A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
M ICHELE C ARRIERO
A NTONIO L EACI
F RANCO T OMARELLI
Strong minimizers of Blake & Zisserman functional
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 25, n
o1-2 (1997), p. 257-285
<http://www.numdam.org/item?id=ASNSP_1997_4_25_1-2_257_0>
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Strong Minimizers
ofBlake & Zisserman Functional
MICHELE CARRIERO - ANTONIO LEACI - FRANCO TOMARELLI (1997), pp.
With deep sorrow for the loss of our Teacher and Friend, we dedicate this paper to Ennio De Giorgi.
We have tried to pursue our research in the direction that he had pointed out.
Abstract. We prove the existence of strong minimizers for functionals depending
on free discontinuities, free gradient discontinuities and second derivatives, which
are related to image segmentation.
1. - Introduction ’
The issue of
minimizing
functionalsdepending
on both a bulk energy anda surfacic
(or
lineic in twodimensions) discontinuity
energy has attracted the interest of many researchers(see
for instance[A 1 ], [A2], [AFP], [AV], [BZ], [C], [CL], [CLT1]-[CLT5], [Co], [DA], [DCL], [DG], [DMS], [DS], [Fo], [LS], [MS], [MSh], [Tl], [T2]).
Here we focus the functional
where Q c M" is an open set,
R,with
are
given;
whileKo, Ki
C are Borel sets(a priori unknown)
withKo
UK1 closed,
and u EB (Ko
UK1))
isapproximately
continuous on S2B Ko.
We notice that in case n = p = q - 2 the energy
( 1.1 )
reduces to thefollowing
oneFunctional
(1.3)
was introducedby
Blake & Zisserman(thin plate
surface under tension[BZ])
as an energy to be minimized in order to achieve asegmentation
of a monocromatic
picture.
In this context g describes thelight intensity
levelon the screen
0, A
is a scaleparameter,
a is a contrastparameter
and a measure ofimmunity
tonoise, fl
is agradient-contrast
parameter.The elements of a
minimizing triplet Ki, u) play respectively
the roleof
edges,
creases andsmoothly varying intensity
in theregion
QB (Ko
Ufor the
segmented image.
The second-order model(1-.3)
was introduced to overcome theover-segmentation
ofsteep gradients (ramp effect)
and other in-convenients which occur in lower order models as in case of Mumford & Shah functional
([MSh]).
We prove the
following
statements.THEOREM 1.1. Under
assumptions (1.2)
with n = p = 2 there is at least onetriplet
amongKo, KI
iC R 2
Borel sets withKo U.K1
closed and u EC2(QB(KoUKl)
approximately
continuous on QB Ko minimizing functional ( 1.1 )
andhaving finite
energy. Moreover the sets
Ko
f1 Q andKl
fl Q are(?nC 1, 1 ) rectifiable.
THEOREM 1.2. Under
assumptions (1.2)
with n = p = 2 and a =there
isat least one
pair
among K C closed set and u EB K) minimizing
thefunctional
and
having finite
energy. Moreover the set K n S2 is1) rectifiable.
We
proved
the existence ofstrong
solutions for different freediscontinuity problems involving
second derivatives inprevious
papers: models of elastic-plastic plates [CLT3]
andrigid-plastic
slabs[CLT4],
but in those cases thecontinuity
ofcompeting
functions was built into the functional(Ko*= 0),
andthis
property
entailed an "apriori"
L°° estimate which is not true any more in thepresent
case. Here the finiteness of energy(1.3)
entails neither essential boundedness of u or Vu nor localsummability
of Vu(see example (1.4)
of
[CLT5]),
and this factdevelops
many substantial difficulties.In the paper
[CLT5]
we introduced a relaxed version of(1.3) (weak
for-mulation of the Blake & Zisserman
functional)
which in case of(1.1)
leads toto be minimized over V E
GSBV(Q),
with Vv E and weproved
the existence of minimizers of
(1.4).
Here we prove that for p = n = 2a weak minimizer
actually provides
aminimizing triplet
of(1.3) by taking
arepresentative
of the function and the closure ofsingular
sets of the function itself and of itsgradient.
The
proofs rely
on adeep
use of the coarea formula and of a new Poincaretype inequality
inGSBV(Q) (see
Theorem4.1 ).
