R ENDICONTI
del
S EMINARIO M ATEMATICO
della
U NIVERSITÀ DI P ADOVA
M ARIO M ARINO
A NTONINO M AUGERI
Partial Hölder continuity of the spatial derivatives of the solutions to nonlinear parabolic systems with quadratic growth
Rendiconti del Seminario Matematico della Università di Padova, tome 76 (1986), p. 219-245
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Continuity Spatial
of the Solutions
toNonlinear Parabolic Systems
with Quadratic Growth.
MARIO MARINO - ANTONINO MAUGERI
(*)
SUNTO - Si considerano soluzioni u E
L2( -
T, 0,H2(D, RN) )
nHi(-
T, 0,L2(D, RN) )
f1CO,V(Q, RN),
N > 1, 0 y 1, del sistema non linear, in forma didivergenza,
e si dimostra,
nell’ipotesi
che il sistema sia fortementeparabolico
ad anda-menti
quadratici,
laparziale
hölderianità delle derivatespaziali Diu
di u.1. Introduction.
Let S2 be a bounded open subset of with
n, ~ 2,
whoseboundary
a S2 is
sufficiently smooth,
for instance of class C3. Let T > 0 andQ
=Q x (- T, 0).
If x =(Xl’
X2, ... ,xn )
is apoint
of Rn and t is areal
number,
we set X =(x, t).
By a)
we denote the subset of R~+1(*)
Indirizzodegli
A.A.:Dipart.
di Matematica, viale A. Doria, 6- 95125 Catania.Lavoro
eseguito
con contributo finanziario del M.P.I, e nell’a~mbito del G.N.A.F.A. del C.N.R.where X° =
(xo, to),
a > 0 andor)
is the(open)
ball of Rn centeredat x° and with radius a.
If u is a function from
Q
to RN( N
is aninteger >1)~
we setDu =
(D~u ~ ... BDnu)
whereDi - Clearly
Du E RnN. We shalldenote
by
p = thetypical
vector of R~N.We consider in
Q
the second order non-linearsystem
where
ai(X, u, p), i = 1, 2, ..., n,
andBO(X,
u,p)
are vectors of RNmeasurable in X and continuous in
(u, p ) .
We suppose that
system (1.1)
isstrongly parabolic, namely
thatv ectors
ai(X, 2c, p), i
=1, 2,
... , n, are differentiable withrespect
to p and there exists a constant v > 0 such thatfor every
system ~~ i~~ -1,..., ~z
of vectors of RN and everyE Q X RN X RnN.
If vectors ai and BI have « controlled
growth (see [7],
n.1), by
asolution to
system (1.1)
we mean a vector ue L2(- T , 0,
m L~~’ (- 1, 0, L2 (Q, RN) )
such thatIn the case of ((natural))
growth (see
n.4),
we shall say thatu : Q -
RN is a solution tosystem (1.1)
if U EL2(- T, 0, H2(Q, RN))
nand u satisfies
( 1.3 ) ,
y(1)
( ~’ ~ )~;
are the scalarproduct
and the norm inRk, respectively.
We shall
drop
thesubscript k
whenever there is no fear of confusion.(2)
Throughout
this paper, the Holdercontinuity
is related to the para-bolic metric
In the work
[7]
S.Campanato
hasproved
H61dercontinuity
andpartial
H61dercontinuity
results for the solutions ofsystem (1.1),
under the
assumption
that the vectors at Z and B° have controlledgrowths.
The aim of this work is to
study
thepartial
H61dercontinuity
in
Q
of thespatial
derivatives of the solutions tosystems
oftype ( 1.1 )
with non controlled
growth.
In the case of non linear
elliptic systems,
somepartial
H61dercontinuity
results for thegradient
of the solutions aregiven
in theworks
[3], [8]
and[4].
