A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
M. C ARRIERO A. L EACI
S
k-valued maps minimizing the L
pnorm of the gradient with free discontinuities
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 18, n
o3 (1991), p. 321-352
<http://www.numdam.org/item?id=ASNSP_1991_4_18_3_321_0>
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Maps Minimizing
the
Gradient with
FreeDiscontinuities
M. CARRIERO - A. LEACI
1. - Introduction
In this paper, we
study
two new variationalproblems involving S’-valued
maps, where
S k = ~ z
ER~+’; I z = 1 } .
We dealwith free discontinuity problems
since a solution is a
pair (K, u),
where K is a(a-priori unknown)
closed setand u is a map
suitably
smooth outside of K(see [11]).
Theseproblems
canbe
regarded
as apossible
schematization ofproblems
in mathematicalphysics
in which both volume forces and surface tensions are present.
In the scalar case,
recently
two freediscontinuity problems
have beenstudied
by
E. DeGiorgi
and the authors in[13], [9].
The main theorem in[13]
can be seen as an existence and
partial regularity
result for aNeumann-type problem,
whereas in[9]
we consider aDirichlet-type problem.
’The main results of this paper are
presented
in Theorems4.1,
4.10 and 5.4. Forbrevity’s
sake here we illustrateonly
asimplified
version of these results.NEUMANN-TYPE PROBLEM. Let n > 2, let SZ C bounded
open set and kEN. Assume that g E
Then, for
every p > 1 and q > 1, there exists at least onepair (Ko, uo) minimizing
thefunctional
in the class
of
the admissiblepairs (K, u)
with K c closed andu E
Sk).
Moreover,for
everyminimizing pair (Ko, uo),
thesingular
setK6
n SZ is( ~l n-1,
n -1) rectifiable
and thereexists 61
1 > 0 such thatfor
every essentialminimizing pair (K’, u’) (see
Remark4.6)
we havePervenuto alla Redazione il 20 Aprile 1990 e in forma definitiva il 23 Novembre 1990.
and
for
every compact setQ
C K’ n Q.DIRICHLET-TYPE PROBLEM. Let SZ c be a bounded open set with
c1 boundary
and let w be a,S’’~)
map. Thenfor
every p > 1 there exists at least onepair (.Ko, uo) minimizing
thefunctional
in the class
of
the admissiblepairs (K, u)
with K C R7closed,
such that u = w in
9QBK.
Moreover theproperties ( 1.1 )
and(1.2),
even at theboundary points,
holdfor
every essentialminimizing pair
While the passage from the case of a scalar function u considered in
[13]
and
[9]
to the case of a vector function u without constraints does not present anyproblem,
the introduction of theconstraint lul
= 1 forcesmeaningful changes
in the
proofs.
The interest inconsidering
such a constraint is connected to recent studies on minima of non-convex functionals and onpossible applications
ofthese studies to the
theory
ofliquid crystals.
In order to prove the above cited theorem for the
Neumann-type problem,
we take into account the idea of the so-called direct methods in the Calculus of Variations. Therefore we
join
to the functional to be minimized a newfunctional defined on a class of
special
functions of bounded variation(the
class
SBV(Q; Sk)),
where a suitabletopology
can be found such that the newfunctional is both lower semicontinuous and coercive. Then Theorem 4.1 and Theorem 4.10 are established
by proving
first the existence of a solution for aminimum
problem
for the new functional in the classSBV(Q; (see
Lemma4.3)
and afterby proving
that the minimum of the new functional is also the minimum of ouroriginal
functional. The same method and further estimatesnear the
boundary points
allow us to solve aDirichlet-type problem (Theorem 5.4).
The
plan
of theexposition
is thefollowing.
In the second section we recall the definition and some
properties
of theclass
SBV(Q)
and weadapt
some resultsproved
in[13], [9]
to the case ofvector valued functions considered here. In
particular
we state the Poincar6-Wirtinger type inequality (Theorem 2.5)
which is an essential tool in the restof this paper.