These tools allow thestudy
of a normalized energy
density (see (5.1 ))
for which we prove a suitabledecay
outside the
singular
set of weak solutions.By
a carefulapplication
of our Poincareinequality
we show that blownup sequences
(vh)
of a weak minimizer are nice aroundpoints
withvanishing
normalized energy
density:
in the sense that the functions vh,though converging only
in measure, arestrongly convergent
intogheter
with theirapproxi-
mate
gradient,
if modified on sets of small area andperimeter
in a way preserv-ing
median andgradient
median(see
Theorem4.3).
Thiscompactness property
is the most technical and difficult
point
of the whole argument and allows us to show that thepointwise
limit of(vh)
solves anelliptic
fourth orderequation (see
Theorem5.1):
thedecay
estimates of its solutions are transferred(by
atechnical
joining lemma)
to the sequence(Vh) (see
Theorem5.4).
This entails that for a weak minimizer v of(1.4),
we find U = 0and v E
B Sv
U5’vu).
We stress the fact that for the Mumford & Shah functional
([DCL]),
the
elastic-plastic plate
functional([CLT3])
and therigid-plastic
slab func-tional
([CLT4]),
the minimizers u arequasi-minimizers
of the mainpart
of the functional so that theforcing
term in the functionalplays
the role of asmall
perturbation.
While for the Blake & Zissermannfunctional,
as like as in the Mumford & Shah functional with unbounded datum(see [L]),
theforcing
term has to be considered in the main
part
of the functional and not as a lower orderperturbation.
The
only point
where theassumption p
= 2 is needed is thedecay
estimatefor solutions of a linear
elliptic equation
of the fourth order(see
Theorem5.2);
elsewhere in the
proofs
theonly assumption
p > n isenough.
The
assumption
g E issharp
in the sense that for every T nq there exist g E such that functional(1.1)
has nominimizing triplet.
Werefer for a
counterexample
to aforthcoming
paper where additionalproperties
of solutions are
given:
lower and upperdensity estimates,
necessary conditions satisfiedby
strongminimizers,
astudy
of the vector valued case and a moregeneral
casefor p
and n.The outline of the paper is the
following.
1. Introduction
2. Notation and functional spaces 3.
Preliminary
results4.
Compactness
and lowersemicontinuity
5.
Blow-up equation
6. Proof of the main results
2. - Notations and functional spaces
From now on we denote
by Q
an open set in 2.For a
given
set U C R" we denoteby
8U itstopological boundary, by
its k-dimensional Hausdorff measure and
by U ~ I
itsLebesgue
outermeasure; Xu is the characteristic function of U. We indicate
by Bp (x)
theopen ball
{y
E~y - x I p},
and we setBp
== If Q, Q’
are open subsets in
R’, by
Q C C S2’ we mean that Q is compact and Q c Q’.We introduce the
following
notations: s A t =min{s, t}, s
V t =max{s, t}
forevery s, t E R;
given
two vectors a,b,
we set a.b =Ei aibi
and =In the
following
with the same letter c we denote suitable constants which maychange
in differentinequalities.
For any Borel R the
approximate
upper and lower limits of v are the Borel functionsv+,
v- : S2 -~ R = R U defined for any xES2by
The set
is a Borel set, of
negligible Lebesgue
measure(see
e.g.[F], 2.9.13);
wesay
that v isapproximately
continuous on QB Sv
and we denoteby v :
QB Sv
R the function-
Let x E Q
B Sv
be suchthat v(x)
E R; we say that v isapproximately
differentiable at x if there exists a
vector VV(X)
E R"(the approximate gradient
of v at
x )
such thatIf v is a smooth function then Vv is the classical
gradient.
In thefollowing
withthe
notation lvvl
we mean the euclidean norm of Vv and we set =denoting
the canonical basis of R". In the one dimensional case(n
=1)
we shall use the notation v’ in
place
We recall the definition of the space of functions of bounded variation in S2 with values in R:
where Dv =
(D1 v, ... , Dn v)
denotes the distributionalgradient
of v anddenotes the space of vector-valued Radon measure with finite total variation.