We start with the
following
remark. Let us suppose that thesystem (1.1)
has naturalgrowth
and that the vectorsa i ( X, u, p ) , 2 = 1, 2, ... , ~12, belong
to Let u EL2(- T, 0, H2(Q, RN) )
nHi(- T, 0, Z2( S~, RN) )
nRN),
0y 1,
be a solution ofsystem ( 1.1 ) .
Fixed an
integer s,
in(1.3)
let us assumeWe obtain that u is solution of the
system
Because
we can write
(1.5)
in thefollowing
waywhere
If now in
(1.6)
we add withrespect
to s and set U =Du,
we ob-tain that U
belongs
to.L2(- T, 0, linN) )
and verifiesi, j
=1, 2,
... , n, is thef ollowing
matrixwhereas
Fi, i == 1, 2,
... , n, are the vectors of R’zN whosecomponents
are
Let us remark that
system (1.9)
isstrongly parabolic
too. Infactfor every
system ~~t~~,-1,2,...,n~ 77
=(1Ji,11’Y}i,21... iq i, 11), RN,
of vec-tors of RnN we have:
·I:
The matrices are bounded and
uniformly
continuous inQx
X RN X RnN
if such are the derivativesThen the
study
of thepartial
H61dercontinuity in Q
of thespatial
derivatives of the solutions u to the
system (1.1)
is reduced to thestudy
of thepartial
H61dercontinuity
of the solution U = Du ofsystems
oftype (1.9)
with coefficients thatdepend
onX, u,
U.We shall be concerned with this
type
ofsystems
in Section3;
in Section 4 we shall prove a
partial
H61dercontinuity
result for thespatial
derivatives of the solutions to thesystem (1.1)
in the caseof natural
growth. Finally
in the Section 2 we mention a few results that will be used in the next sections.2.
Preliminary
results.See
[5~,
Lemma 2.1.Now let
~°~ , i, j
=1, 2,
... , n, be constant nN X nNmatrices,
suchthat
for some v > 0 and any
system ~~ Z~i =1, 2,..., n
of vectors of RnN. Also let= 1, 2 , ... , n,
be functions in and let V ebe a solution of the
parabolic system
Then we have
LEMMA 2.2. Let
(2.1)
and(2.2)
b esatisfied. Then, f or
every -c E( 0,1 ) ,
and
See
[5 ~,
Lemma 2.11.LEMMA 2.3. Let (p, 1p be
nonnegative functions de f ined
in(0, (1].
Let
M,
B benonnegative
constants. Also let a > 0 and A > 1..Assume thattor
every -r E( 0, 1 )
and e E( 0,
Then there exist oonstants K andC, depending onl y
onA,
a, E, such thatf or
every E( 0,1 )
and e E(0, a).
See
[4], Chap. I,
Lemma 1.11.LEMMA 2.4. Let
functions
99 and Wl benon-negative
in(0, d]
and let OJ!be
nondecreasing; also,
letfunction
W2 benonnegative
andnondecreasing
in
( 0, -~-- 00).
LetA,
a bepositive
constants and let0 ~ ~
a.that
every r E
(0, 1)
and J E(0, Also, that, tor
some E E(0, a - ~ ~,
there is a 6~ E(0, d J
s1tch thatThen ,
Vr E(0, 1 )
wher¡te B =
(I
+A)£X/c.
See
[4], Chap. I,
LemmaFinally,
we need thefollowing interpolation
result.THEOREM E
L9(- 1’, 0, H2(Q, RN))
nHl(- T, 0,
Then
and
where c
depends
on ~~~, 8, y,[u]v,-Q.
The
proof
of this theorem is achievedby a
standardtechnique,
ytaking
into account Theorem 3.111 of[2],
Lemma I of theAppendix
to
[9]
and the results of[12] (see
also Theorem 2.111of [1 ] ~ .
3. Local Zq
regularity
forsystems
oftype (1.9).
We start
by recalling
thefollowing
Zqregularity
result for linearsystems.
