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Publié par | karlsruher_institut_fur_technologie |
Publié le | 01 janvier 2010 |
Nombre de lectures | 36 |
Langue | English |
Poids de l'ouvrage | 1 Mo |
Extrait
MaximalRegularityinWeightedSpaces,
Conditions,BoundaryNonlinearttractorsAGlobaland
ZurErlangungdesakademischenGradeseines
WISSENSCHAFTENTURNADERDOKTORS
vonderFakultätfürMathematikdes
KarlsruherInstitutsfürTechnologie
genehmigte
TIONATDISSER
onv
MartinMeyries
RheinamGermersheimaus
TagdermündlichenPrüfung:24.November2010
Referent:Prof.Dr.RolandSchnaubelt
Korreferenten:Prof.Dr.JanPrüss,Prof.Dr.LutzWeis
Für
meine
Eltern
tstenCon
ductiontroIn
1
1TheSpacesLandWeightedAnisotropicSpaces11
p,µ1.1BasicProperties.................................11
1.2AbstractProperties................................28
1.2.1AbstractMaximalL-Regularity...................28
p,µ1.2.2Operator-ValuedFourierMultipliers..................31
1.3WeightedAnisotropicSpaces..........................32
1.3.1TheNewtonPolygon...........................34
1.3.2TemporalTraces.............................38
1.3.3SpatialTraces...............................44
1.3.4PointwiseMultipliers...........................50
2MaximalLp,µ-RegularityforStaticBoundaryConditions65
2.1TheProblemandtheApproachinWeightedSpaces.............65
nn2.2TopOrderConstantCoefficientOperatorsonRandR..........72
+2.2.1TheFull-SpaceCasewithoutBoundaryConditions..........72
2.2.2TheHalf-SpaceCasewithBoundaryConditions............73
2.3TopOrderCoefficientshavingSmallOscillation................79
2.4TheGeneralCaseonaDomain.........................86
2.5ARight-InversefortheBoundaryOperator..................98
3MaximalL-RegularityforBoundaryConditionsofRelaxationType113
p,µ3.1TheProblemandtheApproachinWeightedSpaces.............113
3.2Half-SpaceProblemswithBoundaryConditions................125
3.2.1ConstantCoefficients...........................125
3.2.2TopOrderCoefficientshavingSmallOscillation............134
3.3TheGeneralCaseonaDomain.........................138
4AttractorsinStrongerNormsforRobinBoundaryConditions143
4.1Introduction....................................143
4.2SuperpositionOperators.............................146
4.3TheLocalSemiflow................................153
4.4GlobalAttractorsinStrongerNorms......................160
4.5Applications....................................164
4.5.1Reaction-DiffusionSystemswithNonlinearBoundaryConditions..164
4.5.2AChemotaxisModelwithVolume-FillingEffect...........165
4.5.3APopulationModelwithCross-Diffusion...............166
5BoundaryConditionsofReactive-Diffusive-ConvectiveType167
5.1Introduction....................................167
5.2MaximalL-RegularityfortheLinearizedProblem.............169
p,µ5.3TheLocalSemiflowforQuasilinearProblems.................173
5.4APrioriHölderBoundsimplyGlobalExistence................175
5.5TheGlobalAttractorforSemilinearDissipativeSystems...........180
191endixAppAnA.1BoundariesofDomainsinR..........................191
A.2InterpolationTheory...............................192
A.3SectorialOperators................................194
A.4FunctionSpacesonDomainsandBoundaries.................201
A.5DifferentialOperatorsonaBoundary......................205
A.6Gagliardo-NirenbergInequalities........................207
yBibliograph
209
ductiontroIn
Thesubjectofthisthesisisthemathematicalanalysisoflinearandquasilinearparabolic
problemswithinhomogeneousandnonlinearboundaryconditions.Weconsiderstatic
boundaryconditionsofDirichlet,NeumannorRobintype,andfurtherboundarycon-
ditionsofrelaxationtype,whichincludedynamiconesaswellasboundaryconditionsthat
ariseinthelinearizationoffreeboundaryproblems.
Evolutionequationsofthistypedescribeagreatvarietyofphysical,chemicalandbiological
phenomena,likereaction-diffusionprocesses,phasefieldmodels,chemotacticbehaviour,
populationdynamics,phasetransitionsandthebehaviouroftwophasefluids,forinstance.
Inmanycasesitisnecessarytoimposenonlinearboundaryconditionsintoareaction-
diffusionmodeltocapturethedynamicsofthephenomenonunderinvestigation.Inthe
contextoffreeboundaryproblemsnonlinearboundaryconditionsnaturallyariseaftera
transformationtoafixeddomain.
WefocusonmaximalregularityresultsinweightedLp-spacesforlinearnonautonomous
parabolicproblemswithinhomogeneousboundaryconditions.Comparedtotheapproach
withoutweights,weareabletoreducethenecessaryregularityoftheinitialvalues,to
incorporateaninherentsmoothingeffectintothesolutionsandtoavoidcompatibility
conditionsattheboundary.Thesepropertiesserveusasabasisforconstructingalocal
semiflowforthecorrespondingquasilinearproblemsinascaleofphasespaces,andforthe
investigationofthelong-timebehaviourofsolutionsintermsofglobalattractors.
Ourapproachtoquasilinearproblemsthusreliesonlinearizationandagoodunderstanding
ofthelinearproblem.ThisideagoesbackatleasttoKato[58],Sobolevskii[77]and
Solonnikov[79].InasemigroupcontextitwascarriedoutbyGrisvard[46],DaPrato&
Grisvard[22],Amann[3,4,5,6,7],DaPrato&Lunardi[23],Lunardi[67]andPrüss[70].