We denote
by fo IDvl
the total variation of the measure D v in Q.If v = XE is the characteristic function of a set E, then v E
B V (Q)
ifand
only
if E is a set with finiteperimeter
inQ;
theperimeter
of E in Q isgiven by
r
For every v E
B V (S2)
thefollowing properties
hold:1) v+(x), v-(x)
E R for all x E Q(see [Z], 5.9.6);
2) Sv
iscountably (H ’- 1, n - 1)
rectifiable(see [F], 4.5.9(16));
3)
Vv exists a.e. in S2 and coincides with theRadon-Nikodym
derivative of Dv with respect to theLebesgue
measure(see [F], 4.5.9(26));
4)
for almost all X there exists aunique V
= E8Bi
1 suchthat, setting Bp
={y
EBp(x) : (y - x) ~
v >0}
andBg = [y
EBp(x) :
(y - X) - v 0},
then(see [Z], 5.14.3)
and also
(see [F], 4.5.9(15))
Moreover is an
approximate
normal vector toSv
at x(see [Z], 5.9.6).
We recall the definitions of some function spaces and we refer to
[DA]
and
[A 1 ]
for theirproperties.
DEFINITION 2. l.
SBV (Q)
denotes the class of functions v EB V (Q)
such that
11 p 11
SBVI,,,(Q)
denotes the class of functions v ESBV(Q’)
for every Q’ cc Q.Moreover we define
_ ___ .__ r - - - . - ~ , ~_~ .~... , rt, 1
LEMMA 2. 2. Let v E
GSB V (0).
ThenSv is countably (~-~C n-1, n -1 ) rectifiable
and V v exists a. e. in Q.
PROOF. See
[A2], Proposition
1.3 and 1.4. ElLEMMA 2.3. Let S2 C R nbe a bounded open set with
Lipschitz boundary
andv E
GSB V (S2).
Assume thatThen for
every a, b ER,
a b we have (and
(a
V v Ab) XE
ESBV (Q) for
every set Ewith finite perimeter
in Q.PROOF. Follows
easily by
Definition 2.1 and the coarea formula(see
e.g.[Z],
5.4.4).
DLEMMA 2.4.
Let a, b
E R and v EGSB V (a, b).
The
previous lemma,
whenapplied
to any function inGSB V 2 (a, b)
andto its
approximate derivative,
shows that in dimension one thestrong
formula- tion( 1.1 )
and the weak formulation(1.4)
coincide.Now we may define the
following
function spaces; even if we will useonly
in thefollowing,
we recall the definitions of various spaces related to bounded secondderivatives,
to avoid confusion with other authors’notations.
DEFINITION 2.5. We set
Notice that Dv = Vv in
SBH(Q), Dv =A
Vv in and inGSB V2(Q);
moreover we set
-
Eventually
we introduce the weak energy functional and a space for com-peting
functions.DEFINITION 2.6. For S2 C R’ open set, under the
assumption (1.2), setting
= n
Lq (Q),
we define F:X(0)
--~[0, +00]
asWe need a localization of the
previous
functional ,~’.DEFINITION 2.7. For every Borel subset A C S2 and V E we define
We shall use
0(v, A)
if g, ~, a,f3
areclearly
definedby
the context.The
following
two theorems have beenproved
in[CLT5]
with the inessential restriction p = q = 2. In the first statement we use thefollowing
sequence of smooth truncation functions:for every
integer k >
2. Theproperty
v EGSB V (Q) (see
Definition2.1 )
isclearly equivalent
to therequirement
(see [A2],
Section1 ).
THEOREM 2.8
(Interpolation inequality).
Let n E l~ and letQ
C JRn be a cubewith
edges of lenght
Iand parallel
to the coordinate axes, p > 1 and v E GSBV 2 ( Q).
Then
for
every i =1,
... , n thefollowing inequality
holds trueTHEOREM 2.9
(Existence
of weaksolutions).
Let Q c JRn be an open set.Assume
(1.2)
with g ELq (0).
Then there is Vo EX (Q)
such thatWe recall that
assumption fl
a2~8
is necessary for lowersemicontinuity (see [BZ], [Co]).
3. -
Preliminary
results’
In this section we prove some technical results.
LEMMA 3.1
(Density
upperbound).
Let v Eminimizer for the functional (2.1 ) with
g E(r 2: nq ).
Thenfor
every 0 p 1 andfor
every x E S2 such that
B p (x)
C S2 we havewhere (
PROOF.
By minimality
of v for .~’ we get.~’(w),
where w =VXQBB,(,).
· SinceSw
USvw
c((Sv
USvv) B B,(x))
Ua Bp (x)
andtaking
intoaccount
f3
a,by
subtraction we obtainhence, by
theassumptions
on T and p, we achieve theproof.
