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Contents lists available atScienceDirect

C. R. Acad. Sci. Paris, Ser. I

www.sciencedirect.com

Partial differential equations/Calculus of variations

A maximum principle for the system u − ∇ W ( u ) = 0

Un principe du maximum pour le système u − ∇ W ( u ) = 0

Panagiotis Antonopoulos

a

, Panayotis Smyrnelis

b

aDepartmentofMathematics,UniversityofAthens,Panepistemiopolis,15784Athens,Greece bCentrodeModelamientoMatemático,UniversidaddeChile,Santiago,Chile

a r t i c l e i n f o a b s t r a c t

Articlehistory:

Received5August2015

Acceptedafterrevision1April2016 Availableonline14April2016 PresentedbyHaïmBrézis

Amaximumprincipleisestablishedforminimalsolutionstothesystemu− ∇W(u)=0, withapotential W vanishingattheboundaryofaclosed convexset C0⊂Rm,whichis eitherC2smoothorcoincideswithapoint{a}.

©2016Académiedessciences.PublishedbyElsevierMassonSAS.All rights reserved.

r é s um é

Nousétablissonsunprincipedumaximumpourlessolutionsminimalesdusystèmeu

W(u)=0,dontlepotentielWs’annuleàlafrontièred’unensembleferméconvexeC0⊂ Rm,declasseC2ouréduitàunpoint{a}.

©2016Académiedessciences.PublishedbyElsevierMassonSAS.All rights reserved.

1. Introductionandstatementofthemaximumprinciple

Wewillconsiderthesystem

u

− ∇

W

(

u

) =

0

,

u

:

A

→ R

m

,

A

⊂ R

n

,

(1)

which isthe Euler–Lagrangeequation of thefree energy functional J

(

u

;

A

) =

A

1

2

|∇

u

|

2

+

W

(

u

)

dx. Assumingthat the potential W satisfies:

(a) W

C1

(R

m

;

R),W

(

a

) =

0 forsomea

Rm,W

0,

(b) thereexistsr0

>

0 suchthatforevery

ξ

Rmwith

|ξ| =

1:

(

0

,

r0

)

r

W

(

a

+

r

ξ )

isstrictlyincreasing, thefollowingmaximumprinciplewasprovedin[1].

E-mailaddresses:[email protected](P. Antonopoulos),[email protected](P. Smyrnelis).

http://dx.doi.org/10.1016/j.crma.2016.03.015

1631-073X/©2016Académiedessciences.PublishedbyElsevierMassonSAS.All rights reserved.

(2)

Theorem1.1.LetA

Rnbeanopen,connected,boundedset,with

A Lipschitz,andsupposethatv

( · )

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

minimizes J

(

u

;

A

)

subjecttoitsboundaryconditionson

A:

J

(

v

;

A

) =

min

{

J

(

u

;

A

) :

u

=

v on

A

}.

Then,ifthereholds

|

v

(

x

)

a

| ≤

r on

A,forsomer

>

0with0

<

2r

r0,therealsoholds

|

v

(

x

)

a

| ≤

r onA.

The scopeofthispaperistoestablishageneralizationofTheorem 1.1,by consideringpotentials W thatvanishatthe boundary ofaclosedconvexsetC0

Rm,whichiseitherC2 smooth orcoincideswithapoint

{

a

}

.Wementionthat the convexityassumptionisessentialforsimilarproblemsinvolvingsystemsofPDEs(cf.[6,12,13]).Assumingthat

(i) W

C1

(

Rm

;

R

)

,withW

C0

=

0,W

0 onRm

\

C0,

(ii) there existsr0

>

0 suchthat forevery outerunit normalvector

ξ

atthepoint p

C0 (

| ξ | =

1,ifC0

= {

a

}

):

(

0

,

r0

)

r

W

(

p

+

r

ξ )

isincreasing,andmoreoverW

(

p

+

r0

ξ ) >

0,

wecanstatethefollowingmaximumprinciple.