The third section is devoted to the
study
ofproperties
ofquasi-minima
inSBVioc(Q; Sk)
of some newintegral
functionals. In Theorem 3.6 westudy
thebehaviour of
blow-up
sequences. The lack ofconvexity
of the target space forcesus to
modify
the arguments used in[13], [9] (see
Lemma3.5).
In Theorem3.11 we prove some
properties
of thesingular
sets ofquasi-minima.
In the fourth section we prove the existence theorem for a
Neumann-type problem by using
the direct methods in the Calculus of Variations and thepartial regularity properties
estabilished in Theorem 3.11. In Lemma 4.9 and Theorem 4.10 we prove some resultswhich,
among otherthings,
can be usefulto
approximate
the functionals that we considerby elliptic
ones, more suitable innumerical
computations.
In the scalar case thisapproximation
has beenalready
obtained in
[6].
In the fifth section we sketch the
proof
of the existence theorem for aDirichlet-type problem (Theorem 5.4).
For a
comparison
with other variationalproblems
that deal withseeking
a
minimizer,
under suitableconditions,
of the energyin the Sobolev space
W1,2(Q; Sk),
we mention a few results from thelarge
literature on this
topic.
We recall that such
problems
appear both in thestudy
of harmonic maps(see [27], [28], [14])
as in thetheory
ofliquid crystals (see [10], [15], [22], [30]).
The minimizers are, ingeneral, singular and, according
to the worksof R. Schoen and K. Uhlenbeck
[27], [28]
and also of M.Giaquinta
and E.Giusti
[17],
thesingular
set has Hausdorff dimension at most(n - 3)
and it is discrete for n = 3.Moreover,
in the case n = 3 and k = 2, H.Brezis,
J.M. Coron and E.H. Lieb[8]
have shown that the minimizers map smallspheres
aroundany
singular point
intoS2
withtopological degree plus
or minus one. Thesingularities
appear notonly
fortopological
reasons, but becausethey
enableto reduce energy.
Actually,
R. Hardt and F.- H. Lin[24]
have shownthat,
in
general,
a Lavrentievphenomenon
does occur. As a furtherstep
towards anunderstanding
of thegeometry
of energy minimizers F.J.Almgren
and E.H. Liebhave estimated in
[2]
the number ofpoints
ofdiscontinuity
which a minimizercan have.
In the static
theory
ofliquid crystals
a nematicliquid crystal
is a fluidin a container
S2,
which is formedby
rodlike molecules whose directions arespecified by
a unit vector field(the
map u : Q CJR.3 ~ S2),
these directionsare fixed
along
theboundary
and theconfiguration
assumes aposition
whichminimizes the Oseen-Frank functional
(see
J.L. Ericksen[15]).
The harmonic maps appear as models for the director of a nematicliquid crystal
withequal
Oseen-Frank constants. The results of
[17], [27], [28]
have beengeneralized
tothe case of the Oseen-Frank functional
by
R.Hardt,
D. Kinderlehrer and F.-H.Lin
[22]
and in the case of maps that minimize the LP norm of thegradient
for p > 1
by
R. Hardt and F.-H. Lin[23].
Another
approach
to thestudy
of the energy of maps from Q cJR.3
toS2
has been
proposed
in[7]
with the introduction of a relaxed energy and in[19], [20]
in which smooth functions areregarded
asgraphs,
or, moreprecisely,
ascartesian currents. In these contexts the minimizers
have,
ingeneral, singularities
of Hausdorff dimension at most one.
In the case of the free
discontinuity problems
which we deal withhere,
we prove that the essential
minimizing pairs
have asingular
setwhich,
if notempty,
has Hausdorff dimensionequal
to(n -1 ) (see
Lemma 4.9 or the property( 1.1 )).
It is well-known that for n > 3 the mapuo(y)
=y
is a minimizer inY
1,21 }
forf /V’u/2dy
over the class ofall W1,2
maps withB,
lul =
1 andboundary
dataw(y)
= y(the identity
map on8Bi)
andobviously
itshows an isolated
singularity
at theorigin.
We remark that thepair ({0},~o)
isnot a solution of the
Dirichlet-type problem
withboundary
dataw(y)
= y for thefunctional,
hereconsidered,
Indeed, if we define for 0 r 1
then
It is an open
problem
to describe thegeometric
structure of thesingular
set of an essential
minimizing pair.
