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(1)

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

e

série, tome 25, n

o

1-2 (1997), p. 257-285

<http://www.numdam.org/item?id=ASNSP_1997_4_25_1-2_257_0>

© Scuola Normale Superiore, Pisa, 1997, tous droits réservés.

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http://www.numdam.org/

(2)

Strong Minimizers

of

Blake &#x26; 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

functionals

depending

on both a bulk energy and

a surfacic

(or

lineic in two

dimensions) 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;

while

Ko, Ki

C are Borel sets

(a priori unknown)

with

Ko

U

K1 closed,

and u E

B (Ko

U

K1))

is

approximately

continuous on S2

B Ko.

We notice that in case n = p = q - 2 the energy

( 1.1 )

reduces to the

following

one

(3)

Functional

(1.3)

was introduced

by

Blake &#x26; Zisserman

(thin plate

surface under tension

[BZ])

as an energy to be minimized in order to achieve a

segmentation

of a monocromatic

picture.

In this context g describes the

light intensity

level

on the screen

0, A

is a scale

parameter,

a is a contrast

parameter

and a measure of

immunity

to

noise, fl

is a

gradient-contrast

parameter.

The elements of a

minimizing triplet Ki, u) play respectively

the role

of

edges,

creases and

smoothly varying intensity

in the

region

Q

B (Ko

U

for the

segmented image.

The second-order model

(1-.3)

was introduced to overcome the

over-segmentation

of

steep gradients (ramp effect)

and other in-

convenients which occur in lower order models as in case of Mumford &#x26; Shah functional

([MSh]).

We prove the

following

statements.

THEOREM 1.1. Under

assumptions (1.2)

with n = p = 2 there is at least one

triplet

among

Ko, KI

i

C R 2

Borel sets with

Ko U.K1

closed and u E

C2(QB(KoUKl)

approximately

continuous on Q

B Ko minimizing functional ( 1.1 )

and

having finite

energy. Moreover the sets

Ko

f1 Q and

Kl

fl Q are

(?nC 1, 1 ) rectifiable.

THEOREM 1.2. Under

assumptions (1.2)

with n = p = 2 and a =

there

is

at least one

pair

among K C closed set and u E

B K) minimizing

the

functional

and

having finite

energy. Moreover the set K n S2 is

1) rectifiable.

We

proved

the existence of

strong

solutions for different free

discontinuity problems involving

second derivatives in

previous

papers: models of elastic-

plastic plates [CLT3]

and

rigid-plastic

slabs

[CLT4],

but in those cases the

continuity

of

competing

functions was built into the functional

(Ko*= 0),

and

this

property

entailed an "a

priori"

L°° estimate which is not true any more in the

present

case. Here the finiteness of energy

(1.3)

entails neither essential boundedness of u or Vu nor local

summability

of Vu

(see example (1.4)

of

[CLT5]),

and this fact

develops

many substantial difficulties.

In the paper

[CLT5]

we introduced a relaxed version of

(1.3) (weak

for-

mulation of the Blake &#x26; Zisserman

functional)

which in case of

(1.1)

leads to

to be minimized over V E

GSBV(Q),

with Vv E and we

proved

the existence of minimizers of

(1.4).

Here we prove that for p = n = 2

a weak minimizer

actually provides

a

minimizing triplet

of

(1.3) by taking

a

representative

of the function and the closure of

singular

sets of the function itself and of its

gradient.

The

proofs rely

on a

deep

use of the coarea formula and of a new Poincare

type inequality

in

GSBV(Q) (see

Theorem

4.1 ).

These tools allow the

study

(4)

of a normalized energy

density (see (5.1 ))

for which we prove a suitable

decay

outside the

singular

set of weak solutions.

By

a careful

application

of our Poincare

inequality

we show that blown

up sequences

(vh)

of a weak minimizer are nice around

points

with

vanishing

normalized energy

density:

in the sense that the functions vh,

though converging only

in measure, are

strongly convergent

in

togheter

with their

approxi-

mate

gradient,

if modified on sets of small area and

perimeter

in a way preserv-

ing

median and

gradient

median

(see

Theorem

4.3).