Theorem1.2.LetA

Rnbeanopen,connected,boundedset,with

A Lipschitz,andv

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

.Supposethat v minimizes J

(

u

;

A

)

subjecttoitsboundaryconditionson

A,

J

(

v

;

A

) =

min

{

J

(

u

;

A

) :

u

=

v on

A

} .

Then,ifthereholds

d

(

x

) :=

d

(

v

(

x

),

C0

)

r on

A

,

for some r

>

0with0

<

2r

r0

,

(2) whered istheEuclideandistance,therealsoholds

d

(

x

)

r on A

.

(3)

Moreover,theattainmentofequalityin(3)ataninteriorpointofA,1

d

x

) =

r

,

for somex

ˆ ∈

A

,

(4)

impliesthatd

(

x

) =

r,

x

A,andinadditionifC0isstrictlyconvex,v

(

x

)

constantinA.

Thefollowingextensionisalsotrue:

Theorem1.3.LetA

Rnbeanopen,connected,boundedset,with

A Lipschitz,andlet

DA

=

beaLipschitzportionof

A.As- sumethatv

( · )

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

minimizes J

(

u

;

A

)

subjecttoitsboundaryconditionson

DA:J

(

v

;

A

) =

min

{

J

(

u

;

A

) :

u

=

v on

DA

}

.Then,theconditiond

(

v

(

x

),

C0

)

r on

DA

,

0

<

2r

r0,impliesthesameconclusionsasinTheorem 1.2above.

Notethat thestrictmonotonicityassumption(b)inTheorem 1.1hasbeenweakened.Theorem 1.2isacorollaryofthe replacementresultestablishedinLemma 3.2below.Foru

( · )

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

,satisfyingtheboundarycondition (2),itisshownthat ifd

(

u

(

x

),

C0

) >

ronanon-negligiblesubset,thenthereexists amapu

˜

coincidingwithuon

A,and havinglessenergy.Toconstructthecompetitoru,

˜

weutilizethefollowingdecompositionofu:

u

(

x

) =

p

(

x

) + (

u

(

x

)

p

(

x

)),

(5)

where p

(

x

) :=

p

(

u

(

x

))

istheprojectionofu

(

x

)

ontoC0.Next,wedefinethedistancefunctiond

(

x

) :=

d

(

u

(

x

),

C0

) = |

u

(

x

)

p

(

x

) |

,andconsideradeformationofuoftheform:

˜

u

(

x

) =

p

(

x

) +

g

(

d

(

x

))(

u

(

x

)

p

(

x

)),

(6)

where g

:

R

→ [

0

, ∞)

is a suitable locallyLipschitzfunction. Wepoint out that theabove expression ofu

˜

by-passesthe difficultyencounteredin[1],whichutilizesthenormalvector:n

(

x

) :=

|uu((xx)−)aa| ifu

(

x

) =

a,andn

(

x

) :=

0 ifu

(

x

) =

a,andthe polarrepresentationsofu(respectivelyu):

˜

u

(

x

) =

a

+ |

u

(

x

)

a

|

n

(

x

)

(resp.u

˜ (

x

) =

a

+

f

(|

u

(

x

)

a

|)

n

(

x

)

),with f

:

R

→ [

0

, ∞)

, locallyLipschitz.Indeed,from(6),thecomputationof

|∇ ˜

u

|

iselementary.In addition,thedecomposition(5)allowsusto dealinoneshotwiththepointcase(where p

(

x

)

a,cf.Theorem 1.1),aswellaswiththecaseofsmoothconvexsets.

1 WeareindebtedtoA.Savas-Halilajforsuggestingtheuseoftheusualmaximumprincipleatthispoint.Thestrongmaximumprinciplepartofthe theoremfollowsfromtheusualmaximumprincipleasdevelopedin[12]and[13].

(3)

2. Comparisonwiththeusualmaximumprinciple

2Thetheoremsabovearedifferentfromtheusualmaximumprincipleinthefollowingrespects:

(a) W isnotconvex,hencetheusualmaximumprincipleisnotvalidevenforthescalarcasem

=

1;

(b) the monotonicity condition (ii) on W is extremely mild, andallows applicability in situations where degeneracy is natural(cf.[3]);

(c) theusualmaximumprincipleisacalculusfactandappliestoallsolutions.Thisisnottruefortheresultabove.

