ContentslistsavailableatScienceDirect
The
Journal
of
Supercritical
Fluids
j o ur na l h o me p a g e :w w w . e l s e v i e r . c o m / l o c a t e / s u p f l uImprovement
mechanism
of
resistance
random
access
memory
with
supercritical
CO
2
fluid
treatment
Kuan-Chang
Chang
a,
Jung-Hui
Chen
b,
Tsung-Ming
Tsai
a,
Ting-Chang
Chang
c,i,∗,
Syuan-Yong
Huang
a,
Rui
Zhang
d,
Kai-Huang
Chen
e,
Yong-En
Syu
c,
Geng-Wei
Chang
f,
Tian-Jian
Chu
a,
Guan-Ru
Liu
c,
Yu-Ting
Su
c,
Min-Chen
Chen
c,
Jhih-Hong
Pan
a,
Kuo-Hsiao
Liao
a,
Ya-Hsiang
Tai
f,
Tai-Fa
Young
g,
Simon
M.
Sze
c,h,
Chi-Fong
Ai
j,
Min-Chuan
Wang
j,
Jen-Wei
Huang
kaDepartmentofMaterialsandOptoelectronicScience,NationalSunYat-SenUniversity,70Lien-haiRoad,Kaohsiung804,Taiwan bDepartmentofChemistry,NationalKaohsiungNormalUniversity,Kaohsiung,Taiwan
cDepartmentofPhysics,NationalSunYat-SenUniversity,70Lien-haiRoad,Kaohsiung804,Taiwan dSchoolofSoftwareandMicroelectronics,PekingUniversity,Beijing100871,People’sRepublicofChina eDepartmentofElectronicsEngineeringandComputerScience,Tung-FangDesignInstitute,Kaohsiung,Taiwan
fDepartmentofPhotonicsandtheInstituteofElectro-OpticalEngineering,NationalChiaoTungUniversity,Hsinchu300,Taiwan gDepartmentofMechanicalandElectro-MechanicalEngineering,Kaohsiung804,Taiwan
hDepartmentofElectronicsEngineeringandInstituteofElectronics,NationalChiaoTungUniversity,Hsinchu300,Taiwan iAdvancedOptoelectronicsTechnologyCenter,NationalChengKungUniversity,Taiwan
jPhysicsDivision,InstituteofNuclearEnergyResearch,Taoyuan,Taiwan kDepartmentofPhysics,ROCMilitaryAcademy,Kaohsiung83055,Taiwan
a
r
t
i
c
l
e
i
n
f
o
Articlehistory: Received22August2012
Receivedinrevisedform30August2013 Accepted4September2013 Keywords: Supercriticalfluid RRAM Hydration–dehydrationreaction Tindoping
a
b
s
t
r
a
c
t
WedemonstratedthatthesupercriticalCO2fluidtreatmentwasanewconcepttoefficientlyreducethe
operationcurrentofresistancerandomaccessmemory.Thedanglingbondsoftin-dopedsiliconoxide (Sn:SiOx)thinfilmwerepassivatedbythehydration–dehydrationreactionthroughsupercriticalCO2fluid
treatment,whichwasverifiedbytheXPSandFTIRanalyses.Thecurrentconductionmechanismoflow
resistancestateinpost-treatedSn:SiOxthinfilmwastransferredtohoppingconductionfromOhmic
con-duction.Furthermore,thecurrentconductionmechanismofhighresistancestateinthememorydevice wastransferredtoSchottkyemissionfromFrenkel–Pooleconduction.Thephenomenawereattributedto thediscontinuousmetalfilamentformedbyhydration–dehydrationreactioninSn:SiOxthinfilmthrough
supercriticalfluidtreatment.Finally,areactionmodelwasproposedtoexplainthemechanismofcurrent reductioninSn:SiOxthinfilmwithsupercriticalCO2fluidtreatment.
Crown Copyright © 2013 Published by Elsevier B.V. All rights reserved.
1. Introduction
Fortheincreasingdemands forportable electronicproducts, nonvolatilememoryhasbeenwidelyappliedasinformation stor-agedeviceduetoitslowpowerconsumptionproperties.Modern semiconductor nonvolatile memories are scaled constantly to achievelargecapacitywhiledevicefeaturesapproachthe sub-100-nmregime.However,theincreasingdemandfordevicedensities byscalingdimensionisexpectedtobeamajorchallengedueto thetechnicalandphysicallimitation.Tosurmountthetechnical andphysicallimitationissuesofconventionalchargestorage-based ∗ Correspondingauthorat:DepartmentofPhysics,NationalSunYat-Sen Univer-sity,70Lien-haiRoad,Kaohsiung804,Taiwan.Tel.:+86675252000x3708; fax:+8867.