CLEMMA 3.2. Let Q C R" be an open set and let
Ko, K1
1 C be Borel sets withKo
UK,
closed. Let v EB (Ko
UK1 ))
and let v beapproximately
continuou6in S2
B Ko.
Assume thatthen r
PROOF. The function v is
obviously
inLq(0) and, by
Lemma 2.6 in[CLT3],
we have ~v E
So, by
Lemma 2.3 in[DCL],
theproof
will beachieved as soon as we show that for every cube
Q
c Q withedges parallel
tothe coordinate axes and for every
integer k >
2 we E(possibly
notuniformly
ink, Q),
where satisfies(2.2).
Fix
Q
c Q as above and i E{ 1, ... , n }, then, by
Theorem2.8,
we obtainthe
following interpolation inequality
where 1 is the
edge length
ofQ.
Hence v EX (Q)
and the other assertionsfollow
immediately.
0REMARK 3.3.
By
Theorem 2.9 and Lemma 3.2 we obtainimmediately
thatmin
.~’(v) inf f F(Ko,
"Ki, v) : Ko, KI
C JRn Borel sets,Ko
UKI closed,
v E
c2(Q B
UKi)), v approximately
continuouson Q B Ko } .
LEMMA 3.4
(Scaling).
Let v E For À > 0 andfor
everyx E
BI
set vand,
Then Vr E
PROOF. Follows
immediately by change
of variables.DEFINITION 3.5. A function v E
X (Q)
is a local minimizer of(2.1 ) if,
forevery
compact
set T CQ,
Actually
the infimum in the Definition 3.5 is a minimum due to Theorem 2.9 and to the fact that{z
eX (S2) :
z = vT }
is closed inLEMMA
3.6(Matching).
Let 2 : andThen, by setting
we have
PROOF. Follows
immediately by
the definitions. 0 LEMMA 3.7(Joining).
Let u, v E and let 0 s t 1 be suchthat
B t (x )
C Q. Thenfor
every 8 E(0, 1)
there exist c =c (8, p, n)
> 0 and acut-o, ff function 1/1
EC2 0 (Bt (x)),
with1/1
=- 1 in aneighborhoud of
suchthat, by setting
U =1/Iv
+( 1 - ~ ) u,
we havePROOF. To
simplify
notation we consider x = 0. We fix 8 E(0, 1)
and. Let
and *j ( j
-0,...,
N -1)
cut-off functionsbetween Bj
1 of classC2
such that and ! in(where
and define
Then, by setting
a 0 b= 1 (a ®
b + b ®a),
we get, for everyj,
Since
Cj
f1Cj+l = 0, by adding
withrespect to j
from 0 to N -1,
weget
minBy choosing
theindex j
for which the above minimum isachieved,
we setso that
hence the thesis follows with o
LEMMA 3.8. Let n >
2,
p > 1 and let Q C JRn be open. Let i suchthat, for
every compact set T CQ,
Then
for
PROOF.
Apply
the sameargument
of Lemma 2.6 in[DCL].
4. -
Compactness
and lowersemicontinuity
We prove a Poincare type
inequality
in the class GSB V which extends Theorem 3.1 in[DCL] allowing
a moregeneral
truncation. Weenphasize
thatv E does not even entail that either v or Vv
belongs
toLet B be an open ball in L~n . For every measurable function v : B --* R
we define the least median of v in B as
We remark that
med(., B )
is a non linear operator and ingeneral
it has norelationship
withf B dy . Obviously
we havemed(vXB~E
+med(v, B) XE, B) = med ( v , B )
for every E C B. For every v EGSBV(B)
and a E R withn -
, we set
where yn is the
isoperimetric
constant relative to the balls ofR",
i.e. for every Borel set E0 we define the truncation operator
We
get easily T (T (v,
a,1]),
a,q)
=T (v, a, y?), med(T (v,
a,B)
=med(v, B)
and a, =
1])
for every À > 0 .Moreover IVT(v,
a,1])1 I
a.e. on B and
In case v is vector-valued the
operators
med and T are definedcomponentwise.
THEOREM 4.1
(Poincaré
typeinequality).
Let B C JRn be an openball,
n >2,
p > 1. Let v E
GSBV (B)
and a E R withlet r~ > 0 and
T (v,
a,q)
as in(4.1).