In the scalar case we refer to[11] ]
for some relatedconjectures which,
at ourknowledge,
are still open.Aknowledgement.
We would like to thank Prof. E. DeGiorgi
for manyhelpful
conversations on thesubject
of the present paper.2. -
Preliminary
results for functions inGiven an open set Q C Rn, we
define, following [12],
the class ofspecial
functions of bounded variation and we
point
out a few of itsproperties.
_For a
given
set E c R7 we denoteby
xE its characteristicfunction, by
Eits
topological
closure andby
aE itstopological boundary;
moreover we denoteby
its (n -I)-dimensional
Hausdorff measure andby JEJ
itsLebesgue
outer measure.
If Q, Q’
are open subsets in R~, with Q cc Q’ we mean thatQ
is compact and Q c S2’ .We indicate
by BP(x)
the ball{y
E R7;ly - x p},
and we setBp
=Bp(O),
wn
= By (eB ..., en )
we denote the canonical base of R7 andby (e 1,
..., 8"~) thecanonical
base of Let u : S2 --~ R!l be a Borelfunction;
for x andz E U
{oo} (the
onepoint compactification
ofW’)
we say(following [12])
that z is theapproximate
limit of u at x, and we writeif
for every g E this definition is
equivalent
to other onesexisting
in theliterature
(e.g.
2.9.12 in[16]).
The set
is a Borel set, of
negligible Lebesgue
measure; forbrevity’s
sake we denoteby
u :
im
the functionLet x e be such that
u(x)
E we say that u isapproximately
differentiable at x if there exists a linear map
(the approximate
differential of u at
x)
such thatIf u is a smooth function then Vu is the differential. In the
following
with thenotation
we mean the euclidean norm of Vufor almost all x E S2.
Now we recall some
properties
related to scalar valued functions.For every u E we define
(see [25])
By BV(Q)
we denote the Banach space of all functions u ofL1(Q)
withf I D2c
+00.Q 0
It is well-known that u E
BV(Q)
iff u E and its distributional derivative Du is a bounded vector measure. For the mainproperties
of thefunctions of bounded variation we refer e.g. to
[16], [21], [25].
Here we recall
only
that for every u EBV(Q)
thefollowing properties
hold:
Vu exists a.e. on Q and coincides with the
Radon-Nikodym
derivative of Du withrespect
to theLebesgue
measure(see [16], 4.5.9(26));
for
)In-1
I almost all xE ,Su
there exist v = EaB1, u+(x)
C R andu-(~)
G R(outer
and inner trace,respectively,
of u at x in the directionv)
such that
r r
and
(see [16], 4.5.9(17),(22),(15)).
Following [12],
we define a class ofspecial
functions of bounded variation which are characterizedby
a property stronger than(2.1).
DEFINITION 2.1. We define
SBV(Q)
as the class of all functionssuch that
We remark that the well-known Cantor-Vitali function has bounded
variation,
but it does notsatisfy (2.2).
REMARK 2.2. Let u E
BV(Q)
and set ua =(u
Aa)
V(-a)
for a E(0, +oo).
The
following properties
hold:Moreover,
for u EBV(Q),
it holds:and more
generally:
Lipschitz
continuous with0(0)
= 0.Denote
by (p
>1)
the Sobolev space of functions u ELP(Q)
suchthat Du E
LP(Q; R7);
then we remarkthat,
for u ESBV(Q),
(see
e.g.[16], 4.5.9(30)).
For further results on the functions in
SBV(Q)
we refer to[12], [3], [4], [5].
In this paper we deal with functions in the space
SBV(Q; R!),
i.e. functionsu : Q - whose
components ui (i
=1, ... , m)
are functions inBy SBVI,,C (K2; Wn)
we denote the space of all functions whichbelong
tofor every open set Q’ cc SZ. For every u E
SBV(Q; R!n)
thefollowing properties
hold
(see [3], [4]):
three Borel functions
exist, v
u- : R!n, such that for all x
E Su
c)
for all xc Su
thetriple (u+(x), u- (x), v(x))
isuniquely
determined up to a
permutation
of and achange
ofsign
of v(x). In
particular,
for every u E and LEMMA 2.3. Letbe closed and assume u E and
Then
(i)
2G E(ii) Su
rl Q c K,(iii)
three vector-valued Borelfunctions, u+,
u- and v, exist which aredefined )In-1-a.e.
on K n SZ andsatisfy (2.3)-(2.4).