E-mailaddress:[email protected](T.-C.Chang).
memories[1–8],theresistancerandomaccessmemory(RRAM) constructedofaninsulatinglayersandwichedbytwoelectrodes iswidelyinvestigatedbyindustriesandacademics.TheRRAMisa greatpotentialcandidatefornext-generationnonvolatilememory due to their superior characteristics such as lesser cost, sim-plestructure,high-speedoperation,andnon-destructivereadout [9,10].Variousmaterialshavebeenreportedtopossessresistive switchingbehaviors,suchassolid-electrolyte-basedRRAM[11,12], transitionmetaloxides(MnOx,ZrOx,HfOx)[13–15,9,16,17],and
organicmaterial[18].Inaddition,manyswitchingmechanismof RRAM have been proposedto explain resistive switching phe-nomenon,suchasconductivefilaments[19],valencechange[20], and Schottkybarrier [21]. However,theunderlyingmechanism ofresistiveswitchingbehaviorisstillnotyetunderstoodclearly. Silicon-basedoxideisapromisingmaterialforRRAMapplications becauseofitsgreatcompatibilityinintegratedcircuit(IC)process. 0896-8446/$–seefrontmatter.Crown Copyright © 2013 Published by Elsevier B.V. All rights reserved.
184 K.-C.Changetal./J.ofSupercriticalFluids85 (2014) 183–189 Therefore,theresearchusingsilicon-basedoxideasthe
resistance-switchinglayerwasworthyofinvestigation.
In our preceding research, supercritical CO2 (SCCO2) fluid
technology was used to improve the dielectric properties and performance of various thin film transistors (TFTs), such as hydrogenated amorphous-silicon TFTs and ZnO TFTs [22–30]. Supercriticalphaseispeculiarwithitscharacteristicsofhigh pen-etrationof gas and solubility of liquid. The supercritical water fluidhastremendousoxidationproperty[31].However,high crit-icaltemperatureandhighcriticalpressureareessentialcondition toachieve supercriticalwater fluid, which isdifficult torealize throughmodernfacilities.Byaddingalittlewaterinto supercriti-calCO2fluids,theliquidwatercanattaintothesupercriticalfluid
phaseduetothephaseclosetoideasolution.
Inthiswork,tinmetaldopedintosiliconoxidebyco-sputtering atroomtemperaturewastakenastheresistanceswitchinglayer of RRAM.To evaluatethe resistiveswitching properties of tin-dopedsiliconoxide(Sn:SiOx)layer,thePt/Sn:SiOx/TiNdevicewas
fabricatedatcleanroom.Moreover,thematerialandconduction mechanism analyseswereexecuted toexplain theinfluence of Snmetaldopedinsiliconoxideonresistiveswitchingbehaviors. Inaddition,thePt/SCCO2-treatedSn:SiOx/TiNsandwicheddevices
were fabricatedto investigate the effect of SCCO2 on resistive
switchingpropertiesofSn:SiOxthinfilm.TheeffectsofSCCO2
treat-mentonresistiveswitchingbehaviorsofSn:SiOxthinfilmwasalso
evaluatedbymaterialandcarrierconductionmechanism analy-ses.Furthermore,thereactionmechanism inRRAMwithSCCO2
fluidwasalsodiscussedtoexplainthereasonofelectricalproperty improvementonSn:SiOxRRAM.
