongXiao2001).Theoxideatthesurfaceofthesubstrateisremoved
usingChemicalMechanicalPolishing(CMP)process.STIiscompletedafter
annealingisperformedandSi3N4maskandpadoxideareetched.
Gate oxide is grown via dry oxidation. VTH adjust implantation
is then performed, afterwhich, the substrate undergoes annealing. Next,
polysilicongateis formedbydepositingandetchinga layerofpolysilicon.
The substrate is, again, annealed. LDD is then implanted to suppress hot
electroneffect(HongXiao2001).Subsequently,Si3N4isdepositedviaCVD
process.SidewallspacersareformedbyetchingtheSi3N4lm.Sourceanddrainjunctionsareimplantedonthe2sidesoftheactiveregionsandannealing
processisappliedtoactivatethedopants.Assoonasthebasicstructureofan
NMOSiscompleted,alayeroftitaniumisdepositedonthesubstratesurface.
RapidThermalAnnealing(RTA)isthenemployedtoformsilicideonthegate.
Atransistorisfabricatedsoonaftertheunreactedtitaniumisetched.
Interconnections in between transistors are to be performed with
metallization. A layer of Boron Phosphor Silicate Glass (BPSG) is rst
depositedtoformPremetalDielectric(PMD).PMDactsasaninsulatorfor
multilevelinterconnection(Quirk2001).Afterannealing,BPSGisetchedto
formsource/draincontacts.Therstlevelofmetallizationisdevelopedby
depositing and etching aluminum (Al) on the contacts.An almost similar
procedureistobeperformedonthesecondlevelofinterconnection.Anotherlayer of BPSG, known as Intermetal Dielectric (IMD) (Quirk 2001) is
deposited.ThesimulationprocessiscompletedwhentheredundantIMDis
etched.AsummaryoftheparametersusedinNMOSfabricationisshownin
Table1.
3 SIMULATION RESULTS AND DISCUSSION
A. The 0.14 m NMOS
Figure1showsthecompletecrosssectionofNMOS.Asclearlyshownby
thedopantdensitydistributions,retrogradewelltechniquehasresultedinthe
highestdopantdensityconcentratedacertaindepthbelowthesurfaceofthe
substrate.Itcanalsobeobservedthat,LDDimplantationformedarelatively
lighterndopedregionrightbeneaththesidewallspacers.
B. Retrograde Well
Ascomparedtoconventionalwellformation, inwhich, thehighestdopant
densityliesatthesurfaceofthesubstrate,retrogradewellsusehighenergy
implantationtoplacethehighestdopantdensityatacertaindesiredsubstrate
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depth.Figure2showstheboronconcentrationversusthesubstratedepthof
thesimulated0.14mNMOS.
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Asthechannellengthreduces,thedepletionregionencompassesthe
drainjunctiontendstoextendsfarthertowardsthesource.Atatime,ifthe
depletionregionsofbothdrainandsourcejunctionsmerge,aspuriouscurrent
pathisinevitablyformed.Thegatevoltagewillhavelostitscontroloverthe
currentowinbetweenthe2junctions.Suchphenomenonisknownaspunch
through(Sze1988).
Anincreaseofdopingconcentrationinthesubstrateusingretrograde
wellimplantationallows thedepletionregionsdrain/source junctionsto be
scaleddown.Hence,punchthroughcanbeavoidedwhenthedepletionre-
gionsstayatareasonabledistanceapart.
Figure1.0.14mNMOS.
Figure2.Borondensityversussubstratedepthofa0.14mNMOS.
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C. LDD Implantation
When the dimension of the device shrinks and the supply voltage remain
constant,theelectriceldgeneratedinthesubstratewillincrease.Asaresult,
theelectronsalongthechannelmightgainsufcientenergytobeinjectedonto
thegateoxide.Thechargingofthegateoxidecauseslongtermdegradationon
thedevice.Suchissueisknownashotelectroneffect(Sze1988).
In order to avoidthe electronsfrom gaining sufcient energy,the
electriceldalongthedrainregionistobereduced.Onewayofdoingsois
toimplantalighterndopantsurroundingthen+drain/sourceimplants.As
showninFigure3,thenetdopingofLDDimplantationbeneaththesidewall
spacersisrelativelyshallowcomparedtothedrain/sourceimplants.
D. NMOS Parameters
ImportantparameterssuchasVTH,TOX,andLgaremeasuredandextracted
fromtheATLASmodule. Theparameters arecomparedwith thestandard
parameters published by International Technology Roadmap for
Semiconductor(ITRS)andBerkeleyPredictiveTechnologyModel(BPTM)
(Berkeley2006). Sinceonlythestandardparametersfor 70nm,0.10m,
0.13m,and0.18mNMOSdevicewerepublishedinITRSandBPTM,
polynomial regression technique (using MATLAB tools) was applied to
acquire the required parameters for a 0.14 m NMOS. Table 2 shows a
comparisonbetweentheparametersextractedfromATLASandthestandard
parametersobtainedusingpolynomialregression.ItcanbeobservedthattheparametersextractedfromtheATLASmodulefallwithinthetolerancerange
ofthestandardparametersobtainedthroughregressiontechnique.Therefore,
thesimulationresultsarevalidated.
E. Electrical Characteristics
The ID-VD and ID-Vgelectrical characteristics curves were plotted using
ATLASmodule.
Figure 4 and 5 shows the NMOS ID-VD relationshipsbefore and
after metallization 2; whereas, Figure 6 and 7 shows the NMOS ID-Vg
relationshipsbeforeandaftermetallization2.ThedifferencesinIDbefore
and after second level interconnection were compared. The results are
summarizedinTable3and4.
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Figure3.LDDImplantation.
Figure4.NMOSID-VDrelationshipbeforemetallization2isdeposited.
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Figure5.NMOSID-VDrelationshipaftermetallization2isdeposited.
Figure6.NMOSID-Vgrelationshipbeforemetallization2isdeposited.
As can be seen from Figure 4 to Figure 7, the current- voltage
characteristic curves remain unchanged even though a second layer of
metallizationhasbeendepositedontothedevice.
Nevertheless, ID increases after metallization 2. Since power
consumption is directly proportional to ID, the simulation shows that by
increasingthelevelofmetallization,powerconsumptiontendtoincreaseas
well.
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Figure7.NMOSID-Vgrelationshipaftermetallization2isdeposited.
Table3ComparisonofIdbeforeandafterLevel2MetallizationinId-VdNMOS
Graph.
Table4ComparisonofIdbeforeandafterLevelMetallizationinId-VgNMOS
Graph.
4 CONCLUSION
A0.14msubmicronNMOShasbeensuccessfullysimulatedandvalidated.
The result shows that retrograde well technique controls the highest
concentration dopant at certain depth of the substrate; whereas, LDD
implantation reduces the concentration of n dopant beneath the sidewall
spacers.Thesetechniquesareeffectiveinminimizingshortchanneleffects.
The current-voltage characteristic curves also show that as the level of
interconnectionincreases,IDincreasesaswellwhichshouldresultinhigher
powerconsumption.
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