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FEMAG晶体生长计算软件GlobalSimulationofCzochralskiSiliconGrowthundertheEffectofaTransverseMagneticFieldFEMAGSoft©2013CzSigrowthunderaTMFMHDboundarylayers:HartmannlayersFEMAGSoft©2013TheHartmannlayersdevelopalongthesurfaceswherethenormalcomponentofthemagneticfieldisnon-negligible.AnorderofmagnitudeofthethicknessofaHartmannlayerisdH=LHa-1(L=RsorRc).Typically
dH=0.05-0.08mminindustrialfurnaces.
CzSigrowthunderaTMF(cont’d)Transversemagneticfields:
FLETmethodMethod:Fourierdecompositionofallfields(velocity,pressure,temperature)Hypothesis:Principalissue:whichandhowmanymodes?Objective:global,quasi-steadyortime-dependent calculationsatareasonablecostFEMAGSoft©2013
CzSigrowthunderaTMF(cont’d)FourierLimitedExpansionTechnique(FLET)FEMAGSoft©2013ThefieldvariablesareexpandedasFourierseriesintheazimuthal(q)direction:CzSigrowthunderaTMF(cont’d)FourierLimitedExpansionTechnique(FLET)FEMAGSoft©2013andwhilethenumberofmodesMis
assmallaspossiblewithoutlossofaccuracy(spectralconvergence).whilethedifferentmodecoefficients:are2DFiniteElementfunctionsofthemeridionalcoordinates(r,z)Thisresultsinasystemwhosesizeisthatofthe2DsystemmultipliedbythenumberofFouriermodesconsideredandhenceinadramaticsystemsizereduction.CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013RadiationtransferCouplingbetween3Dand2Daxisymmetricheattransferacrossaradiativeenclosuretheviewedandhiddenpartsarecalculatedasaxisymmetricor,equivalently,eachsurfaceoftheenclosureisviewedasaxisymmetricfromtheothersurfacesMainmodelinghypothesis:generally3Dcomponentsarerotatingwithrespecttothe2Denvironment3Dcomponentsmostlyview2DcomponentsbecauseofthepresenceofheatshieldsThishypothesisissatisfactorybecause:CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013FlowandglobalheattransferinasiliconCzpullerundertheeffectofaTMF(quasi-steadysimulation)CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Top:
topviewofthevelocitymagnitudeandstreamlines.Bottom:
velocityfieldmagnitudeandcross-sectionshowingasharpHartmannlayeralongthemelt-crucibleinterface.Growthofa300mmdiameterSicrystalundertheeffectofa0.5TTMF.
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013InatypicalTMFconfigurationextremelythinHartmannlayers
of50-80mmdevelopGrowthofa300mmdiameterSicrystalundertheeffectofa0.5TTMF.
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013DetailofthedeformingBoundaryLayerMesh(BLM)usedFlowandglobalheattransferinasiliconCzpullerundertheeffectofaTMFCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Hartmannboundarylayersalongthemelt-crystalandmelt-crucibleinterfacesandassociatedboundarylayermeshes.StrongHartmannbackflowsdevelop.Growthofa300mmdiameterSicrystalundertheeffectofa0.5TTMF.
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013CzSigrowthunderaTMF(cont’d)Czochralskigrowthofasiliconcrystalundera500mThorizontalmagneticfieldGlobalsimulationthegrowthof300mmand400mmcrystalsFEMAGSoft©2013CzSigrowthunderaTMF(cont’d)Growthofa300mmcrystalundera500mTTMFLeft:meltsurfaceRight:meridionalcross-sectionsparallelandperpendiculartothemagneticfieldTop:velocityfieldBottom:temperaturefieldFEMAGSoft©2013CzSigrowthunderaTMF(cont’d)Growthofa400mmcrystalundera500mTTMFLeft:meltsurfaceRight:meridionalcross-sectionsparallelandperpendiculartothemagneticfieldTop:velocityfieldBottom:temperaturefieldFEMAGSoft©2013Czochralskigrowthofasiliconcrystalundera3000or5000GhorizontalmagneticfieldGlobalsimulationofthegrowthof300mmand400mmcrystalsCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013GeometryandoperatingconditionsCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013DescriptionofthesimulationsCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection;topright:topviewCase1CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystal
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case2Crystaldiameter:
300mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCase1
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCase2Crystaldiameter:
300mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystalCase2Crystaldiameter:
300mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystal
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:5000GGasflow:no
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection;topright:topviewCase3
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection;topright:topviewCase1
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCase3Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:5000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystalCase3Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:5000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystalCase3Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:5000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystalCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Ovoidmagneticfield:topleft:sketchofthemagneticfield;bottomleft:sideview;right:topviewCase4CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Ovoidmagneticfield:topleft:sketchofthemagneticfield;bottomleft:sideview;right:topviewCase4
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case4Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection;topright:topviewCrystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoidMagneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection;topright:topviewCase1
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCase4Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoidMagneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case4Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystalCrystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoidMagneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case1Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:no
Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystal
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Ovoidmagneticfield(lifted):topleft:sketchofthemagneticfield;bottomleft:sideview;right:topviewCase5
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case5Ovoidmagneticfield(lifted):topleft:sketchofthemagneticfield;bottomleft:sideview;right:topview2.CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case5Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection;topright:topviewCrystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoid(lifted)Magneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case4Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoidMagneticfieldstrength:±3000GGasflow:no
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssection;topright:topviewCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case5Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCrystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoid(lifted)Magneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Velocityfield
(m.s-1):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCase4Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoidMagneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case5Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystalCrystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoid(lifted)Magneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case4Oxygenconcentration
(m-3):topleft:parallelcrosssectioninmelt;bottomleft:perpendicularcrosssectioninmelt;topright:crystalCrystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:ovoidMagneticfieldstrength:±3000GGasflow:no
CzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Case7Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneticfieldtype:horizontalMagneticfieldstrength:3000GGasflow:yes
Temperaturefield
(K):topleft:parallelcrosssection;bottomleft:perpendicularcrosssectionCzSigrowthunderaTMF(cont’d)FEMAGSoft©2013Crystaldiameter:400mmPullingrate:0.45mm/minCruciblerotationrate:5RPMMagneti
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