We note
only
that(i)
and(ii)
areproved
in Lemma 2.3 of[13]
for m = 1 and that(iii)
followsby
thepreceding
propertyb) setting u+(x)
=u-(x)
= u(x) for x EKBSu
and v anarbitrary
constant direction onKBSu.
In this paper we use the
following
compactness theorem inSBV(Q; JRm),
that is an obvious consequence of a result
by
L. Ambrosio(see
Theorem 2.1 of[4]).
THEOREM 2.4. Let p > 1, n E
N,
n >2,
S2 c open, LetQ
c JRm be a compact set and let(Uh)
C be a sequence such that1
and
Uh(X)
EQ for
almost all x E Q. Then there exists asubsequence converging
in measure to afunction
u ESBVioc(Q;Rm)
withu(x)
EQ for
almost all x E Q.
We remark that the conclusions
just
asserted do not follow if p = 1, because in this case it ispossible
toapproximate
every u Eby
asequence of smooth functions
(which
are also functions of classSBV(Q; JRm)).
In
[13],
section3,
aPoincare-Wirtinger type inequality
for scalar valued functions of the class SBV in a ball and two consequences have beenproved.
Here we
give
the statements ofanalogous
results for the vector valued case.The
proofs
are omitted becausethey
aresimple generalizations
of thosegiven
in
[13].
Let B be a ball in > 2; for every measurable function u : B --+ JRm with u =
(u 1, ... , U m)
and for 05
we setwhere
We define
moreover, for every u E such that
we set ,
where -1,,
is theisoperimetric
constant relative to the balls of R~.In the
following, given
a, b E JRm we poseand
THEOREM 2.5. Let
I
, and
Then
We remark
that, by
thedefinition,
THEOREM 2.6. Let B c R7 be a
ball,
p > 1, and let
Then a
subsequence (uh~ )
and afunction
for
everymoreover
and
then
3. - A limit theorem and some estimates for
quasi-minima
inS).
Assumptions.
In this section we will assume n n >2, mEN,
m >
2,
p >1,
Q c JRn open subset.Let 1: (0,+oo)
be a Borel function with theproperty
that there exist two constants ao, a 1 such that
for every be
positively
0-ho-mogeneous.
DEFINITION 3.1. Let / We set
) and c > 0. Let
Q
c Q be closed.For
every t
> 0 and for every u suchthat Jul
= t a.e. inQ,
we setmoreover, if , we set
We first state three technical lemmas, whose
proofs
arestraightforward.
LEMMA 3.2. Let u E For every c > 0 and t > 0 the
functions
are
non-decreasing
in(0,
r) andWe remark
only
that thepreceding inequality
followsby choosing
theadmissible function
LEMMA 3.3. Let u E with
lul =
t a.e. inB,(xo).
Forp E
(0, r)
andfor
every x EBr/p
setup(x)
=pO-p)/p u(xo
+px),
thenand
LEMMA 3.4. Let 1
Suppose
Set
then
Now we prove the
following
lemma.LEMMA 3.5. Let t >
0,
E E(0, 1 );
letQ, Q’,
Q" be open setssuch
that S2 cc Q’ cc Q". Let u E with
lul =
t a.e. in92"B?Y,
um >
( 1 - E)t
a. e. inK2’,
and let v EW 1,P(Q";
with( 1 - E)t
a. e. in Q".Then
a function
w ESBVIO, (K2"; JRm)
exists with t a. e. inK2",
w = u a. e.in
S2"B
SZ’ and such that,for
every c > 0,where nE E Nand
PROOF. Let
P(z)
= for every z E Fixed E > 0, let n, E N be such that2P-1/nf
E; letSZi (i = 1,..., n,)
be open sets of Rn such that Q CC SZ1 CC ... CCQn! =
Q’ anddist(Qi,
=dlnf (i = 1, ... ,
nf -1).
