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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
baDepartmentofMathematics,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 suchthatforeveryξ ∈
Rmwith|ξ| =
1:(
0,
r0)
r→
W(
a+
rξ )
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.
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 normalvectorξ
atthepoint p∈ ∂
C0 (| ξ | =
1,ifC0= {
a}
):(
0,
r0)
r→
W(
p+
rξ )
isincreasing,andmoreoverW(
p+
r0ξ ) >
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,therealsoholdsd
(
x) ≤
r on A.
(3)Moreover,theattainmentofequalityin(3)ataninteriorpointofA,1
d
(ˆ
x) =
r,
for somexˆ ∈
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].
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) =
14
(
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)
suchthat2 WewanttothankProf.N.D.Alikakosforprovidingtheexamplesofthissection.
˜
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))
satisfiesA
|∇ ˜
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
≤
r2r−s
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)satisfiesf
≤ ˆ
r on∂
A (in the sense of trace) andLn(
A∩ {ˆ
s<
f} ) >
0for somerˆ < ˆ
s.
(14) Then,Ln(
A∩ {ˆ
r<
f≤ ˆ
s} ) >
0.Proof. Let
σ , τ :
A→
Rbedefinedbyσ (
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),
rˆ } =
rˆ
forx∈
E1ˆ
s forx
∈
E3.
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 Aimplythatτ ≡
constant (cf.[7, p.307]). Henceτ ≡ ˆ
s since Ln(
E3) >
0. Itfollows thatLn(
E1) =
0 and f>
sˆ
a.e. in A. Thus, f≥ ˆ
s on∂
A inthe senseoftrace,whichiscontradicting(14).Theproofiscomplete. 2Conclusion: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)) =
Wp
(
x) +
g(
d(
x)(
u(
x) −
p(
x))
≤
Wp
(
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. 2NowtheproofofTheorem 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=1D2
(
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. 2ProofofTheorem 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. 2Acknowledgements
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).
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