A NNALI DELLA
S CUOLA N ORMALE S UPERIORE DI P ISA Classe di Scienze
L AVI K ARP
On Liouville type theorems for second order elliptic differential equations
Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 4
esérie, tome 22, n
o2 (1995), p. 275-298
<http://www.numdam.org/item?id=ASNSP_1995_4_22_2_275_0>
© Scuola Normale Superiore, Pisa, 1995, tous droits réservés.
L’accès aux archives de la revue « Annali della Scuola Normale Superiore di Pisa, Classe di Scienze » (http://www.sns.it/it/edizioni/riviste/annaliscienze/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une infraction pénale.
Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.
Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
http://www.numdam.org/
Order Elliptic Differential Equations
LAVI KARP (*)
0. - Introduction
The classical Liouville’s theorem asserts that if u is a harmonic function in
Rn,
andu(x) - (0 ~ ê 1) as Ixl
-~ oo, then u is a harmonicpolynomial
ofdegree
m.In this paper we prove the
analogous
result for thefollowing
class ofsecond-order
uniformly elliptic
operators: ,(i)
P = A +Q,
whereQ
is anoperator
with variables coefficients which havea certain
decay
to zero atand
(ii)
P is subcritical in Rn.If the
operator P
admits apositive
Green’s function(fundamental solution) G p (x, y)
in Rn, then P is subcritical in In order toclarify
theconcept
of subcriticaloperators,
theequivalent
conditions provenby Agmon [2]
aregiven
below. Let be the Hilbert space defined
by
thecompletion
ofCol(ii)
in the norm of the Sobolev space
W 1’2(S2).
The Dirichlet realization of P in is denotedby P~
and is defined as follows:Let
IF(,P, 0) =
Espectrum
of - andr(P) = Q
is
compact
in In[2] Agmon proved
that thefollowing properties
areequivalent (see
also[17]):
(a)
P is subcritical in Rn.Pervenuto alla Redazione 1’8 Novembre 1993 e in forma definitiva il 2 Febbraio 1995.
(*) This research was carried out
during
a period in which the author was a research fellow in the Department of Mathematics, Technion - Israel Institute ofTechnology.
(b) r( P )
> 0 and 0 is not aneigenvalue
of P.(c)
There exists u E such that u > 0, Pu 0 and 0 in Condition(c) yields
asimple
wayby
which one can check whether anoperator
is subcritical. Forexample,
if the zero-order term of P isnon-positive
and not identical to zero, then any
positive
constants is a subsolution. Thus P is subcriticalby
the aboveequivalences.
We refer to[17]
and[19]
for further details and referencesconcerning
subcriticaloperators.
A Liouville type theorem for a different class of second-order
elliptic operators
wasproved by
Avellaneda and Lin[3]. They proved
it foroperators
in thedivergence
form and withperiodic
coefficients. Moser and Struwe[15]
gave an alternative
proof
of that theorem. Both methods usehomogenization theory.
Our
approach
is based upon aninvestigation
of the action of P on function spaces withweighted
norms. For aninteger
m, 0 ~ 1 and 0 ~ 1,C2.,,, +6
is the space of twice differentiable functions for which the second derivatives
are 03C3-Hölder continuous. In
addition,
if u EC2,03C3m+e’
thenu(x) =
Du(x) =
andD2u(x) =
asIxl
- oo. denotesthe space of u-H61der continuous functions such that
u(x)
=In this paper we will prove that
is a
surjective
Fredholmoperator
for 0 E 1.Moreover, P
has the same Fredholm’s index as theLaplace operator.
We will show also that the Fredholm’s index of theLaplace operator
isequal
tothe number of
linearly independent
harmonicpolynomials
ofdegrre
m(see
e.g.
[23]). Begehr
and Hile[5]
as well as Friedman[7]
showed that P issurjective
for m -1 and 0 ~ 1.We will discuss the case c = 0
separately,
since in that case theoperator
P in(0.1)
is not Fredholm.Nevertheless,
and inspite
thatdifficulty,
we willprove that
provided
that theperturbation Q decays
faster atinfinity
than it does in thecase 0 6* 1.
We will also consider
weighted
Sobolev spaces. These spaces are definedas the
completion
of withrespect
to the normwhere || . ||
denotes the standardV-norm,
1 p oo and 6 E R. We denote themby
I if k = 0they
become the usualweighted V-spaces
which aredenoted
by L~.