ThenIf
p n,setting
, we have alsoIf
p > n,for
eve ry ~ we have alsoPROOF. We may assume that
med(v, B) =
0 and theright
hand sides arefinite. If 0 and a = 0 then V E
T (v, 0, r~)
= v andthe
inequalities
are well-known.By
Lemma2.3,
ESBV(B)
and weobtain
By
the coarea formula of Lemma 2.3 and theisoperimetric inequality
we obtainBy
theassumption
on a andby comparison
with(4.7)
in the case t7 = 0 wehave
hence
By
substitution in(4.7),
we obtain for everyso
(4.4)
followsby
Holderinequality. By (4.8)
and(4.10)
weget
alsoBy
the classical Poincareinequality (see [F],
pag.504) applied
towe
get
We define
Then, by taking
into account(4.1), (4.2)
and(4.4),
we have for everyHence if p =
1, by (4.13 )
with s =1 * , (4.12)
and(4.10)
forT ( v ,
a,0)
we getso that
(4.5)
isproved
in the case p = 1. We focus now the caseWe set
-*
and we notice that w E
SBV(B), med(w, B)
=med(v, B)
andBy plugging
w in(4.12)
and(4.10) with 17
= 0 andby
Holderinequality
Dividing by
which is finite sinceT (v,
a,0)
isbounded,
we
get
By (4.13)
with s =p *
and(4.14)
we obtainIf p > n, fix and set
r = 2013~.
Then r n and r * = s,hence
by (4.5)
and Holderinequality,
stillassuming med(v, B)
= 0 andsetting
, we have
and the
proof
iscompleted.
We show
that,
beside(4.2),
also theperimeter
of the setcan be estimated for many suitable 1] E
(0, 1).
LEMMA 4.2. Let B C R" be an open
ball,
n >2,
s > 1. Let v EGSB V (B)
and a E R with
(
Then there exists q E(0, 1 )
such thatActually
: both(4.15)
and(4.16) hold ) I
PROOF.
By
coarea formula of Lemma 2.3 andby
the definition ofSBV (B)
and
analogously
We
get
the thesisby Chebyshev
and Holderinequalities
andby (4.2).
DFor any
given
function inGSB V,
we define an affinepolynomial
correctionsuch that both median and
gradient
median vanish.Let C Q and V E for every y E R’ we set
Since
med(v -
c,Br (x ) )
=med(v, B,. (x ) ) -
c for every c E R andthen we have say
We notice that there are v such that
med(v, # med(Px,rv, B,(x)),
takee.g.
v(x)=
where H is the Heaviside function.In the
following
we denoteby s’
theconjugate exponent
of s in the Holderinequality.
THEOREM 4.3
(Compactness
and lowersemicontinuity).
Let2,
Br (x )
C be an openball, (Vh)
CGSBV2(Br(x)).
SetL h
Assume
Then there exist Z E
W 2’ p ( Br (x)),
a sequence(Zh)
C GSBV 2 ( Br (x))
and apositive
constant c
(depending
on theleft
hand sideof (4.19))
suchthat,
up toa finite
numberof indices,
Moreover there is a
subsequence
suchthat for
everyPROOF. We can assume x =
0,
0 and we extractsubsequences
without
relabeling.
We useproperties
of functions that hold trueonly
up to a finite number ofindices,
henceby (4.20)
we can assume thatArguing separately
oneach component Of V Vh
we deduce that V k E{ 1, ... , n },
there existq§
E(0, 1)
and cdepending
on the l.h. s. of(4.19)
suchthat
Inequality (4.28)
followsby (4.2),
while(4.29)
followsby
Lemma 4.2 withs = p
applied
toVkvh
and1) through (4.19).
We define small subsets
Eh
CBr
where we have tomodify vh
in orderto force boundedness
of Vvh,
and weperform
a formertuning
of Vh. To this aim setSince
med(vh, Br ) = 0
thenmed(wh,
andby
the definitionmed(Vwh , Br)
=
med(Vvh, Br)
= 0.By (4.29) Eh
has finiteperimeter,
henceby
Lemma 2.3we have wh E
GSB V2 (B,)
andV Wh
ESBV(Br,
nL’(B,, JRn).