This

compactness property

is the most technical and difficult

point

of the whole argument and allows us to show that the

pointwise

limit of

(vh)

solves an

elliptic

fourth order

equation (see

Theorem

5.1):

the

decay

estimates of its solutions are transferred

(by

a

technical

joining lemma)

to the sequence

(Vh) (see

Theorem

5.4).

This entails that for a weak minimizer v of

(1.4),

we find U = 0

and v E

B Sv

U

5’vu).

We stress the fact that for the Mumford &#x26; Shah functional

([DCL]),

the

elastic-plastic plate

functional

([CLT3])

and the

rigid-plastic

slab func-

tional

([CLT4]),

the minimizers u are

quasi-minimizers

of the main

part

of the functional so that the

forcing

term in the functional

plays

the role of a

small

perturbation.

While for the Blake &#x26; Zissermann

functional,

as like as in the Mumford &#x26; Shah functional with unbounded datum

(see [L]),

the

forcing

term has to be considered in the main

part

of the functional and not as a lower order

perturbation.

The

only point

where the

assumption p

= 2 is needed is the

decay

estimate

for solutions of a linear

elliptic equation

of the fourth order

(see

Theorem

5.2);

elsewhere in the

proofs

the

only assumption

p &#x3E; n is

enough.

The

assumption

g E is

sharp

in the sense that for every T nq there exist g E such that functional

(1.1)

has no

minimizing triplet.

We

refer for a

counterexample

to a

forthcoming

paper where additional

properties

of solutions are

given:

lower and upper

density estimates,

necessary conditions satisfied

by

strong

minimizers,

a

study

of the vector valued case and a more

general

case

for p

and n.

The outline of the paper is the

following.

1. Introduction

2. Notation and functional spaces 3.

Preliminary

results

4.

Compactness

and lower

semicontinuity

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 denote

by

8U its

topological boundary, by

its k-dimensional Hausdorff measure and

by U ~ I

its

Lebesgue

outer

(5)

measure; Xu is the characteristic function of U. We indicate

by Bp (x)

the

open ball

{y

E

~y - x I p},

and we set

Bp

=

= 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}

for

every 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 may

change

in different

inequalities.

For any Borel R the

approximate

upper and lower limits of v are the Borel functions

v+,

v- : S2 -~ R = R U defined for any xES2

by

The set

is a Borel set, of

negligible Lebesgue

measure

(see

e.g.

[F], 2.9.13);

we

say

that v is

approximately

continuous on Q

B Sv

and we denote

by v :

Q

B Sv

R the function

-

Let x E Q

B Sv

be such

that v(x)

E R; we say that v is

approximately

differentiable at x if there exists a

vector VV(X)

E R"

(the approximate gradient

of v at

x )

such that

If v is a smooth function then Vv is the classical

gradient.

In the

following

with

the

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 distributional

gradient

of v and

denotes 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)

if

and

only

if E is a set with finite

perimeter

in

Q;

the

perimeter

of E in Q is

given by

r

(6)

For every v E

B V (S2)

the

following properties

hold:

1) v+(x), v-(x)

E R for all x E Q

(see [Z], 5.9.6);

2) Sv

is

countably (H ’- 1, n - 1)

rectifiable

(see [F], 4.5.9(16));

3)

Vv exists a.e. in S2 and coincides with the

Radon-Nikodym

derivative of Dv with respect to the

Lebesgue

measure

(see [F], 4.5.9(26));

4)

for almost all X there exists a

unique V

= E

8Bi

1 such

that, setting Bp

=

{y

E

Bp(x) : (y - x) ~

v &#x3E;

0}

and

Bg = [y

E

Bp(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 to

Sv

at x

(see [Z], 5.9.6).

We recall the definitions of some function spaces and we refer to

[DA]

and

[A 1 ]

for their

properties.

DEFINITION 2. l.

SBV (Q)

denotes the class of functions v E

B V (Q)

such that

11 p 11

SBVI,,,(Q)

denotes the class of functions v E

SBV(Q’)

for every Q’ cc Q.