ConsidertheO.D.E.

u

W

(

u

) =

0

,

u

: R → R,

withW

: R → R,

W

(

u

) =

1

4

(

u2

1

)

2

.

(7)

Notice that (7) hasperiodic solutions forr

>

0 as small asdesired such that minRu

= −

1

+

r andmaxRu

=

1

r. By choosing A

= (

0

,

T

)

suchthatu

(

0

) =

u

(

T

) =

1

r,andC0

= {

1

}

,weseethatTheorem 1.1doesnotapplytothesesolutions.

Similarly, forthe potential H

(

u

) =

1

+

cos

(

πu

)

,andfor C0

= [

1

,

3

]

,the previous periodic solution u doesnot satisfy the maximumprincipleofTheorem 1.2.

ThefollowingexampleshowsthatTheorem 1.1doesnotapplyeventolocalminimizers(stablesolutionsto(1),defined intermsofthedefinitenessofsignofthesecondvariation).ConsiderthescalarP.D.E.

2

u

W

(

u

) =

0 in

,

u

n

=

0

,

(8)

whereW isasin(7)aboveand

isadumbbelldomain.Itiswellknown(cf.[5,9,10])thatfor

>

0 sufficientlysmall,(8) hasastablesolutionwhichon theleftandrightoftheneckisascloseto

1 and

+

1,respectively,asdesired(bytaking

>

0 sufficiently small).Bychoosing the set A

= \

B,with B

a closedball located on therightof theneck, and

DA

=

B,wecansecurethat

|

u

(

x

)

1

| ≤

ron

DA,andthereforeweseethatTheorem 1.3doesnotapply.

Thesolutionsto(1)forwhichTheorems 1.2 and1.3apply areusuallycalledminimal.Theyhavethepropertythatthey minimizethefreeenergywithrespecttotheirDirichletvaluesontheboundaryofanyopenboundedsubsetoftheirdomain ofdefinition.Thisisreminiscentofa familiarpropertyof minimalsurfaces.Thatitis sharedbythe minimalsolutions is notsurprising,sincethefunctional J islinkedtotheperimeterfunctionalifscaledappropriately.Moreprecisely,itiswell knownthattheGammalimit undera blow-downof J istheperimeterfunctional(cf.[11] forthescalarcase, and[2]for thevector),andthatthelevelsetsoftherescaledminimizersconvergetominimalsurfaces.

3. Proofofthemaximumprinciple

In what follows C0

Rm is a closed convex set, which is either C2 smooth orcoincides with a point

{

a

}

. We first compute

|∇ ˜

u

|

2 forthemapu

˜

definedin(6),utilizingthepropertiesoftheprojection p

(

x

)

.

Proposition3.1.Let A

Rn openandbounded,withLipschitzboundary,letu

(·)

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

,andletu

˜ (

x

) =

p

(

x

) +

g

(

d

(

x

))(

u

(

x

)

p

(

x

))

,where p

(

x

) :=

p

(

u

(

x

))

istheprojectionofu

(

x

)

ontoC0,d

(

x

) :=

d

(

u

(

x

),

C0

) = |

u

(

x

)

p

(

x

)|

,and g

:

R

→ [

0

,)

isalocallyLipschitzfunction.Then,u

˜ ( · )

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

,and

|∇ ˜

u

|

2

= |∇

p

|

2

+

f

(

d

)

2

|∇

d

|

2

+

g

(

d

)

2

|∇(

u

p

)|

2

− |∇

d

|

2

+

2g

(

d

)

n i=1

pxi

,

uxi

pxi

,

wherewehaveset f

(

s

) :=

sg

(

s

)

.Inaddition,if

|

f

| ≤

1and0

g

1,then

|∇ ˜

u

|

2

≤ |∇

u

|

2. Theproofofthemaximumprincipleisbasedonthefollowingcut-offlemma:

Lemma3.2.LetA

Rn,open,bounded,connected,with

A Lipschitz,andletW satisfyHypotheses(i),(ii)above.Supposethat u

(·)