R~N ) )
be a solution inQ of
the linearsystem
Here the nN X nN matrices
i, j
=1, 2,
... , n, aredefined
andbounded in
Q
andsatisfy
thestrong ellipticity
condition. Then there exists yo E( (n - 2 ) In, 1)
suchthat, if
we have
(3.3)
and
for
every andSee
[6],
Section4,
Theorem 4.IV.Now we are
ready
to prove,taking
into account Theorem3.1,
thefollowing
Z~regularity
result for non-linearsystems:
THEOREM 3.2. Assume that u is in,
, and U = Du is a solution in
Q
(1)Q(X°,
means that .of system
Here the rtN >C nN matrices
i, j
=1, 2,
... , n, and the nN-vectors.I’i(X,
u,p),
i =1, 2,
... , n, are assumed to be as itfollows: Aii
aredefined
and bounded inQ
an,dsatisfy
thestrong ellipticity condition;
I’i ( X,
u,p)
are measurable in X and continuous irc( u, p)
and have thefollowing growths
Then
(3.7)
and
for every
in
RN),
0 y1,
be such that U = Du is solution inQ
of thesystem (3.4), namely
From Theorem 2.1 of Section 2 it follows
therefore,
for everyinteger j,
Then,
iff
i verifies(3.6), taking
into account(3.5),
it resultsOn the other
hand, by
well-known results(see [13], [14]),
we haveFrom
(3.11 ), (3.12 )
and from Theorem 3.1(applied
toQ* )
we obtain:and,
Now let us estimate the norms of the vectors
Z~ ) , 2
=-1~27
..., 7 it, in theright
side ofinequality (3.14).
Inparticular,
taking
into account(3.5),
we need to estimate theintegral
If j
is aninteger, l C j ~ ~2,
we have:On the other
hand, (2.4)
enables us to writewhere c does not
depend
on (1 butonly
onMoreover we
easily
haveThen from
(3.15), (3.16)
and(3.17)
we obtainfrom
this,
fora ~ 1,
it f ollows thatFrom
(3.5)
and(3 .18 )
we obtain the estimates of vectors Fi inf 26) ~ RnN) .
.Estimate
(3.8) easily
follows from(3.14)
and(3.19).
We need a different version of Theorem 3.2.
We set
f or every
number q
in the intervalI
THEOREM 3.3. Under the
assumptions o f
Theorem 3.2 withwe have
PROOF. Estimate
(3.22)
follows from(3.8)
and from theinequality
It is self evident that Theorems 3.2 and 3.3 also hold for the
2c
E L2( - T, 0, RN))
nHi(- T, 0, L2(Q, RN))
r1RN),
0 y1,
such that U = Du is a solution inQ
of asystem
of thetype (1.9)
with
u, p), i, j
=1, 2,
... , n, bounded nNxnN matrices definedin and such that
for every
system {~},=i,2,...~
of vectors of RnN and every(X, u, p)
EE Q X RN X RnN.
4. Partial Holder
continuity
of thespatial
derivatives of the solutionsto
system (1.1).
be a solution of the non-linear
system
where
~(~~jp)~==l,2,...~
andB°(x, u, p)
are vectors of RNmeasurable in
X,
continuous in( u, p )
andverifying
thefollowing
conditions:
there exists a constant v > 0 such that
(4.4)
the9~’/~~~~==1~2~...~~7~~=~2~..~~
are uni-formly QxRNxRnN;
and
it results
with
Set U =
Du,
then we havetl.lso, taking
into account what wepointed
out in Section1,
U issolution of the
system
where
Aii, i, j =1, 2, ... , n,
is the matrix definedby (1.10)
and
~1.7),
andFi,
i =1, 2, ...,
n, is the vector of R~Ngiven by
The
assumptions
on the vectors aiimply
that the matricesAij(X, u, p ),
=1, 2 7 * * , n,
areuniformly
continuous and bounded inQ X X RN X RnN,
andsatisfy
thestrong ellipticity
condition(3.23).