Thenby summarizing
and
by (4.20), (4.28)
and(4.29)
p. Since 0
1]~ 1, by (4.32), (4.6), (4.19)
and(4.20)
weBy (4.32), (4.9)
andby
theassumptions (4.19), (4.20)
and p > n, we getNow we want to force boundedness of
(wh). By (4.32)
we can assumeand there are ?7h E
(0, 1)
and a constant,depending
on the l.h.s. of(4.19),
such that
Inequality (4.36)
followsby (4.2),
while(4.37)
followsby
Lemma 4.2 withs = p,
applied
to Wh,taking
into account(4.32)
and(4.34).
Then we defineand we
perform
thefollowing tuning
of the sequenceWe notice that zh E and
Hence
(4.21 )
and(4.22)
followby (4.28), (4.36),
and(4.29), (4.37) respectively,
taking
into account theassumption
p 2: n.By (4.7), (4.9)
and(4.34)
we haveMoreover, by (4.39)
and(4.34),
and
by (4.32), (4.39)
we gethence
by (4.11)
and theassumption p
we haveSince 0 17h
1, by (4.6)
and(4.41)
By (4.41), (4.42)
and thecompactness
theorem inapplied
tothere exists
f
E such thatBy (4.39), (4.19), (4.20)
and Theorem 2.1 in[All, f
ESBV(Br, JRn)
and alsohence
f
EBy [B],
Theorem 18 inAppendix,
andby (4.34)
we get
By (4.40), (4.43)
and the compactness theorem inB V (Br ) applied
to(Zh) ,
there exists z EB V (Br)
such thatBy (4.39), (4.41)
and Theorem 2.1 in[Al]
we have z ESBV(Br)
and alsohence z E and also
by (4.43)
By (4.45)
and(4.46) f
= Vz = Dz so that z EW2,p (B,). By
the arbitrarinessof 6, (4.23), (4.24), (4.25)
hold true and(4.26), (4.27)
followby (4.21).
05. -
Blow-up equation
The aim of this section is to prove for any minimizer v of
(2.1 )
a fasterdecay
estimate of the functional aroundpoints X
such thatTHEOREM 5.1
(Blow
upequation).
Let p > n > 2 andB,. (x )
C S2 be anopen
ball, (Vh)
CX (Q), (~ph )
C let(ah ),
and(,c,ch )
three sequencesof positive
numbers withPh
ah and let Z E Assume thatThen, for
every p r, z minimizes thefunctional
over all v E such that v = z in
Br (x ) B Bp (x)
andIn
particular
z is a weak solutionof
thefourth
orderelliptic equation
PROOF. Assume x = 0 and set for
brevity’s
sake. We will extractsubsequences (without saying explicitly
and withoutrelabeling)
each timeis needed and we will omit the
arguments
ah,Ph
in First we estimateand we have
by (iv), (v)
and even
by (v),
Hence
and
then, by
Fatou’slemma,
By (ii)
and(iii),
theassumptions
of Theorem 4.3 aresatisfied,
so that we can choose zh and z as like as in Theorem 4.3 and z turns out to be the same ofassumption (iv). By (4.25), (5.2)
and(iii)
we obtainTo achieve the
proof
we want to show that for almost every p r , for every v E with v = z inBr B Bp
By monotonicity (o
is continuous for a.e. p E(0, r).
Assumeby
contradiction that there exist s r, vE W2,P(Br)
and E > 0 such that cv is continuous at s,v = z in and
As like as in Theorem
4.3,
we setLh
=1t n-l (SVh
U andAh
=Eh
UWh
=(vh - PVh))-
Toget
a contradiction wepaste together zh
+PVh and Vh along
theboundary
of asuitably
choosen ball and then wejoin
the new functionwith v
(which
reduces the energy inBs).
To thisaim,
we remark that for a.e.p E
(0, r)
we haveand, by (4.22),
Integrating
inpolar
coordinates andby
theisoperimetric inequality
we getSince
by (iii)
the sequence~ah Lh ~
isbounded,
thenby (ii)
Hence,
for a.e. p E(0, r),
we haveNow, by
thecontinuity
of cv at s andby (5.4),
we choose t E(s, r)
such thatand we
glue together vh
and Zh +~vh by defining
By
Lemma3.6,
u h E andWe join
u h and Let1frh
be the cut-off functionsbetween BS and Bt provided by
Lemma 3.7 and setThen
Uh belongs
inBr B Bt
and wehave, by
theminimality of vh
inBt, by v
= zon B, B BS
andby (5.7),
By taking
into account(4.22)-(4.27), (4.31), (4.38), v
and assump- tions(i), (iii)
and(v),
we take the limit as h -~ +00 and we haveThen
by
the arbitrariness of 3 andby (5.3)
and(5.5)
we getcontradicting
themonotonicity
of cv. 0We recall the
following
well-known result for the biharmonic operator. For theproof
we refer to[G],
Ch.III,
sect. 2.THEOREM 5.2
(Estimate
on the solutions of the biharmonicequation).