2. Experimental
Theexperimentalspecimenswerepreparedasfollows:Inthe firstgroup,theSn:SiOxthinfilm(about30nm)wasdepositedon
theTiN/Ti/SiO2/Sisubstratebyco-sputtering withthepureSiO2
andSntargets.ThesputteringpowerwasfixedatRFpower200W and3Wfor SiO2 and Sntargetsrespectively.Theco-sputtering
wasexecutedinargonambient(Ar=30sccm)withaworking pres-sureof 0.789Paat roomtemperature. Inthesecondgroup,the Sn:SiOxthinfilmswereputintothereactivechamberof
supercrit-icalfluidsystem,andthentheSCCO2fluidmixedwith0.5mlwater
weresyringedintothereactivechambertotreatthespecimens. Thepassivationefficiencyincreaseswiththerisingoftemperature andCO2pressureaslongasexceedingthecriticalpoint,whichare
31◦Cwith7.3MPaCO2.Butowingtothelimitationofour
exper-imentequipment,thewater-mixedsupercriticalCO2fluidswere
heatedandpressuredto120◦Cand20.4MPainthestainlesssteel chamberofsupercriticalfluidsystemfor1h.Finally,thePttop elec-trodeof200nmthicknesswasdepositedonSn:SiOxthinfilmto
formelectricaldeviceswithPt/Sn:SiOx/TiNsandwichstructuresby
DCmagnetronsputtering.Bycontrast,thePt/SiO2/TiNsandwich
structuresweremade bysame process procedurewitha sput-teredSiO2layerinsteadofaSn:SiOxlayerascontrolsamples.The
entireelectricalmeasurementsofdeviceswiththePtelectrodeof 250mdiameterwereperformedusingAgilentB1500 semicon-ductorparameteranalyzer.Besides,theFouriertransforminfrared spectroscopy(FTIR)measuredbyBrukerVERTEX70v spectrom-eterinfarinfraredregionandX-rayphotoelectronspectroscopy (XPS)wereusedtoanalyzethechemicalcompositionandbonding oftheseinsulatormaterials,respectively.
3. Resultsanddiscussion
The“formingprocess”isrequiredtoactivatealloftheSn:SiOx
RRAM devices, using dc voltage sweeping with a compliance
Fig.1. TheformingcurrentcurvesoftheSn:SiOxRRAMdevicesbeforeandafter SCCO2treatment.
currentof2mA.TheleakagecurrentoftheSn:SiOxRRAMdevices
after SCCO2 treatment was lower than that of pre-treatment
devices(Fig.1).Thisphenomenonisattributedtotheimprovement ondielectricpropertiesthroughSCCO2treatment,whichhasbeen
reportedbyourpreviousstudy[23].Thevoltagesweepbiaswas appliedonTiNelectrodewiththegroundedPtelectrodeasshown inthebottomleftinsetofFig.2.Aftertheformingprocess,a grad-ualdecreaseincurrentwasobservedwherethecellswitchesfrom lowresistancestate(LRS)tohighresistancestate(HRS),calledas “resetprocess”,bysweepingthevoltagefrom0to−1.8Vwithout currentcompliance.Oncontrast,asthevoltagewassweptfrom0to 1.2Vwitha5mAcurrentcompliance,theresistanceswitchedfrom HRStoLRS,calledas“setprocess”.InthePt/Sn:SiOx/TiNdevice,
theresistanceratioofHRSandLRSisabout102timesata
read-ingvoltageof 0.1V. Theelectrical current-voltage propertiesof theSn:SiOxdeviceswerecomparedbeforeandafterSCCO2
treat-ment(Fig.2).ThecurrentofSn:SiOxdevicesisreduced at0.1V
readingvoltageafterSCCO2treatment.Toinvestigatethe
interest-ingphenomena,weanalyzedthecurrentconductionmechanism ofSn:SiOxthinfilmwithandwithoutSCCO2treatmentasshown
inFig.3.ThecarriertransportinLRSstateofSn:SiOxdevicewas
dominatedbyOhmicconductionintheSn:SiOxlayer.AfterSCCO2
treatment,thecurrentconductionmechanismwilltransferto hop-pingconductionbecauseofthechangeofmaterialproperties.In addition,wealsoanalyzedthecurrentconductionmechanismin HRSof Sn:SiOx withand withoutSCCO2 treatmentasshownin
Fig.4.Therelationshipinthecurveofln(I/V)versusthesquareroot
Fig.2.TheblackandredcurvesaretheresistiveswitchingcharacteristicsofSn:SiOx filmbeforeandafterSCCO2treatment,respectively.Thecurrentinhighresistance stateofpost-treatedSn:SiOxfilmisreducedabout15timesfrom9Ato0.6A.
Fig.3. ThecurrentconductioncurvesintheLRSofSn:SiOxdevicesbeforeandafterSCCO2treatment.Thecurrentvs.voltagediagramsweremeasuredatdifferenttemperature environmentsintheSn:SiOxfilmbeforeandafterSCCO2treatment.
Fig.4.ThecurrentconductioncurvesintheHRSofSn:SiOxdevicesbeforeandafterSCCO2treatment.Thefittingofcurrentvs.voltagecurvesintheHRSofthedevicesbefore andafterSCCO2treatmentwasdrawninrightside.
