纳米材料和纳米结构第七讲.ppt
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第七讲,PhysicalVaporDeposition物理气相沉积,纳米材料和纳米结构,PhysicalVaporDeposition(PVD),DefinitionFilmdepositionbycondensationfromvaporphaseThreeStepsofPVDGeneratingavaporphasebyevaporationorsublimationElectron-beamevaporationMolecular-beamepitaxyThermalevaporationSputteringCathodicarcplasmadepositionPulsedlaserdepositionTransportingthematerialfromthesourcetothesubstrateFormationoffilmbynucleationanddiffusion,ApplicationCoatingsofelectronicmaterialsInsulatorSemiconductorConductorSuperconductorNanometerscalemultilayerstructuresAdvancedelectronicdevicesAbrasionresistantcoatings,ConcernedProblemsandChallengesContaminationattheinterfacesorintermixingMulti-materialsystemsinvolvedCostofequipmentandmaintenanceComplexionofoperationSystemsDescribedinThisSectionSputteringPulsedlaserdeposition,1Sputtering(溅射),1-1PrincipleofSputtering1-2SputteringSystem1-3PreparingMultilayerStructuresbySputtering1-4CurrentStatusofSputtering,1-1PrincipleofSputtering,EjectionofAtomsfromtheTargetEnergeticparticlesbombardingatargetsurfacewithsufficientenergy(50eV1000eV)TargetCathode,connectedtoanegativevoltagesupplyComposedofthematerialstobedepositedSubstrateAnodeMaybegrounded,floated,orbiased,GlowDischargeMediuminSputteringChamberAgasoramixtureofdifferentgases,mostcommonlyArorHeInreactivesputtering:
introducereactivegasessuchasO2orN2Pressure:
afewmTorrtoseveralhundredsmTorrProcedureGenerationofpositiveions:
ionizingthesputteringgasbyglowdischargeBombarding:
acceleratedpositiveionstostrikethetargetsurfaceandremovemainlyneutralatomsCondensation:
neutralatomsleavethetargetandcondenseonthesubstratesurface,andformintothinfilms,AnImportantConcept:
SputteringYieldAmeasurementoftheefficiencyofsputteringRatioofthenumberofemittedparticlestothenumberofbombardingones,1-2SputteringSystem,TypicalTypesofSputteringSystemsDirectcurrent(dc)diodesputteringUsedforsputteringconductingmaterialsRadiofrequency(rf)diodesputteringUsedforsputteringinsulatingmaterialsMagnetrondiodesputteringMostcommonlyusedtodayPlasmabeconfinedaroundthetargetsurfacebyamagnetfieldAdvantagesofusingmagnetronsputteringFeasibilityoflargecathodesizeHighsputteringyieldLessbombardmenttothesubstrate,用于制备TiN/VN多层膜的磁控溅射系统,氩气,流量表,流量控制阀,压力传感器,低温泵,低温泵,靶1,靶2,旋转衬底支架,衬底,流量表,阀门,流量表,流量控制阀1,流量控制阀2,主流量控制阀,质谱仪,阀门,锁定装置,Waystoreducethedamageandre-sputteringofgrowingfilmDamagecausedbynegativeioneffectandradiationenhanceddiffusionImprovementmethodUsehighgaspressure:
toreducetheenergyofthenegativeionsUseoff-axissputtering:
toavoidthesubstratedirectlyfacingthecathodeDisadvantageofoff-axissputtering:
lowdepositionratesmalldepositionareaDepositionofmagneticmaterials:
facingtargetsputteringsystems,偏轴溅射系统示意图Schematicofoff-axissputteringsystem,可360度旋转的衬底支架,陶瓷加热器,负离子撞击区,衬底,靶,溅射枪溅射源,屏蔽闸,空间屏蔽区,正面溅射系统示意图Schematicofthefacingtargetsputteringsystem,衬底,靶,磁体,冷却水,氩气,1-3PreparingMultilayerStructuresbySputtering,TypesandPropertiesofMultilayerStructuresTypesofarchitecturesMetal/metalCeramic/ceramicMetal/ceramicSemiconductor/semiconductorStructuralandphysicalpropertiesWithstructurallymodulatedarchitecturesWithcompositionallymodulatedarchitecturesHighinterfacevolumefractionLargeintrinsicstressWithstructuraland/orcompositionalgradientExhibitinguniqueandenhancedelectric,dielectric,magnetic,andmechanicproperties,BaTiO3NanolayerFerroelectricThinFilmCapacitorsAdvantage:
higherrelativedielectricconstantDisadvantage:
highleakagecurrentElectricalpropertiesstronglydependingupontheprocessingcondition,microcrystalstructure,andchoiceofbottomelectrodeAmorphous:
lowdielectricconstant(16at105V/cm),lowleakagecurrentPolycrystalline:
highdielectricconstant(400at105V/cm),highleakagecurrentAimofnanolayerstructureBaTiO3filmcapacitor:
highdielectricconstantandlowleakagecurrent,RealizationandeffectsSubstrate:
Ru/SiO2/SiTechnique:
rfmagnetronsputtering,sputteringinterruptionbetweenlayerstochangethesubstratetemperatures(680C,60C)Layerstructure:
n-cyclealternatelayersofamorphousandpolycrystallineBaTiO3(microcrystallinebeobtainedbyannealingamorphouslayer)ResultsobtainedLeakagecurrentdensitybeconsiderablyreduced,andtheeffectbecomingbetterwithincreasingcyclenumberDielectricconstantbetwoorthreetimeshigherthansingleamorphouslayerbutlowerthanasinglepolycrystallinelayer,具有纳米多层结构的BaTiO3薄膜电容器横截面示意图,NanolayerMoSi2/SiCSubstrate:
singlecrystalsilicon(sc-Si)Techniques:
MagnetronsputteringfordepositionofMoSi2rfsputteringfordepositionofSiCMoSi2/SiClayeredcompositesbepreparedbycyclicallypassingthesamplesbeneaththetwotargetswithaspeed(thicknessof10nm/3nm)Heattreatmentorannealing:
inducingrecrystallizationintheMoSi2/SiCmultilayeredfilmPropertiesafterannealing:
SuperioroxidationresistanceSignificanthardness,MoSi2/SiC多层膜的剖面透射电镜图片Cross-sectionalTEMimageofMoSi2/SiCmultilayeredfilm,MoSi2/SiC多层膜退火前的电子衍射花样ElectronDiffractionPatternofMoSi2/SiCmultilayeredfilmbeforeannealing,经过800C,1h退火处理的MoSi2/SiC多层膜的低放大倍数亮场电镜照片,NanolayerCu/NbSubstrate:
(100)sc-SiTechniques:
dcmagnetronsputteringLayerthickness:
(100nm/100nm)Properties:
HighstrengthSuperiorthermalconductivitySuperiorelectricalconductivity,通过磁控溅射技术沉积的Cu/Nb多层膜的剖面透射电镜图像,Cu/Nb多层膜的电子衍射花样ElectrondiffractionpatternofCu/Nbmultilayer,1-4CurrentStatusofSputtering,AdvantagesMostwidelyusedsputteringmethodWell-establishedcoatingtechniquesformicroelectronicapplicationsManynanometermultilayerstructuresbepreparedbysputteringShortcomingsMaterialssystemlimitation:
mainlyconductorsornitridesDifficultyincontrolstoichiometry,lowdepositionrateetc.Bequestionabletobeusedasthemaincoatingtoolinmicroelectronicsindustry(althoughsuccessfulforSrTiO3,BaTiO3,andBa1-xSrxO3),2-1PrinciplesofPLD2-2DepositionofNano-ScaleMetalOxideThinFilms2-3MultilayerStructuresPreparedbyPLD2-4CurrentStatusofPLD,PulsedLaserDeposition(PLD,脉冲激光沉积),2-1PrinciplesofPLD,AdvantagesandPropertiesofPLDSimplestdepositiontechniqueamongallthinfilmgrowthtechniquesStoichiometricremovalofconstituentspeciesfromtargetVersatiledepositionofawidevarietyofmaterialsMetalsSemiconductorsNitridesDielectricmaterialsOxidesOrganiccompounds/ploymersTernarycompounds,TechnicalDescriptionofPLDBasedonphysicalvapordepositionImpactofhigh-powershortpulsedlaserradiationonsolidtargetsRemovalofmaterialsfromimpactzoneEquipmentconstituentHighpowerlaser:
externalenergysourcetovaporizetargetmaterialsVacuumchamberwithaquartzwindowTargetholderormultipletargetholderSubstrateholder(withaheater)Integrationwithothertypeofevaporationsources,脉冲激光沉积系统(示意图)SchematicdiagramofaPLDsystem,激光束,加热器,衬底,喷流,靶,2-2DepositionofNanoscaleMetalOxideThinFilms,ImportanceMetaloxidescouldexhibitversatilepropertiesHightemperaturesuperconductivityFerroelectricityColossalmagnetoresistivityNon-linearopticalpropertiesMetaloxidesberecognizedaspossiblecandidatesfornextgenerationelectronicmaterialsduetotheirdiverseproperties,SubstratesforMetalOxideFilmsImportance:
properchoiceofsubstratebeessentialforaccomplishingperfect2-dimensionalepitaxyofmetaloxideheterostructuresRequirementsforagoodsubstrateGoodinplanelatticematchThermalexpansioncoefficientclosetothatoffilmAtomicallysmoothsurfaceGoodchemicalcompatibilitywiththefilm,CommonlyusedsinglecrystalsubstratesYttria-stabilizedzirconia(YSZ)MgOLaAlO3SrTiO3NdGaO3(LaAlO3)0.3(Sr2AlTaO6)0.7SapphireSurfacetreatmentofsubstratesIonmilling+insituannealingIonmilling+pre-depositionChemicaletching+annealingSurfaceterminating,InitialGrowthofMetalOxideFilmsObservationandmonitortechniquesInsitu:
reflectedhighenergyelectrondiffraction(RHEED),laserlightscattering,real-timeopticaldiagnosisExsitu:
scanningtunnelingmicroscope(STM),atomicforcemicroscopy(AFM),cross-sectionaltransmissionelectronmicroscopy(TEM),X-raydiffractionGrowthModeHighlydependinguponthequalityofsubstrateStranski-Krastanovmode(layerplusislandgrowth)toVolmer-Webermode(islandgrowth)atacriticalthicknessScrew-growthinthickerfilms,Layerplusislandgrowth(ThicknessCriticalThickness),Islandgrowth(ThicknessCriticalThickness),YBCO薄膜的早期生长模式及其转变,D.-W.Kimetal.,PhysicaC313(1999)246,CharacterizingmultilayerthicknessbyX-raydiffractionYBCO/PrBCOsuperlattice:
anewman-madeperiodicityThemodulationthicknessinsuperlatticesismeasuredbythepositionofsatellitespeaks,givenbyD=(/2)/(sinn+1-sinn)DisthemodulationthicknesswithD=dYBCO+dPrBCO;isthewavelengthofX-raysource;n+1andnarepositionsofthenthandthe(n+1)thsatellitepeaksThesatellitepeaksuptothefourthorderindicateatomicallysharpandflatinterfaces,NominalThickness2.4nm/12nm,CalculatedThickness14.6nm,C.Kwonetal.,Appl.Phys.Lett.62(2004)1289,X-ray-2scanaround(001)and(002)peaksofaYBCO/PrBCOsuperlattice,CharacteringfilmthicknessbylowangleX-raydiffractionCharacteringfilmthicknessbySTM,AFM,SEM,andTEM,C.Kwonetal.,Appl.Phys.Lett.62(2004)1289,AlowangleX-rayreflectionofanominally27.6nmthickYBCOonNdGaO3,SuperconductivityinaUnit-cellThickYBCOAimedQuestions:
Whatistheminimumunitneededfortheoccurrenceofsuperconductivity?
HowessentialistheinterlayercouplingbetweenCu-Oplanesindeterminingthetransitiontemperature?
Waytothequestion:
usingsuperlatticestructuresasmodelsystem(possiblecouplingorotherparameterscanbechangedartificiallybyinterposingothermaterialsinbetweentheCu-Oplanesorunit-cells)SystemComposing:
UltrathinYBCOlayers+nonsuperco