Moreover we define

_ ___ .__ r - - - . - ~ , ~_~ .~... , rt, 1

LEMMA 2. 2. Let v E

GSB V (0).

Then

Sv 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. El

LEMMA 2.3. Let S2 C R nbe a bounded open set with

Lipschitz boundary

and

v E

GSB V (S2).

Assume that

Then for

every a, b E

R,

a b we have (

and

(a

V v A

b) XE

E

SBV (Q) for

every set E

with finite perimeter

in Q.

(7)

PROOF. Follows

easily by

Definition 2.1 and the coarea formula

(see

e.g.

[Z],

5.4.4).

D

LEMMA 2.4.

Let a, b

E R and v E

GSB V (a, b).

The

previous lemma,

when

applied

to any function in

GSB V 2 (a, b)

and

to its

approximate derivative,

shows that in dimension one the

strong

formula- tion

( 1.1 )

and the weak formulation

(1.4)

coincide.

Now we may define the

following

function spaces; even if we will use

only

in the

following,

we recall the definitions of various spaces related to bounded second

derivatives,

to avoid confusion with other authors’

notations.

DEFINITION 2.5. We set

Notice that Dv = Vv in

SBH(Q), Dv =A

Vv in and in

GSB 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]

as

We 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

are

clearly

defined

by

the context.

(8)

The

following

two theorems have been

proved

in

[CLT5]

with the inessential restriction p = q = 2. In the first statement we use the

following

sequence of smooth truncation functions:

for every

integer k &#x3E;

2. The

property

v E

GSB V (Q) (see

Definition

2.1 )

is

clearly equivalent

to the

requirement

(see [A2],

Section

1 ).

THEOREM 2.8

(Interpolation inequality).

Let n E l~ and let

Q

C JRn be a cube

with

edges of lenght

I

and parallel

to the coordinate axes, p &#x3E; 1 and v E GSB

V 2 ( Q).

Then

for

every i =

1,

... , n the

following inequality

holds true

THEOREM 2.9

(Existence

of weak

solutions).

Let Q c JRn be an open set.

Assume

(1.2)

with g E

Lq (0).

Then there is Vo E

X (Q)

such that

We recall that

assumption fl

a

2~8

is necessary for lower

semicontinuity (see [BZ], [Co]).

3. -

Preliminary

results

In this section we prove some technical results.

LEMMA 3.1

(Density

upper

bound).

Let v E

minimizer for the functional (2.1 ) with

g E

(r 2: nq ).

Then

for

every 0 p 1 and

for

every x E S2 such that

B p (x)

C S2 we have

where (

(9)

PROOF.

By minimality

of v for .~’ we get

.~’(w),

where w =

VXQBB,(,).

· Since

Sw

U

Svw

c

((Sv

U

Svv) B B,(x))

U

a Bp (x)

and

taking

into

account

f3

a,

by

subtraction we obtain

hence, by

the

assumptions

on T and p, we achieve the

proof.

C

LEMMA 3.2. Let Q C R" be an open set and let

Ko, K1

1 C be Borel sets with

Ko

U

K,

closed. Let v E

B (Ko

U

K1 ))

and let v be

approximately

continuou6

in S2

B Ko.

Assume that

then r

PROOF. The function v is

obviously

in

Lq(0) and, by

Lemma 2.6 in

[CLT3],

we have ~v E

So, by

Lemma 2.3 in

[DCL],

the

proof

will be

achieved as soon as we show that for every cube

Q

c Q with

edges parallel

to

the coordinate axes and for every

integer k &#x3E;

2 we E

(possibly

not

uniformly

in

k, Q),

where satisfies

(2.2).

Fix

Q

c Q as above and i E

{ 1, ... , n }, then, by

Theorem

2.8,

we obtain

the

following interpolation inequality

where 1 is the

edge length

of

Q.

Hence v E

X (Q)

and the other assertions

follow

immediately.

0

REMARK 3.3.

By

Theorem 2.9 and Lemma 3.2 we obtain

immediately

that

min

.~’(v) inf f F(Ko,

"

Ki, v) : Ko, KI

C JRn Borel sets,

Ko

U

KI closed,

v E

c2(Q B

U

Ki)), v approximately

continuous

on Q B Ko } .