Let ~pi E
with
0 ~pi1,
~Z - 1 in aneighbourhood
ofSZi
andI 2nE/d. Setting
wi= P((1 -
+ we have wi ESBVI,,(Q";
(see [5]),
wi = u a.e. inIWi = t
a.e. inS2",
and
then it follows that
Therefore a suitable function wi exists such
that, setting w
= wi, we haveThen the thesis follows
immediately. q.e.d.
We are now in a
position
to prove thefollowing
limit theorem.be such that
for
almost allThen there exists a
hyperplane I
such that theimage of
liesessentially
in E; moreover the
function
u~ isp-harmonic
inBr (x) (i. e.
it minimizes thefunctional j I Vu lpdy
in +W¿’P(Br(x); JRm))
andB,(x)
for
almost all p r.PROOF. We may assume that x = 0, sup
a(p)
+oo and moreover, up topr
rotations,
thatmed(uh, Br) =
withAh
> 0. From theassumptions (3)
and(1),
it follows thatso
that, by
Theorem2.6,
The
proof
will becompleted by proving
that theimage
of liesessentially
in the
hyperplane {~
E R!I; zm =01,
i.e.and that, for almost all p r and for every v E v = in
BrBBp,
it follows
We prove
(3.1 )
with an argumentanalogous
to that used in[22]
forproving
Lemma 2.1. In the
following
with A we denote ageneric positive
constant,which does not
depend
on h. Becausesetting
we haveBy
Theorem 2.5 and thesubsequent remark,
we havewhere,
without loss ofgenerality,
we have assumed p n. Therefore we haveand, possibly by
restriction to asubsequence,
we may supposeBy using
the trivialidentity
we haveand also
Then, letting h -
+oo,by
thehypothesis (5)
andby (3.3)
we obtain0 + em = 2d a.e. in
Br,
so thatFinally
we deduce 0 a.e. inBr.
Now we show
(see
next(3.5))
that is the limit in of asequence of functions which are obtained
by uh - med(uh, Br)
under suitable truncations.Fixing
E E(o,1 ),
we definewhere u i are defined as in Theorem 2.5 and
By (3.3)
we havedefinitively
and
by
Theorem 2.6 it followsMoreover,
by
Theorem2.5,
we havedefinitively,
for h such thatB tfr J
Multiplying by
ch thepreceding inequality
andby
thehypothesis (1),
we obtainBeing possibly passing
to asubsequence,
we obtainfor almost all p r.
Finally
we may prove(3.2) by
contradiction.By (3.1)
we may assume, without loss ofgenerality,
that v~ - 0 a.e. inBr.
Since the function p -
a( p)
isnon-decreasing,
it is also a continuousfunction for almost all p r. Let
p’
r such that a(.) is continuousin p’
andthe
hypothesis (3)
is fulfilled.We
suppose that a function v exists such thatv C = U,,,, in
BrBBp’
and for > 0Let now p > 0 be such
that p’
p r anda(-)
be continuous in p, let thehypotheses (3), (4)
and the condition(3.6)
be fulfilled and moreoverBy using
the functions definedby (3.4)
we setBy
Lemma 3.4 andby (3.6)
it followsBy
Lemma 3.5applied
to the functionsuh
andv + Àhêm
for hlarge enough
weobtain a sequence of
functions
wh E such thatlwhl =
th a.e. inBr,
wh = uh a.e. inBrBBp
and moreover, for a nE EN, nE >2P-1jE,
Since
letting h -
+oo,by
thehypotheses (3)
and(4)
andby
the conditions(3.5), (3.7)
and(3.8)
we obtainhence,
because of the arbitrariness of E,and this is a contradiction because the
function p - a(p)
isnon-decreasing.
and
>
for
almostall ,
Under these conditions, the conclusion
of
Theorem 3.6 remains valid.PROOF. We may assume that x = 0. If
limsupAh =
+00 the assertionh
follows
by
Theorem 3.6. Iflim sup A h
+00,setting
h
we have +oo and also 0.