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

.Ifthefollowingtwoconditionshold,

(I) d

(

x

) :=

d

(

u

(

x

),

C0

)

r on

A,0

<

2r

r0,

(II) Ln

(

A

∩ {

d

(

x

) >

r

}) >

0(Ln

(

E

)

,then-dimensionalLebesguemeasure), then,thereisu

˜ ( · )

W1,2

(

A

;

Rm

)

L

(

A

;

Rm

)

suchthat

2 WewanttothankProf.N.D.Alikakosforprovidingtheexamplesofthissection.

(4)

˜

u

=

u on

A

,

(9a)

d

˜ (

x

) :=

d

(

u

˜ (

x

),

C0

)

r

,

on A

,

(9b)

J

(

u

˜ ;

A

) <

J

(

u

;

A

).

(9c)

Proof. Case1.Wewillfirstestablishthelemmaundertheadditionalhypothesis:

d

(

x

)

r0

.

(10)

The argumenthereis easy sinceu stays inthe monotonicityregion of W about C0. Let f

(

s

) =

min

{

s

,

r

} =

g

(

s

)

s. Clearly,

|

f

| ≤

1 and0

g

1.ByProposition 3.1,u

˜ (

x

) =

p

(

x

) +

g

(

d

(

x

))(

u

(

x

)

p

(

x

))

satisfies

A

|∇ ˜

u

(

x

)|

2dx

A

|∇

u

(

x

)|

2dx

.

(11)

Havingacloserlookweseethatincaseofequalityin(11),then 0

=

A

|∇ ˜

u

|

2dx

A

|∇

u

|

2dx

A

|∇

d

|

2

((

f

(

d

))

2

1

)

dx

≤ −

A∩{d>r}

|∇

d

|

2dx

,

fromwhich itfollowsthat

d

=

0 a.e. onA

∩ {

d

>

r

}

,andtherefore

∇(

d

˜ −

d

) =

0 a.e. onA,where d

˜ (

x

) =

f

(

d

(

x

))

via(6).

Sinced

˜ −

d

W1,2

(

A

)

,we haveby connectednessd

˜ (

x

)

d

(

x

) =

constant a.e. in A,andfromd

˜ −

d

=

0 on

A inthesense of trace, we obtain d

˜ (

x

)

d

(

x

) =

0 a.e. inA, in contradictionto assumption (II) inLemma 3.2. Thereforewe havestrict inequalityin(11).

Ontheotherhand,since f

(

d

) =

g

(

d

)

d

d

r0,wehaveby(ii):

A

W

p

(

x

) +

g

(

d

(

x

))(

u

(

x

)

p

(

x

))

dx

A

W

p

(

x

) + (

u

(

x

)

p

(

x

))

dx

,

A

W

(

u

˜ (

x

))

dx

A

W

(

u

(

x

))

dx

,

henceCase1issettled.Noticethatinthiscasethestrictnessin(9c)wasobtainedviathegradientterm.

Case2.Assume

Ln

(

A

∩ {

d

>

r0

}) >

0

.

(12)

Considerthefollowingcut-offfunctions:

α (

s

) :=

⎧ ⎪

⎪ ⎩

1 fors

r

2rs

r forr

s

2r 0 fors

2r

,

f

(

s

) =

min

{

s

,

r

} α (

s

) =

g

(

s

)

s

.

Again,itisclearthat

|

f

| ≤

1 and0

g

(

s

)

1,thusu

˜ (

x

) =

p

(

x

) +

g

(

d

(

x

))(

u

(

x

)

p

(

x

))

satisfiesthankstoProposition 3.1:

|∇ ˜

u

(

x

)|

2

≤ |∇

u

(

x

)|

2

.

(13)

Wenote inpassingthat u

˜

isareflectionofualongd

(

u

,

C0

) =

r,andthus(13)isexpected.UnlikeinCase1,thestrictness oftheinequalityin(9c)willfollowfromthepotentialterm.Wewillneedthefollowingproposition.