LEMMA 3.4

(Scaling).

Let v E For À &#x3E; 0 and

for

every

x E

BI

set v

and,

Then Vr E

PROOF. Follows

immediately by change

of variables.

(10)

DEFINITION 3.5. A function v E

X (Q)

is a local minimizer of

(2.1 ) if,

for

every

compact

set T C

Q,

Actually

the infimum in the Definition 3.5 is a minimum due to Theorem 2.9 and to the fact that

{z

e

X (S2) :

z = v

T }

is closed in

LEMMA

3.6

(Matching).

Let 2 : and

Then, 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 such

that

B t (x )

C Q. Then

for

every 8 E

(0, 1)

there exist c =

c (8, p, n)

&#x3E; 0 and a

cut-o, ff function 1/1

E

C2 0 (Bt (x)),

with

1/1

=- 1 in a

neighborhoud of

such

that, by setting

U =

1/Iv

+

( 1 - ~ ) u,

we have

PROOF. To

simplify

notation we consider x = 0. We fix 8 E

(0, 1)

and

. Let

and *j ( j

-

0,...,

N -

1)

cut-off functions

between Bj

1 of class

C2

such that and ! in

(where

and define

(11)

Then, by setting

a 0 b

= 1 (a ®

b + b ®

a),

we get, for every

j,

Since

Cj

f1

Cj+l = 0, by adding

with

respect to j

from 0 to N -

1,

we

get

min

By choosing

the

index j

for which the above minimum is

achieved,

we set

so that

hence the thesis follows with o

LEMMA 3.8. Let n &#x3E;

2,

p &#x3E; 1 and let Q C JRn be open. Let i such

that, for

every compact set T C

Q,

Then

for

PROOF.

Apply

the same

argument

of Lemma 2.6 in

[DCL].

(12)

4. -

Compactness

and lower

semicontinuity

We prove a Poincare type

inequality

in the class GSB V which extends Theorem 3.1 in

[DCL] allowing

a more

general

truncation. We

enphasize

that

v E does not even entail that either v or Vv

belongs

to

Let 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 in

general

it has no

relationship

with

f B dy . Obviously

we have

med(vXB~E

+

med(v, B) XE, B) = med ( v , B )

for every E C B. For every v E

GSBV(B)

and a E R with

n -

, we set

where yn is the

isoperimetric

constant relative to the balls of

R",

i.e. for every Borel set E

0 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 &#x3E; 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 defined

componentwise.

THEOREM 4.1

(Poincaré

type

inequality).

Let B C JRn be an open

ball,

n &#x3E;

2,

p &#x3E; 1. Let v E

GSBV (B)

and a E R with

let r~ &#x3E; 0 and

T (v,

a,

q)

as in

(4.1).

Then

(13)

If

p n,

setting

, we have also

If

p &#x3E; n,

for

eve ry ~ we have also

PROOF. We may assume that

med(v, B) =

0 and the

right

hand sides are

finite. If 0 and a = 0 then V E

T (v, 0, r~)

= v and

the

inequalities

are well-known.

By

Lemma

2.3,

E

SBV(B)

and we

obtain

By

the coarea formula of Lemma 2.3 and the

isoperimetric inequality

we obtain

By

the

assumption

on a and

by comparison

with

(4.7)

in the case t7 = 0 we

have

(14)

hence

By

substitution in

(4.7),

we obtain for every

so

(4.4)

follows

by

Holder

inequality. By (4.8)

and

(4.10)

we

get

also

By

the classical Poincare

inequality (see [F],

pag.

504) applied

to

we

get

We define

Then, by taking

into account

(4.1), (4.2)

and

(4.4),

we have for every

Hence if p =

1, by (4.13 )

with s =

1 * , (4.12)

and

(4.10)

for

T ( v ,

a,

0)

we get

(15)

so that

(4.5)

is

proved

in the case p = 1. We focus now the case

We set

-*

and we notice that w E

SBV(B), med(w, B)

=

med(v, B)

and

By plugging

w in

(4.12)

and

(4.10) with 17

= 0 and

by

Holder

inequality

Dividing by

which is finite since

T (v,

a,

0)

is

bounded,

we

get

By (4.13)

with s =

p *

and

(4.14)

we obtain

If p &#x3E; n, fix and set

r = 2013~.