Indeed,
for hlarge enough,
h h
Passing
to thelimit, by
theassumption (1),
thepreceding
assertionfollows.
We note that
and that for h
large enough
Hence,
by
theassumptions ( 1 )
and(3),
we obtain lim hl(uh,
Ch,Bp) = a(p)
for_
almost all p r. In the same way we obtain also h Ch,
Bp)
= 0. Thenthe assertion follows
by
Theorem 3.6.q.e.d.
In the next Lemma 3.9 we shall use a result which is
proved
in a moregeneral
situation in[29] (see
the Theorem in page244).
THEOREM 3.8. Let u E be
p-harmonic
in Q. Let Br be a ball with r E(0,
1 ] such that Br C Q. Then there exists apositive
constant co whichdepends only
on n, m and p such thatLet k G N, we define
LEMMA 3.9.
(Decay lemma).
For every a E(0, 3 ], fl
E(0, 1 ),
such thata!3 l/co(wn
+1)2P-1,
andfor
every c > 0, there exist threepositive
constantsE, {) and r,
depending
on n,k,
p, c, ao, a 1, a and{3,
such that:if
S2Rn is open, p E(0,
r],Bp(x)
c Q andif
u ESBYIoc(SZ; Sk)
withand then
PROOF.
Suppose
the lemma is not true. Then there exist n > 2, a e(o, 2/3], ,3
E(0, 1),
such thata!3 11CO(Wn
+1)2P-1,
c > 0, three sequences(Ch), (’Oh)
and(ph)
such thatliM Ch
= =lim ph
= 0, a sequence(uh)
inSk)
andh
_
h h
a sequence of balls
B Ph (Xh)
C Q, such thatand
For
each h, translating
Xh into theorigin
andblowing
up, i.e.setting
where
we
have, by using
Lemma3.3,
and also
By
Theorem2.6,
there exist asubsequence
of(Vh),
still denotedby (Vh),
and afunction Voo E such that = a.e. in Bl. In
h
order to use
Corollary
3.7 we prove that = 0. We may assume p n, hso that q =
p*. Then, recalling
that 7 = 03C8 + (D,by using
Lemma 3.2 we haveconst > 0 and
By Corollary
3.7 we argue that the function isp-harmonic
in B1 and thatmoreover
By
Theorem 3.8 we havewhereas
by (3.9)
we haveObviously
if in Lemma 3.9 we suppose inplace
of
EPpn-1
then the same thesis holds. Henceby
an iterationargument as in
[13],
Lemma 4.10 and 4.11, we obtain thefollowing
result._
LEMMA 3.10. Let cx,
fl,
c, E, ~9 and r be as in Lemma 3.9. Let p E(0,
r],BP(x)
C Sz and u ESBVioc(Q; Sk).
Assumemoreover, assume that
Then
Finally
we prove apartial regularity
theorem for functions in the space whichsatisfy
thequasi-minimum
condition(3.10).
THEOREM 3.11. Let c > 0 and let u E
SBVioc(Q; Sk).
Assume thatfor
every compact set
Q
c Q,l(u,
c,Q)
+oo and moreover thatPROOF. Let x E
Qo
and let a,(3,
E, ?9 and r be as in Lemma 3.9.By
thedefinition of
Qo
andby (3.10),
there exists apositive
p1 dist(x, 8Q)
A r suchthat
and
for every and for every Then we infer that
for every y E
By
Lemma 3.10 we conclude thatBpl2(X)
CQo.
ThusQo
is an open set.By
Theorem 2.7 wehave Su
c and so cFinally (ii)
followsby
acovering
argument(see
e.g. Lemma 2.6 in[13]).
q.e.d.
4. - A
Neumann-type problem
Let n > 2, let Q C be a bounded open set, let k Ei N and p > 1.
To
begin,
we consider the class of the admissiblepairs
We note that if
(K, u) by
Lemma 2.3 it follows thatand that three vector-valued Borel functions
u+, u-, v
exist which are definedon K n Q and
satisfy (2.3), (2.4).