Con-sequently
there exists a bounded continuous function defined for which isincreasing,
concave, such that = 0 andY E Q,
andwhere
6 (X, Y)
is theparabolic
distance:The vectors
== 17 2,...., n,
are measurable inX,
con-tinuous in
( u, p )
and have thefollowing growth
where
By
Theorem 2.1 we have:and
From
( 4.12 ) ,
written for 8 =4,
it follows Vr E(0, 1 ) :
and hence
Let us recall that if
and
the following inequality
where c
depends
on the distance ofQ(X°, or)
from theparabolic
bound-ary of
Q (g)
and on theL2(Q)-norm
ofto.
From
(4.14)
and Lemma2.1,
we deducewhere the constant c
depends
on the usualarguments.
Now we are
ready
to prove thefollowing
where q is an
arbitrary
number in the~
and aredefined as in (3.20)
and(3.21).
PROOF. Consider
Q(X°, 20’)(ÇQ
We set U = Du.Taking
into account the remark made at the
beginning
of thisSection,
wehave that 17 is solution of
system (4.8)
andbelongs
to the spacethen,
inQ(X°, a),
U can be written in the formwhere
is the solution of the
problem
whereas
is solution of the
system
By
well-known results(see [13]),
theproblem (4.17)
admits anunique solution;
this solutionbelongs
to the space.L2(B(x°, a), RnN)~
and thefollowing
estimate holds :Moreover from
(4.9), (3.22)
,taking
intoaccount the fact that oi is bounded and concave
(’),
it followsNow the
following
estimate holds for the termon the other hand
hence we obtain
From
(4.19), (4.20)
and(4.21), taking
into account the fact thatand ~n+2,
we deduceFrom
(4.22)
and Lemma 2.1 itfollows,
Vr E(o, 1]:
If we use Lemma
2. 2,
then weget
thefollowing
estimate onVr e (0,1)
andand, denoting
from
(4.11),
it followsHence,
VO and Vr E( 0, 1 ) ,
we haveNow,
Vr E(0, 1)
and 0 ~ c a, thefollowing
estimate is true:in
fact,
from(4.13) (written
for i-= o),
we deducehence, adding
the term(ro)I
to the first and the lastside,
the ine-quality (4.26)
follows.From
(4.25), (4.26), by
virtue of Lemma2.3,
it follows that Vr Ee (0,1)
andSince U == cu
+
W in(1),
from(4.23)
and(4.27)
weget
in astandard way that Vr E
(0, 1)
and VA E(n, ~)
whereas from
(4.26)
we have Vr E(0, 1)
Now let us show that also the term to the
right
side of(4.28).
Q(is less or
equal
is a solution of the
system ( 4.1 ) ,
we haveand
hence, by
virtue of thegrowths (4.5)
and(4.6),
and hence
From
(4.13) (written
for 1. = weget
from
(4.28),
it follows afterwardsThen,
from(4.31), (4.32)
and(4.33),
w-e obtainVT=(0,1)
andE
(~z, ~):
The estimates
(4.28), (4.29), (4.34)
holdtrivially
also for t E[1, 2 ) ;
then
adding
suchinequalities
we deduce(0, 2 ) , VÂE(n, ~) , VQ(X°, 2o) C Q, o 1
and the lemma follows.
Now we can
easily
achieve thepartial
H61dercontinuity in Q
ofthe derivatives
Diu
of the solutions to thesystem (4.1 ) making
useof the some
technique
used in Section 3 of[51.
Let
It is well-known that
and
hence
We can
give
a more accurate estimate of the measure ofQo, considering
a suitable Hausdorff measure. From(3.10)
and(3.13),
viaH61der
inequality,
weget J) e Q :
for every
Moreover from
(4.30),
that holds for~)
withQ(X, a) Cc Q,
we deduce
after
which, taking
into account(4.35)
and(4.36),
it followsUsing
Lemma 2.111 of[7] ] (see
also[9],
Lemma2.11)
weget
and
hence,
because of(4.36)
and(4.37),
From
(4.35), (4.36), (4.37)
and(4.38)
it followsconsequently, by
a well-known result(see [11])
where is the
(n +
2 -q)-dimensional
Hausdorff measure withrespect
to theparabolic
metric(4.10).