Then r n and r * = s,

hence

by (4.5)

and Holder

inequality,

still

assuming med(v, B)

= 0 and

setting

, we have

and the

proof

is

completed.

(16)

We show

that,

beside

(4.2),

also the

perimeter

of the set

can be estimated for many suitable 1] E

(0, 1).

LEMMA 4.2. Let B C R" be an open

ball,

n &#x3E;

2,

s &#x3E; 1. Let v E

GSB V (B)

and a E R with

(

Then there exists q E

(0, 1 )

such that

Actually

: both

(4.15)

and

(4.16) hold ) I

PROOF.

By

coarea formula of Lemma 2.3 and

by

the definition of

SBV (B)

and

analogously

We

get

the thesis

by Chebyshev

and Holder

inequalities

and

by (4.2).

D

For any

given

function in

GSB V,

we define an affine

polynomial

correction

such that both median and

gradient

median vanish.

Let C Q and V E for every y E R’ we set

(17)

Since

med(v -

c,

Br (x ) )

=

med(v, B,. (x ) ) -

c for every c E R and

then we have say

We notice that there are v such that

med(v, # med(Px,rv, B,(x)),

take

e.g.

v(x)=

where H is the Heaviside function.

In the

following

we denote

by s’

the

conjugate exponent

of s in the Holder

inequality.

THEOREM 4.3

(Compactness

and lower

semicontinuity).

Let

2,

Br (x )

C be an open

ball, (Vh)

C

GSBV2(Br(x)).

Set

L h

Assume

Then there exist Z E

W 2’ p ( Br (x)),

a sequence

(Zh)

C GSB

V 2 ( Br (x))

and a

positive

constant c

(depending

on the

left

hand side

of (4.19))

such

that,

up to

a finite

number

of indices,

Moreover there is a

subsequence

such

that for

every

(18)

PROOF. We can assume x =

0,

0 and we extract

subsequences

without

relabeling.

We use

properties

of functions that hold true

only

up to a finite number of

indices,

hence

by (4.20)

we can assume that

Arguing separately

on

each component Of V Vh

we deduce that V k E

{ 1, ... , n },

there exist

E

(0, 1)

and c

depending

on the l.h. s. of

(4.19)

such

that

Inequality (4.28)

follows

by (4.2),

while

(4.29)

follows

by

Lemma 4.2 with

s = p

applied

to

Vkvh

and

1) through (4.19).

We define small subsets

Eh

C

Br

where we have to

modify vh

in order

to force boundedness

of Vvh,

and we

perform

a former

tuning

of Vh. To this aim set

Since

med(vh, Br ) = 0

then

med(wh,

and

by

the definition

med(Vwh , Br)

=

med(Vvh, Br)

= 0.

By (4.29) Eh

has finite

perimeter,

hence

by

Lemma 2.3

we have wh E

GSB V2 (B,)

and

V Wh

E

SBV(Br,

n

L’(B,, JRn).

Then

by 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)

we

(19)

By (4.32), (4.9)

and

by

the

assumptions (4.19), (4.20)

and p &#x3E; n, we get

Now we want to force boundedness of

(wh). By (4.32)

we can assume

and there are ?7h E

(0, 1)

and a constant,

depending

on the l.h.s. of

(4.19),

such that

Inequality (4.36)

follows

by (4.2),

while

(4.37)

follows

by

Lemma 4.2 with

s = p,

applied

to Wh,

taking

into account

(4.32)

and

(4.34).

Then we define

and we

perform

the

following tuning

of the sequence

We notice that zh E and

Hence

(4.21 )

and

(4.22)

follow

by (4.28), (4.36),

and

(4.29), (4.37) respectively,

taking

into account the

assumption

p 2: n.