Let 0 :
: x R7 ,[0, +too)
be a function suchthat 0
is lowersemicontinuous,
for
every u EI~k+1
let0(u, .)
be convex andpositively ]-homogeneous,
and moreover let two constants ao, a 1 exist such that 0~(u, v)
alfor
every u EJRk+1, v
Csn-1
and’lj;( . , v) be positively 0-homogeneous.
We definefor every
The main result of this section is the
following
existence theorem.THEOREM 4.1. Let n E N, n > 2, let S2 c R7 be a bounded open set and Assume that g E let I be
given by (4.1 ).
Thenfor
every p > 1, q > 1, A > 0 > 0 apair (Ko, uo)
c A exists such thatwhere
We prove this result
by
the direct methods in the Calculus of Variations.We shall use the
following semicontinuity
resultproved
in[4], (see
Theorem 3.6 and Section5.1 ).
THEOREM 4.2. Let 1 be
given by (4.1 ).
Thenfor
every p > 1,for
everysequence
(Uh)
C nconverging
in tou E
SBV(Q;JRk+1)
andsatisfying
the condition +00, thefollowing
h
inequality
holdsNow we introduce a new functional defined for every u E
SBV(Q; Sk ) by
First we prove that at least one minimizer of the functional
g
exists inSBV(Q; S k).
LEMMA 4.3. Under the
hypotheses of
Theorem 4.1, there existsand it is smaller
than,
orequal
to,PROOF. Let
(uh)
CSBV(Q; S)
be aminimizing
sequence for~C.
Sinceand
we conclude
By
the compactness theorem in(see
e.g.[21],
Theorem1.19),
there are a
subsequence,
still denotedby (uh),
and a function w Esuch that in
ll~k+1). By
Theorem 2.4 w ESBV(Q; ,Sk) and, by
Theorem
4.2,
thus w is a minimizer
for g
inSBV(Q; Sk).
By
Lemma2.3,
if(K, u)
C .~ then u CSBV(Q; and Su
n Q c K, hence we inferLEMMA 4.4.
-Under
thehypotheses of
Theorem_4.1, if
w is a minimizerof
the,functional g
inSBV(Q; Sk),
thenfor
everyBp(x)
c SZ thefollowing
estimates hold
and
PROOF. Let of w we have
vith v = w in
QBBp(x). By
theminimality
thus,
because of the arbitrarinessof v,
we infer(4.2). Choosing
we deduce
(4.3). q.e.d.
_Now
we state someregularity properties
for a minimizer of the functio- naly.
LEMMA
4.5. Under
thehypotheses of
Theorem 4.1 andif
w is a minimizerof
thefunctional y
inSBV(Q;
thenwhere,
for
every PROOF. Let of the functionaland it is a minimizer
,- , ,- ..
among the functions u in w +
Sk). By
theinequality (4.3)
andby
Theorem 3.5.2 of[26]
we have 16 e To infer theC1
1regularity
of w near thepoint
x, we assumew(x)
= and choose 0p’
p so thatw(Bp/(x))
is contained inSk
nB1/2(êk+1).
Then we may, inBp,(x),
substitutein the functional
(4.4)
to infer that(iV-1, ... , Zk)
is a local minimizer in of the functionalWe now may
adapt
theproof
of Theorem 4.3 in[18]
in the case p > 2, or theproof
of Theorem 1.2 in[1] ]
inthe case
1 p 2, in order to obtain that VZ islocally
Holder continuous inMoreover, taking
into account(4.2), by
Theorem 3.11 we infer also
PROOF OF THEOREM 4.1. Let w C be a minimizer for
~. By
Lemma 4.5 the
pair
E A and moreoverSince, by
Lemma4.3,
we conclude that the
pair (Sw, w) gives
the minimum of~C. q.e.d.
REMARK 4.6. We note
that,
if(K, u)
E ~1 and minimizes~C,
then thereexists a
unique pair (K’, u’)
E .~ with thefollowing
property: K’ is the smallest closed set contained in K such that u has an extension u’ E sucha
pair
is called essentialminimizing pair.
REMARK 4.7.