186 K.-C.Changetal./J.ofSupercriticalFluids85 (2014) 183–189
Fig.5.ThecomparisonofFTIRspectraofSn:SiOxfilmbeforeandafterSCCO2 treat-ment.BothintensityofSn OandSi O SibondsareincreasedinSn:SiOxfilmafter SCCO2treatment.
oftheappliedvoltage(V1/2)islinear.Accordingtothe
relation-shipofFrenkel–Pooleconduction,I∝Vexp[(q/kT)(2a√V−Bt)],
whereais
q/4εid,Btisthetrapbarrierheight,anddistheinsu-latorthickness.TheFrenkel–Pooleconductionisduetoemissionof trappedelectronsintoconductionband. Thesupplyofelectrons fromthetrapsisthroughthermalexcitation.Thebarrier reduc-tionis largerthanin thecase ofSchottky emissionby a factor of2,which canbeobtainedascompared withtheslopeofthe plotofln(I)versus(V1/2)basedontheformulaofSchottky
emis-sion,I∝I2exp[(q/kT)(a√V−
B)],whereBistheSchottkybarrier
height.TheresultsrevealedthatthecarriertransportofSn:SiOxfilm
wasdominatedbyFrenkel–Pooleconductionduetothetrapinthe film.AfterSCCO2 treatment,thecurrent conductionmechanism
willtransfertoSchottkyemissionbecauseoftheimprovementof dielectricproperties.Therefore,weutilized thematerial spectra analysestofindoutthereasonofdifferentelectricaltransfer mech-anismsinconductioncurrentbeforeandafterSCCO2 treatment.
ComparedtheFTIRspectraofSn:SiOxfilmwithandwithoutSCCO2
treatment(Fig. 5), we foundthat the absorption peak of Sn-O bondat586cm−1wasincreasedafterSCCO2treatment.Theresult
impliesthatthedensityofSn ObondwasincreasedintheSn:SiOx
filmafterSCCO2treatment.Inaddition,theabsorptionofSi O Si
stretchbondat 450cm−1 wasalsoincreasedafterSCCO2
treat-ment,illustratingthecontentofsiliconoxidebondinginthefilm alsoincreased [32,33].To analyzethe chemical composition of Sn:SiOxfilminthisstudy,X-rayphotoelectronspectroscopy(XPS)
of Sn3d5/2,Si 2p and O1s peakswere performed.After
com-paredwiththepeakareaofSn,SiandOXPSspectra,themole fractionofSn: Si:Oin theco-sputteredSn:SiOx filmwas0.3%:
29.5%:70.2%.AccordingtoXPSspectraanalysesforSn3d5/2core
level(Fig.6),themolefractionofSn Obondwasobviouslyrisen butthatofSnelementwasdecreasedinSn:SiOxfilmafterSCCO2
treatment.Besides,themolefractionofSi Obondwas substan-tiallyincreasedincontrastwiththatofSi OHbondafterSCCO2
treatmentintermsoftheXPSspectraanalysesofSi2pcorelevel asshowninFig.6.Table1showsthecomparisonoftheareasof deconvolutionpeaksofSn3d5/2andSi2pcorelevels.Wefoundthe
molefraction(SnO2:Sn=50.6%:49.4%)inSn:SiOxfilmischanged
tothat(SnO2:Sn=70.6%:29.4%) afterSCCO2 treatment.Also,the
molefraction(SiOH:SiO2=18.9%:81.1%)inSn:SiOxfilmischanged
tothat(SiOH:SiO2=66.4%:33.6%)inthepost-treatedSn:SiOxfilm.
Therefore,weinferthatthelevelofoxidationwouldincreaseand
Fig.6. XPSspectraofSn3d5/2andSi2pcorelevelsinSn:SiOxfilmbeforeandafterSCCO2treatment.ThemolefractionofmetallictinandSi OHbondsinSn:SiOxfilmare reducedobviouslybutthatoftinoxideandsiliconoxidebondsareincreasedafterSCCO2treatment.
Fig.7. Theschematicdiagramofhydration–dehydrationreactionmechanismonSn:SiOxfilmtoillustratedefectpassivationthroughSCCO2treatment.
Table1
ComparisonoftheareasofdeconvolutionpeaksofSn3d5/2andSi2pcorelevels beforeandafterSCCO2treatment.