By (4.7), (4.9)

and

(4.34)

we have

(20)

Moreover, by (4.39)

and

(4.34),

and

by (4.32), (4.39)

we get

hence

by (4.11)

and the

assumption p

we have

Since 0 17h

1, by (4.6)

and

(4.41)

By (4.41), (4.42)

and the

compactness

theorem in

applied

to

there exists

f

E such that

By (4.39), (4.19), (4.20)

and Theorem 2.1 in

[All, f

E

SBV(Br, JRn)

and also

hence

f

E

By [B],

Theorem 18 in

Appendix,

and

by (4.34)

we get

(21)

By (4.40), (4.43)

and the compactness theorem in

B V (Br ) applied

to

(Zh) ,

there exists z E

B V (Br)

such that

By (4.39), (4.41)

and Theorem 2.1 in

[Al]

we have z E

SBV(Br)

and also

hence z E and also

by (4.43)

By (4.45)

and

(4.46) f

= Vz = Dz so that z E

W2,p (B,). By

the arbitrariness

of 6, (4.23), (4.24), (4.25)

hold true and

(4.26), (4.27)

follow

by (4.21).

0

5. -

Blow-up equation

The aim of this section is to prove for any minimizer v of

(2.1 )

a faster

decay

estimate of the functional around

points X

such that

THEOREM 5.1

(Blow

up

equation).

Let p &#x3E; n &#x3E; 2 and

B,. (x )

C S2 be an

open

ball, (Vh)

C

X (Q), (~ph )

C let

(ah ),

and

(,c,ch )

three sequences

of positive

numbers with

Ph

ah and let Z E Assume that

Then, for

every p r, z minimizes the

functional

(22)

over all v E such that v = z in

Br (x ) B Bp (x)

and

In

particular

z is a weak solution

of

the

fourth

order

elliptic equation

PROOF. Assume x = 0 and set for

brevity’s

sake. We will extract

subsequences (without saying explicitly

and without

relabeling)

each time

is needed and we will omit the

arguments

ah,

Ph

in First we estimate

and we have

by (iv), (v)

and even

by (v),

Hence

and

then, by

Fatou’s

lemma,

By (ii)

and

(iii),

the

assumptions

of Theorem 4.3 are

satisfied,

so that we can choose zh and z as like as in Theorem 4.3 and z turns out to be the same of

assumption (iv). By (4.25), (5.2)

and

(iii)

we obtain

To achieve the

proof

we want to show that for almost every p r , for every v E with v = z in

Br B Bp

(23)

By monotonicity (o

is continuous for a.e. p E

(0, r).

Assume

by

contradiction that there exist s r, v

E W2,P(Br)

and E &#x3E; 0 such that cv is continuous at s,

v = z in and

As like as in Theorem

4.3,

we set

Lh

=

1t n-l (SVh

U and

Ah

=

Eh

U

Wh

=

(vh - PVh))-

To

get

a contradiction we

paste together zh

+

PVh and Vh along

the

boundary

of a

suitably

choosen ball and then we

join

the new function

with v

(which

reduces the energy in

Bs).

To this

aim,

we remark that for a.e.

p E

(0, r)

we have

and, by (4.22),

Integrating

in

polar

coordinates and

by

the

isoperimetric inequality

we get

Since

by (iii)

the sequence

~ah Lh ~

is

bounded,

then

by (ii)

Hence,

for a.e. p E

(0, r),

we have

Now, by

the

continuity

of cv at s and

by (5.4),

we choose t E

(s, r)

such that

and we

glue together vh

and Zh +

~vh by defining

By

Lemma

3.6,

u h E and

(24)

We join

u h and Let

1frh

be the cut-off functions

between BS and Bt provided by

Lemma 3.7 and set

Then

Uh belongs

in

Br B Bt

and we

have, by

the

minimality of vh

in

Bt, by v

= z

on B, B BS

and

by (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 have

Then

by

the arbitrariness of 3 and

by (5.3)

and

(5.5)

we get

contradicting

the

monotonicity

of cv. 0

We recall the

following

well-known result for the biharmonic operator. For the

proof

we refer to

[G],

Ch.

III,

sect. 2.

THEOREM 5.2

(Estimate

on the solutions of the biharmonic

equation).