Let B,
C R’ and let u E solutionof
Then the
following inequality
holds:where cn is an absolute constant
depending only
on the dimension.REMARK 5.3.
For q
> 1 there exists a constant cdepending only
on n andq such that for every affine
function ~
and every 0 p r we havehence there exists a constant cn,q such that for every biharmonic function u and for every affine
function ~
we haveTHEOREM 5.4
(Decay).
Assume(1.2)
with n = p = 2. For every k >2,
ri, a E
(0, 1 )
withr
there is 80 > 0 such thatfor
every 8 E(0, EO]
and.4
is a local minimizer it, a,
f3, Q)
withand
then
PROOF. Assume that the theorem is false. In such case, there exist k >
2,
77, Or E
(0, 1)
withr0’ £,
a sequenceof 8h
> 0 withlimh 8h =
0 andC2.a
local minimizers of
(.,
JL, a,~, Q)
such thatand
By translating
into theorigin
andrescaling
we setwhere
The
functions vh
are local minimizers inB1
for , whereBy
Lemma 3.4 we gethence
By (5.9)
andby
Theorem4.3,
up to asubsequence
that we do notrelabel,
thereexists z such that
Now we
verify
that thefunctions vh
and zsatisfy
all theremaining assumptions
of Theorem 5.1.
Assumption (i)
followsby
Lemma 3.4 and(ii)
followsby (5.10).
We prove(iii):
let(tj)
be a sequence of radii dense in(0, 1). By (5.9), by extracting
forany tj
asubsequence of vh
andby diagonalizing,
there exists forany tj
Since tj
-~ is monotonenondecreasing,
hence continuous up to a countable set, then the above limit exists for almost everyradius p
E(0, 1).
Toverify (v)
of Theorem5.1,
we prove first thatBy
Lemma 3.1(hh)
isbounded,
so our claim is obviousif q
>2,
and in the case q 2 it followsby
theassumption
ph8h k .
Moreover,by changing
variables and
using
Holderinequality,
weget
hence
Finally
we prove that is bounded inBl .
Since are affinefunctions,
it will beenough proving
that ph isbounded,
and theconvergence follows
possibly extracting
asubsequence.
Infact, referring
to thefunctions Zh
introduced in Theorem 4.3 andsetting Ah =
-~for every h
big enough
we havedue to
(5.9)
and(5.12). By
Theorem 5.1 we haveOn the other
hand, by (5.8),
hence which contradicts the
assumption
on 17.6. - Proof of the main results
In this
concluding
section we prove Theorems 1.1 and 1.2.Let v E
GSBV2(Q)
be a minimizer of .~’given by
Theorem 2.9. We remark first that if B is an open ball such that B C S2 U = 0 then v is smooth inB,
since we have v EW2,2 (B)
so thatby
the standardregularity theory
we obtain D EC2(B) (see
e.g.[B]
for the case q > 1 and use anapproximation argument for q
=1).
Hence we have v EC2(Q B
UWe now estimate ’ Set
We prove that
Qo
is open. In order toapply
Theorem5.4,
we fix k > 2 and r~, o~ E(0, 1)
withr~~ ~2 ;
; let 80 be as in Theorem5.4,
let x EQo
and letr > 0 be such that
We show that If z then
hence we may
apply
Theorem 5.4inductively
to obtainfor every h E N. For every 0 t qr there
exists j
such thatso that
~ , , ,
then
passing
to the limit as t - 0(so that j
- we get z ES2o.
SinceSv
U iscountably 1) rectifiable, by
Theorem 3.2.19 in[F]
we haveH1«Sv
USvv)
nS2o)
= 0 so and(Sv
USVv)
nQo
= 0. SinceQo
is open then USov
= 0.By
Lemma 3.8 we haveSetting
we have that is
closed,
and ’hence are ( )
rectifiable,
moreoverand, by
Remark3.3,
we conclude that(Ko, K1, C)
is a minimizer for F in theclass of the admissible
triplets.
DTheorem 1.2 follows
immediately by
Theorem 1.1choosing
K =Ko
UKl
and