Semilinearproblemscanbetreatedintheframeworkofanalyticsemigroups,seeHenry’s
[51].monograph
Maximalregularitymeansthatthereisanisomorphismbetweenthedataandthesolution
ofthelinearprobleminsuitablefunctionspaces.Havingestablishedsuchasharpregularity
resultforthelinearization,thecorrespondingquasilinearproblemcanbetreatedbyquite
simpletools,likethecontractionprincipleandtheimplicitfunctiontheorem.Thereare
approachesinspacesofcontinuousfunctions(seeAngenent[12]andClément&Simonett
[19]),inHölderspaces(seeLunardi[67])andinLp-spacesforp∈(1,∞)(seeClément
2
ionuctdIntro
&Li[17]andPrüss[70]).Formoredetailsandotherapproachestoquasilinearparabolic
problemswerefertothediscussionin[10].
Thethreementionedmaximalregularitysettingshaveadvantagesanddisadvantages.The
continuoussettingisquitesimple,butstrongrestrictionsontheunderlyingspacesare
necessary.IntheHöldersettingthenonlinearitiesareeasytohandleandtheapproach
isalsoapplicabletofullynonlinearproblems,butunpleasantcompatibilityconditionsat
theinitialtimearenecessaryandaprioriestimatesinhighnormsarerequiredtoshow
globalexistenceofsolutions.IntheLp-settingpowerfultoolsfromvector-valuedharmonic
analysisareavailable(andneeded!),butontheotherhandgeometricassumptionsonthe
underlyingspacesarerequiredandalsohereonehastoworkinhighnorms.Forafurther
discussionwereferagainto[10].InthisthesisweentirelyworkinanLp-framework.
TodecidewetheraconcretelinearproblemenjoysmaximalLp-regularityinasuitable
settingisnoteasy.Forlinearproblemswhichcanbereducedtoanabstractequationof
formthe∂tu(t)+Au(t)=f(t),t>0,u(0)=u0,(1)
onaBanachspaceE,whereAisaclosedanddenselydefinedoperatoronE,theoperator
summethod,asdevelopedbyDaPrato&Grisvard[21]andextendedbyDore&Venni[31]
andKalton&Weis[57],isappropriateinmanycases.Weis[85]characterizedthemaximal
Lp-regularitypropertiesofanoperatorintermsofR-sectoriality.IfEisaHilbertspace,
theneverynegativegeneratorofaboundedanalyticC0-semigroupenjoysmaximalLp-
regularity.Unfortunately,aHilbertspacesettingdoesoftennotseemtobesuitableforthe
applicationstoquasilinearproblems.
Totreatsecondorderparabolicdifferentialequationswithinhomogeneousornonlinear
boundaryconditionsinamaximalLp-regularityapproachonetypicallychoosesE=Lp,
E=Wp−1orEasaninterpolationspaceinbetweenasabasicunderlyingspace.IfEis
closetoWp−1thentheboundaryconditionsareapriorionlysatisfiedinaweaksense,butin
thiswaytheproblemcanbecastintheform(1)andoperatorsummethodsareavailable,
inprinciple.IfEisclosetoLp,thentheboundaryconditionscanbeunderstoodina
pointwisesense,butaformulationintheabstractform(1)doesnotseemtobepossiblein
areasonableway,ingeneral-thereisalwaysa’PDEpart’lefttodealwith.Anadvantage
ofchoosingEclosetoLpisthatgrowthconditionsonthenonlinearitiescanbeavoided.
Combiningoperatorsummethodswithtoolsfromvector-valuedharmonicanalysis,Denk,
Hieber&Prüss[24,25]andDenk,Prüss&Zacher[26]showedmaximalLp-regularitywith
Lpasanunderlyingspaceforalargeclassofvector-valuedparabolicproblemsofevenorder
withinhomogeneousboundaryconditions.In[25]problemswithboundaryconditionsof
statictypeareconsidered,i.e.,
∂tu+A(t,x,D)u=f(t,x),x∈Ω,t>0,
Bj(t,x,D)u=gj(t,x),x∈Γ,t>0,j=1,...,m,(2)
u(0,x)=u0(x),x∈Ω.
tioncduIntro
3
Thisincludesthelinearizationofreaction-diffusionsystemsandofphasefieldmodelswith
Dirichlet,NeumannandRobinconditions.In[26]theauthorsstudyproblemswithbound-
aryconditionsofrelaxationtype,i.e.,
∂tu+A(t,x,D)u=f(t,x),x∈Ω,t>0,
∂tρ+B0(t,x,D)u+C0(t,x,DΓ)ρ=g0(t,x),x∈Γ,t>0,
Bj(t,x,D)u+Cj(t,x,DΓ)ρ=gj(t,x),x∈Γ,t>0,j=1,...,m,(3)
u(0,x)=u0(x),x∈Ω,
ρ(0,x)=ρ0(x),x∈Γ,
whichincludesdynamicboundaryconditionsaswellasproblemsarisingaslinearizations
offreeboundaryproblemsthataretransformedtoafixeddomain.HereΩ⊂Rnisa
domainwithcompactsmoothboundaryΓ=∂Ω.Thecoefficientsoftheoperatorsareonly
assumedtobepointwisemultiplierstotheunderlyingspaces,andthetopordercoefficients
arerequiredtobeboundedanduniformlycontinuous.Theseregularityassumptionsallow
toapplythelinearresultstoquasilinearproblems.Earlierinvestigationson(2)startedat
leastwithLadyzhenskaya,Solonnikov&Ural’ceva[64]andincludealsoWeidemaier[84].
AprincipleshortcomingofthemaximalLp-regularityapproachto(1),(2)and(3)isthat
forfixedponecansolvetheequationforinitialvaluesonlyinonesinglespaceofrelatively
highregularity,andthatonedoesnothavetheflexibilitytoworkinascaleofsp