SnO2 Sn SiOH SiO2
BeforeSCCO2 50.6% 49.4% 66.4% 33.6%
AfterSCCO2 70.6%↑ 29.4%↓ 18.9%↓ 81.1%↑
accompanywithdehydrationinthepost-treatedfilm.Theseresults
wereconsistentwiththeabove-mentionedFTIRanalyses.
Basedontheelectricalandmaterialanalyses, weproposeda
reactionmodetoexplainreactionmechanismofSn:SiOxfilmwith
SCCO2 treatmentasshowninFig.7.Asthesamplewasputinto
thewater-mixedSCCO2fluidenvironment,theH2Omoleculewas
carriedinto thegrainboundaryof Sn:SiOx film bySCCO2 fluid,
whichisattributedtothehighpenetrationabilityofSCCO2fluid.
AstheH2Omoleculeapproachedtograinboundaryofthefilm,the
hydrationreactionoccurredintheSn:SiOxfilm.Then,
monomolec-ularCO2insupercriticalfluidsinducesthedehydrationofneighbor
hydroxylgroupssoastoformSi O SiandSn O Sinetwork-like bondinginthefilm.Themechanismiscallhydration–dehydration reactionofSCCO2fluidsinSn:SiOxfilm.AsfortheLRSofSn:SiOx
film,theconductivefilamentwillbeformedinpre-treatedSn:SiOx
filmaftertheformingprocess.Theconductivefilamentwillbe con-nectedwithdanglingbondintheswitchingregionofthefilm.The carriersweretransportedthroughthesedanglingbonds,leading tothecurrentconductiondominatedbyOhmicconduction.Ifthe Sn:SiOxfilmwasputintotheSCCO2fluidenvironment,theH2O
moleculewascarriedintothegrainboundaryofthefilmbySCCO2
fluid,whichisattributedtothehighpenetrationabilityofSCCO2
fluid.Hence,thetinmetalinSn:SiOxthinfilmwillbeisolateddue
tohydration–dehydrationreaction bySCCO2 treatment.Onlyif
theconductive filamentformed in theSn:SiOxfilm, thecarrier
willhopthroughtheisolated tinmetalintheswitchingregion ofthepost-treatedfilm.Thisphenomenawillmaketheelectrical
currentconductioninLRSofSn:SiOxfilmtransferredfromOhmic
conductiontohoppingconductionasshownin Fig.8.Owingto thetrapofSn:SiOx filmcanbepassivated bySCCO2 treatment,
theelectrical currentconduction inHRSofSn:SiOxfilm willbe
transferredtoSchottkyemissionfromFrenkel–Pooleconduction asshowninFig.9.Thisphenomenonwillcausetheimprovementof dielectricpropertiesofthinfilm,leadingtodecreasetheoperation currentandthepowerconsumptionofRRAM.
Fig.8. TheschematicdiagramofcarrierhoppingmodelinSn:SiOxfilmafterSCCO2 treatment.
188 K.-C.Changetal./J.ofSupercriticalFluids85 (2014) 183–189
Fig.9.TheschematicdiagramofthetransferoncarrierconductionmechanisminSn:SiOxfilmafterSCCO2treatment.
4. Conclusion
Insummary,theoperationcurrentofSn-dopedsiliconoxide RRAMdevicewasreducedbysupercriticalfluidtreatmentinthis study.Thewatermolecularcanbebroughtintothefilmto pas-sivatethedanglingbondofgrainboundaryinresistiveswitching layerbysupercriticalCO2 fluid.Invirtueofthephenomena,the
discontinuousconductivefilamentinSn:SiOxfilmwasformedby
hydration–dehydrationreactionthroughSCCO2fluids.The
opera-tioncurrentofRRAMcanbereducedduetothedecreaseofdefect inthelayer,which resultsin lowpowerconsumption. Besides, theeffectofjouleheatingcanalsobeimprovedforthedevice. Therefore,supercriticalfluidtreatmentcanenhancethe proper-tiesofresistiveswitchinglayerofRRAMdevice.Webelievethat thetechnologyisbeneficialtothedevelopmentofRRAMforthe nextgenerationnonvolatileapplications.
Acknowledgments
ThisworkwasperformedattheNationalScienceCouncilCore Facilities Laboratory for Nano-Science and Nano-Technology in theKaohsiung-PingtungareaandwassupportedbytheNational ScienceCounciloftheRepublicofChinaunderContractNos. NSC-102-2120-M-110-001,andNSC101-2221-E-110-044-MY3.
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