Proposition3.3.(‘Continuity’ofSobolevfunctions,cf.[4].)LetA

Rn,open,boundedandconnected,withLipschitzboundary,and assumethatf

W1,2

(

A

;

R)satisfies

f

≤ ˆ

r on

A (in the sense of trace) andLn

(

A

∩ {ˆ

s

<

f

} ) >

0for somer

ˆ < ˆ

s

.

(14) Then,Ln

(

A

∩ {ˆ

r

<

f

≤ ˆ

s

} ) >

0.

Proof. Let

σ , τ :

A

Rbedefinedby

σ (

x

) =

min

{

f

(

x

), ˆ

s

} =

f

(

x

)

forx

E1

:=

A

∩ {

f

≤ ˆ

r

} ˆ

s forx

E3

:=

A

∩ {ˆ

s

<

f

}, τ (

x

) =

max

{ σ (

x

),

r

ˆ } =

r

ˆ

forx

E1

ˆ

s forx

E3

.

(5)

Suppose,for thesake ofcontradiction, that Ln

(

A

∩ {ˆ

r

<

f

≤ ˆ

s

} ) =

0.Therefore,

τ

is astep function.Thus

τ =

0 a.e.

in A.Ontheotherhand,

σ

,

τ

areinW1,2

(

A

;

R)(cf.[8,p.130]).Thisandtheconnectednessof Aimplythat

τ ≡

constant (cf.[7, p.307]). Hence

τ ≡ ˆ

s since Ln

(

E3

) >

0. Itfollows thatLn

(

E1

) =

0 and f

>

s

ˆ

a.e. in A. Thus, f

≥ ˆ

s on

A inthe senseoftrace,whichiscontradicting(14).Theproofiscomplete. 2

Conclusion:Let

>

0 suchthatW

(

u

) >

0 onr0

d

(

u

,

C0

)

r0

+

.Wedefinethesets E1

:=

A

∩ {

d

r0

},

E2

:=

A

∩ {

r0

<

d

r0

+ },

E3

:=

A

∩ {

d

>

r0

+ }.

From (12), we obtain that in the event that Ln

(

E2

) =

0, then necessarily Ln

(

E3

) >

0. But d

r

<

r0 on

A, hence by Proposition 3.3:

Ln

(

E2

) >

0

.

(15)

Therefore,(15)holdsunderanycircumstances.On A

∩ {

0

d

2r

}

wehave:

W

(

u

˜ (

x

)) =

W

p

(

x

) +

g

(

d

(

x

)(

u

(

x

)

p

(

x

))

W

p

(

x

) + (

u

(

x

)

p

(

x

))

=

W

(

u

(

x

)),

since g

(

d

)

d

=

f

(

d

)

d

2r

r0. On the other hand, on A

∩ {

d

>

2r

}

we have 0

=

W

(

u

˜ (

x

))

W

(

u

(

x

))

, while on E2: 0

=

W

(

u

˜ (

x

)) <

W

(

u

(

x

))

.Therefore,wehave J

u

;

A

) <

J

(

u

;

A

)

andtheproofofLemma 3.2iscomplete. 2

NowtheproofofTheorem 1.2isstraightforward.

ProofofTheorem 1.2. Weproceedbycontradiction.Sosupposethat(3)doesnothold,henceLn

(

A

d

(

v

(

x

),

C0

) >

r

} ) >

0.