Now, taking
into account Lemmas 4.1 and 2.4 andusing
the sometechnique
of[5] (Lemma 3.11),
we can prove that and V Â E(n, ~)
it ispossible
to find 1 and r > 0 withQ(X°, r + aa)
ccQ
such that
r)
and Vr E(0, 1)
In
particular, Qo
is closed inQ.
Then from
(4.39)
andtaking
into account the definition ofø,
it follows that if XOE E
Q (X °, r ) ,
r E(0, 1)
Finally
from(4.15)
we deduceThe
pre;ious inequality
ensures that(see ~10 ] ~ :
Therefore we have
proved
thefollowing
RN))
r10°,1’( Q, RN),
0 y1,
be a, solutionof
thesystem (4.1).
Letconditions
(4.2)-(4.6)
befulfilled.
Then there exists a setQoc Q,
closedin
Q,
such thatand
REMARK 4.1. In the case of natural
growth,
theproblem
of thelocal
differentiability
of the solutions u EL2 (- T, 0, RN))
nn
C°,%(Q, RN),
0y 1,
to thesystem (4.1)
is open. In the case of controlledgrowth,
thisproblem
is to consider solved.REMARK 4.2. The
assumptions
of Theorem 4.1 on the matricesAij
do not
imply
thoserequired
in Theorem 5.1I of[9];
hence our resultis not a
particular
case of the results obtained in[9].
BIBLIOGRAPHY
[1] S. CAMPANATO,
Equazioni paraboliche
del secondo ordine espazi £2,03B8(03A9,
03B4),Ann. Mat. Pura
Appl.,
73(1966),
pp. 55-102.[2]
S. CAMPANATO,Maggiorazioni interpolatorie negli spazi H03BBm,p(03A9),
Ann.Mat. Pura
Appl.,
75 (1967), pp. 261-276.[3] S. CAMPANATO, Partial Hölder
continuity of
thegradient of
solutionsof
some nonlinear
elliptic
systems, Rend. Sem. Mat. Padova, 59(1978),
pp. 147-165.
[4] S.
CAMPANATO,
Sistemi ellittici informa divergenza. Regolarità
all’interno,« Quaderni» Ann. Scuola Norm.
Sup.
Pisa, 1980.[5] S. CAMPANATO, Partial Hölder
continuity of
solutionsof quasilinear
para-bolic systems
of
second order with linear growth, Rend. Sem. Mat. Padova, 64 (1981), pp. 59-75.[6] S. CAMPANATO, Lp
regularity
andpartial
Hölder continuityfor
solutionsof
second orderparabolic
systems withstrictly
controlled growth, Ann. Mat.Pura
Appl.,
128 (1981), pp. 287-316.[7] S. CAMPANATO, On the nonlinear
parabolic
systems indivergence form.
Hölder continuity and
partial
Höldercontinuity of
the solutions, Ann.Mat. Pura
Appl.,
137 (1984), pp. 83-122.[8] S. CAMPANATO - P. CANNARSA,
Differentiability
andpartial
Hölder con-tinuity of
the solutionsof
nonlinearelliptic
systemsof
order 2m with qua- draticgrowth,
Ann. Scuola Norm.Sup.
Pisa, (4), 8 (1981), pp. 285-309.[9] P. CANNARSA, Second order non variational
parabolic
systems, Boll. Un.Mat. Ital., (5), 18-C (1981), pp. 291-315.
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Spazi £(p,03B8)(03A9, 03B4)
e loroproprietà,
Ann. Mat. PuraAppl.,
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H1,p esingolarità
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bounded mean oscillation, Comm.Pure
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Math., 14 (1961), pp. 415-426.[13] O. A. LADYZEKSKAJA - V. A. SOLONNIKOV - N. N. URAL’CEVA, Linear and
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Vol. 23, Amer. Mathem.Society,
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Equations differentielles opérationnelles
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