*The operator
was studied
by
severalauthors, including
Lockhart[9],
McOwen[12],
Lockhartand McOwen
[10]
and Murata[16].
Their main result is that if theperturbation
Q
= ~ qa(x)aa
satisfies the condition|a|2
then P = A + Q in
(0.3)
is Fredholm with the same Fredholm’s index as theLaplace
operator. That result is true for -6 -n/p
different from apositive integer
if 6-n/p,
and for s + 2 -n(I - 1 /p)
different from apositive integer
if s >
-n/p.
Since in this paper we assume that P is
subcritical, P
has a Green’s functionG p (x, y).
In[20]
Pinchoverproved
that if the coefficientsof Q
tendto zero in a certain swiftness
as Ixl
-~ oo, thenWe use that estimate to
improve
the above mentioned result as follows: P in(0.3)
isinjective
if 6 >-n/p. Hence,
if in addition 6 + 2 -n( 1 - 1 /p)
is not apositive integer,
thenwhere P * is the formal
adjoint
of P and1 / p + 1 /pl
= 1.We prove those results in > 3. Yet we believe
they
remain true forn = 2.
However,
we refrain to treat the case n = 2 in the present paper.The outline of this paper is as follows: In Section 1 we define norms and the spaces
C~ ~~ ,
and state the main results within them. Section 2 deals withweighted
Schauder estimates. In Section 3 westudy
the behavior of theLaplace operator.
Sections 4 and 5 deal with the null spaces of P and the range ofP, respectively.
In Section 6 we prove the theorems which were stated in Section 1. We will treatweighted
Sobolev spaces in Section 7.Finally,
in Section 8we will indicate the failure of Liouville
type
theorems for fourth-orderelliptic
operators.
List of notations where
{x: Ix - Br
=S2r =
A =
Laplace operator, A~
=BiLaplace operator.
Du =
gradient
of u.The spaces
Cfl’°
and thenorms II .
are defined in Section 1.The spaces
Wkp,6
and thenorm 6,k,p
are defined in Section 7.X)
= null space of operator A :X Y.
dim
ker(A, X )
= dimension ofker(A, X ).
dm -
number oflinearly independent
harmonicpolynomials
ofdegree
m,see
(0.2).
Large generic
constants will be denotedby
C(even
in the same sequence ofinequalities).
1. - Definitions of the norms and statement of the main results Let Q be a domain in 6 E R and let u E We define
For 0 (1 1, set
and define
It is easy to see that for 6 = it + v,
If Q
= R,
we write :=IJUI16,k
and :=lIullö,k,u.
LetCk
andC6°°
be the Banach spaces of all functions u such thatJIU116,k
and arefinite, respectively.
Whenever k = 0 we will not denote it.Now we can state the Liouville’s theorem as follows:
THEOREM
(Liouville).
Let m be anon-negative integer
and 0 ~ ê 1.Then the null space
of
the operatorconsists
of
2
all harmonic
polynomials of degree
m.Therefore,
dim
ker(A, C;;~ê) = dm (dm
isgiven
in(0.2)),
andif
u Eker(A,
thenu E
C2m,,,.
Let
and consider the
following assumptions
on P :where A is a
positive
constant and6ij
are the Kronecker’ssymbols.
here A is a
positive
constant.REMARK. 0 is a sufficient condition for a
uniformly elliptic operator
P to be subcritical in Rn under thedecay assumption (1.9). Indeed,
0implies
that any u - const > 0 is asubsolution, further,
Lemma 5.3 in[20] yields
that constants are not
ground
statesprovided
that P satisfies(1.9).
Therefore P is subcritical.Our main results are:
THEOREM 1.1. Let m be a
non-negative integer
and 0 c 1.Suppose
P
satisfies (1.5)-(1.9),
then P is asurjective
Fredholm operator. Moreover,THEOREM 1.2. Let m be a
non-negative integer
and assume Psatisfies (1.5)-(1.8)
and(1.9)
isreplaced by
Then
COROLLARY. Under the
hypotheses of
Theorem 1.2 :if
u Eker(P, C,2,,,’ ),
then u E
C2.,,,.