If (K, u)
E .~ andminimizes g, then, by
Lemma2.3,
u C and
Su
n Q c K.By the proof
of Theorem 4.1we
concludethat, conversely, u
is a minimizer forg, -g(u) = g(K,
u),)In-1 «KBSu)
nSZ)
= 0and u may be extended as a
c1
function to hence(Su,11)
is an essentialminimizing pair.
Finally
we prove that for every essentialminimizing pair
of the functionalevery compact
contained in thesingular
set has(n -1 )-dimensional
Hausdorffmeasure which is
equal
to its Minkowski content(see
Theorem4.10).
To thisaim we
give
two estimates for the minimizers of the functionaly.
LEMMA 4.8. There
exist
two constants E, ro > 0 suchthat if
w is aminimizer
of
thefunctional y
inSBV(Q;
thenfor
every x ESw
n Qfor
every p ro Adist(x, 8Q).
PROOF. Let a,
0,
Eg 79 and r be as in Lemma 3.9. LetWere the lemma
false,
we would find x E,Sw n
Q and apositive
such that
Since
by (4.2)
for
every t
p and alsothen, by
Lemma 3.10 and Theorem3.11,
we would havex §K S’w
n Q.q.e.d.
LEMMA 4.9. There
exist
two constants El, T1 > 0 suchthat if
w is aminimizer
of
thefunctional g
inSBV(Q; Sk)
thenfor
every x ES’w f1
Qfor
every p rl Adist(x,
PROOF. Let a,
fl,
E, 0 and r be as in Lemma 3.9. Let x ESw
n Q.By
Lemma 4.8 we have
Let ci be such that the
inequality (4.3)
can be rewritten asLet a’ E
(o, 2/3]
be such that(a’)R
and 6~.By
Lemma 3.9 there exist threepositive
constants, which we denoteby
f.1,1 and ri,
depending
on n, k, p, A, ao,and 3,
such that ri 1 ro, +1)QWnT1/EP 191
and for every p E(0,
rl] withBp(x)
C Q, ifand
then
Assume
by
contradiction that there exists apositive
number p rl so thatand (
Hence
by (4.6)
we have thatwhich contradicts
(4.5). q.e.d.
THEOREM 4.10. Let
(K, u)
E A be aminimizing pair of
thefunctional g.
Then
I
rectifiable;
there exists an essential
minimizing pair (K’, u’)
E if such thatfor
every compact setQ
C K’ n S2 thefollowing equality
holdsPROOF.
By Remark
4.7 we havethat u
is a minimizerof 9
inSBV(Q; Sk),
nQ) =
0 and(Su, u)
is an essentialminimizing pair.
Theassertion (i) immediately
follows sinceSu
is( ~ n-1, n - 1)
rectifiable and nQ)BSu) =
0.By choosing
K’ =Su
and u’= ic,
theequality
(4.7)
follows as in[6], Proposition 5.3, by using
the uniformdensity
estimateestablished in Lemma 4.9.
q.e.d.
REMARK 4.11. We remark that the conditions on 1
(see (4.1))
are sufficientto obtain the
semicontinuity
result in Theorem 4.2. For moregeneral integrands
-1, for which also
semicontinuity
theoremshold,
we refer to Theorems 3.6 and 4.1 in[4].
For these cases,if 1
is assumed even to be bounded above and belowby
twopositive
constants, one may repeat the discussions of this section in order to extend thepreceding
results.5. - A
Dirichlet-type problem
Let 1, ~ and T be as in Section
4;
let assume n, > 2, p > 1.For any
C
1function p : IRn-1
~ R withp(0)
= 0= IV’ p(0)1, Lip p
1, letwhere x’ =
(x 1, ... ,
Xn-1).’
Arguing
as in Theorem 3.7 andCorollary
3.8 of[9],
we maymodify
theproof
ofCorollary
3.7 in order to obtain thefollowing
limit theorem.such that
such that
such that Assume that
for
almostall , for
everyThen E
cO(B1; JRk+1),
there exists ahyperplane L
such that theimage of
u,,.lies
essentially
in 1:, u,, = 0 in isp-harmonic
in >and
_
r
for
almost all p 1.We note that for the