ButthiscontradictstheminimalityofvbyLemma 3.2.Thus(3)holds.Next,suppose(4)holdsandnoticethatd2

=

d2

(

v

,

C0

)

satisfies

(

d2

)(

x

) =

2d

(

x

)

d

(

x

),

W

(

v

(

x

)) +

n i=1

D2

(

d2

)(

v

(

x

))(

vxi

(

x

),

vxi

(

x

))

0

,

foreveryx

Asuchthat0

<

d

(

v

(

x

),

C0

)

r0,thankstoHypothesis(ii)onW,totheconvexityofthefunctionu

d2

(

u

,

C0

)

inthecomplementofC0,andtothefactthattheminimizervsolvessystem(1).Bythestrongmaximumprinciple,itfollows thatd

(

v

,

C0

)

isconstantin A.Inaddition,ifC0 isstrictly convex,thenthefunction u

d2

(

u

,

C0

)

isstrictlyconvexinthe complementofC0.Thisimpliesthat

(

d2

)(

x

) |∇

v

(

x

) |

2

,

x

A

:

0

<

d

(

v

(

x

),

C0

)

r0

,

forsome

>

0.Thus,

v

0 sinced

(

v

,

C0

)

isconstant,andasaconsequencev isconstantin A. 2

ProofofTheorem 1.3. First we note that if in Lemma 3.2, specificallyin condition (I), one replaces

A with

DA, then the sameconclusion (9)holds,where

A isnow replacedwith

DA. Theargumentis completelyunaltered. Similarly,in Proposition 3.3,

A isreplacedwith

DA,withoutchangeintheproof.TheproofofTheorem 1.3iscomplete. 2

Acknowledgements

PanayotisSmyrneliswaspartiallysupportedbyFondoBasalCMM-Chile,FONDECYTpostdoctoralgrantNo.3160055,and through theproject PDEGE PartialDifferential Equations Motivatedby Geometric Evolution, co-financedby the European Union European Social Fund (ESF) and national resources, in the framework of the program Aristeia of the Operational ProgramEducationandLifelongLearningoftheNationalStrategicReferenceFramework(NSRF).

References

[1]N.D.Alikakos,G.Fusco,Amaximumprincipleforsystemswithvariationalstructureandanapplicationtostandingwaves,J.Eur.Math.Soc.17 (7) (2015)1547–1567.

[2]S.Baldo,MinimalinterfacecriterionforphasetransitionsinmixturesofCahn–Hilliardfluids,Ann.Inst.HenriPoincaré7 (2)(1990)67–90.

[3]J.M.Ball,E.C.M.Crooks,Localminimizersandplanarinterfacesinaphase-transitionmodelwithinterfacialenergy,Calc.Var.PartialDiffer.Equ.40 (3–4) (2011)501–538.

[4]H.Brézis,FunctionalAnalysis,SobolevSpacesandPartialDifferentialEquations,Universitext,Springer-Verlag,NewYork,2011.

[5]R.G.Casten,C.J.Holland,Instabilityresultsforreaction-diffusionequationswithNeumannboundaryconditions,J.Differ.Equ.27(1978)266–273.

[6]L.C. Evans, A strongmaximum principlefor parabolicsystems inaconvexset witharbitrary boundary,Proc. Amer.Math. Soc. 138 (9)(2010) 3179–3185.

[7]L.C.Evans,PartialDifferentialEquations,secondedition,GraduateStudiesinMathematics,vol. 19,AmericanMathematicalSociety,2010.

[8]L.C.Evans,R.F.Gariepy,MeasureTheoryandFinePropertiesofFunctions,CRCPress,BocaRaton,FL,USA,1992.

[9]R.V.Kohn,P.Sternberg,Localminimisersandsingularperturbations,Proc.R.Soc.Edinb.,Sect.A111 (1–2)(1989)69–84.

[10]H.Matano,Asymptoticbehaviorandstabilityofsolutionsofsemilineardiffusionequations,Publ.Res.Inst.Math.Sci.15 (2)(1979)401–454.

(6)

[11]L.Modica,S.Mortola,Unesempiodi-convergenza,Boll.UnioneMat.Ital.,B14 (1)(1977)285–299.

[12]H.Weinberger,Invariantsetsforweaklycoupledparabolicandellipticsystems,Rend.Mat.Ser.VI8(1975)295–310.

[13]H.Weinberger,Someremarksoninvariantsetsforsystems,in:P.W.Schaefer(Ed.),MaximumPrinciplesandEigenvalueProblemsinPartialDifferential Equations,in:PitmanResearchNotesinMathematics,vol. 175,Longman,1988,pp. 189–207.

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