Let B,

C R’ and let u E solution

of

Then the

following inequality

holds:

where cn is an absolute constant

depending only

on the dimension.

(25)

REMARK 5.3.

For q

&#x3E; 1 there exists a constant c

depending only

on n and

q such that for every affine

function ~

and every 0 p r we have

hence there exists a constant cn,q such that for every biharmonic function u and for every affine

function ~

we have

THEOREM 5.4

(Decay).

Assume

(1.2)

with n = p = 2. For every k &#x3E;

2,

ri, a E

(0, 1 )

with

r

there is 80 &#x3E; 0 such that

for

every 8 E

(0, EO]

and

.4

is a local minimizer it, a,

f3, Q)

with

and

then

PROOF. Assume that the theorem is false. In such case, there exist k &#x3E;

2,

77, Or E

(0, 1)

with

r0’ £,

a sequence

of 8h

&#x3E; 0 with

limh 8h =

0 and

C2.a

local minimizers of

(.,

JL, a,

~, Q)

such that

and

By translating

into the

origin

and

rescaling

we set

where

(26)

The

functions vh

are local minimizers in

B1

for , where

By

Lemma 3.4 we get

hence

By (5.9)

and

by

Theorem

4.3,

up to a

subsequence

that we do not

relabel,

there

exists z such that

Now we

verify

that the

functions vh

and z

satisfy

all the

remaining assumptions

of Theorem 5.1.

Assumption (i)

follows

by

Lemma 3.4 and

(ii)

follows

by (5.10).

We prove

(iii):

let

(tj)

be a sequence of radii dense in

(0, 1). By (5.9), by extracting

for

any tj

a

subsequence of vh

and

by diagonalizing,

there exists for

any tj

Since tj

-~ is monotone

nondecreasing,

hence continuous up to a countable set, then the above limit exists for almost every

radius p

E

(0, 1).

To

verify (v)

of Theorem

5.1,

we prove first that

By

Lemma 3.1

(hh)

is

bounded,

so our claim is obvious

if q

&#x3E;

2,

and in the case q 2 it follows

by

the

assumption

ph

8h k .

Moreover,

by changing

variables and

using

Holder

inequality,

we

get

(27)

hence

Finally

we prove that is bounded in

Bl .

Since are affine

functions,

it will be

enough proving

that ph is

bounded,

and the

convergence follows

possibly extracting

a

subsequence.

In

fact, referring

to the

functions Zh

introduced in Theorem 4.3 and

setting Ah =

-~

for every h

big enough

we have

due to

(5.9)

and

(5.12). By

Theorem 5.1 we have

On 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 in

B,

since we have v E

W2,2 (B)

so that

by

the standard

(28)

regularity theory

we obtain D E

C2(B) (see

e.g.

[B]

for the case q &#x3E; 1 and use an

approximation argument for q

=

1).

Hence we have v E

C2(Q B

U

We now estimate ’ Set

We prove that

Qo

is open. In order to

apply

Theorem

5.4,

we fix k &#x3E; 2 and r~, o~ E

(0, 1)

with

r~~ ~2 ;

; let 80 be as in Theorem

5.4,

let x E

Qo

and let

r &#x3E; 0 be such that

We show that If z then

hence we may

apply

Theorem 5.4

inductively

to obtain

for every h E N. For every 0 t qr there

exists j

such that

so that

~ , , ,

then

passing

to the limit as t - 0

(so that j

- we get z E

S2o.

Since

Sv

U is

countably 1) rectifiable, by

Theorem 3.2.19 in

[F]

we have

H1«Sv

U

Svv)

n

S2o)

= 0 so and

(Sv

U

SVv)

n

Qo

= 0. Since

Qo

is open then U

Sov

= 0.

By

Lemma 3.8 we have

Setting

we have that is

closed,

and ’

hence are ( )

rectifiable,

moreover

and, by

Remark

3.3,

we conclude that

(Ko, K1, C)

is a minimizer for F in the

class of the admissible

triplets.

D

Theorem 1.2 follows

immediately by

Theorem 1.1

choosing

K =

Ko

U

Kl

and

taking

into account the

assumption

a =

~8.

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