We conclude this section with a
proposition
which will be needed in the next sections.PROPOSITION 1.3. Let 6 be a real number.
If
Du EC~_ l,
thenwhere C =
C(b, u).
PROOF.
where3z
lies onthe segment [x, y].
For z in the ball-:/: Ix-yl 4 (x) ~ we
have
4 (x) (z) 4 ~~~° Hence,
with the constant
REMARK. It follows from
inequalities (1.11)
that condition(1.7)
is satisfied if2. -
Weighted
Schauder estimatesThe Schauder estimates
play
an essential role in theregularity theory
ofelliptic operators.
In addition to theregularity,
theweighted
Schauder estimatescontrol the
growth
of the derivatives nearinfinity. Meyers proved
theweighted
Schauder estimates for functions which are defined in a
neighborhood
ofinfinity [13]. Only slight
modifications ofMeyers’
methods arerequired
in order to prove Theorem 2.1 below. A differentproof
isgiven
in[5].
THEOREM 2.1
(Meyers, Begehr
andHile).
Let 6 be a real number.If
theoperator P satisfies
conditions(1.5)
and(1.6),
thenwhere
3. - The
Laplace operator
2
In this section we
study
the behavior of theLaplace operator
in the spaces The results of this section are based on thefollowing
lemma.LEMMA 3.1. Let m be a
non-negative integer
and 0 c 1.(i) If f
EC,,,,,-2,
then there exists u E such thatwhere C =
C(m,
n,c).
(ii) If f
ECm-2’
then there exists u such thatwhere C =
C(m, n).
Moreover, thelog-factor
in that estimate isindispensable.
(iii) If f
ECm-2
and00
where
h(t)
is anon-increasing function satisfying K2.
Then there exists u ECm
such that Iwhere C =
C(m,
n,Kl, K2).
As a consequence of Lemma 3.1
(i),
of theweighted
Schauder estimates(2.1 )
and of the classical Liouville’s theorem we obtain:THEOREM 3.2. Let m be a
non-negative integer
and 0 - 1. Then theLaplace
operatoris a
surjective
Fredholm operator. Its kernel consistsof
all harmonicpolynomials of degree
m, and henceLet
be a
projection.
COROLLARY. Let rn be a
non-negative integer
and 0 c 1. Then thereexists a
positive
constant C such thatThe main device in the
proof
of Lemma 3.1 is a modification of the fundamental solution of theLaplace operator by subtracting finitely
many termsof its
Taylor expansion.
That method was used in[8]
as well as in many other situations.and
Fm
is therrath-order Taylor expansion
of the function x -1’(y - x).
PROPOSITION 3.3. For
Iyl
>where C =
C(m, n).
PROOF. Since
rm(x, y)
is the remainder term of theTaylor expansion (3.4),
For jyj
>21xl
and for 0 t1,~ tx !~ 3 and therefore
Using
the fact that aar ishomogeneous
ofdegree 2 - n - lal
andinserting
theabove
inequality
in(3.7),
we obtain(3.6).
0For any
f
ECm+ê-2, (0 e 1)
withsupp( f )
CS21
:={x : Ixl (
>1 ~
weput
-(3.6) implies
thatKm f
is well-defined.Furthermore,
it is easy to show that=
f
in the sence of distributions(and hence, Km f
is a classical solution iff
is 03C3-Höldercontinuous).
We turn now to estimate thegrowth
ofKmf.
PROPOSITION 3.4. Let m be a
non-negative integer
and 0 e 1. Assumef
Esupp( f )
CQi
1 1. Thenfor x 2::
1where C =
C(m,
n,c).
PROOF. Since
supp( f )
CQl and 1, 1 f (Y) 1 :5
for any 0 ~ 1, where
C(m
+ E -2)
= SoEach of the above terms is now
analyzed separately.
Estimate
of
I: For m + c - 2 > 0,For
?~ + c - 2 0,
Estimate
of
II: Since aar ishomogeneous
ofdegree
2 -n - lal,
we havefrom
(3.4)
Hence,
Estimate
of
III:By Proposition 3.3,
We
complete
theproof by combining
the estimates for I, II and for III.0 PROPOSITION 3.5. Let m be a
non-negative integer.
Assumef
ECm-2, supp( f ) C S21
and 1.Then for lxl
> 1where C =
C(m, n).
PROOF. The
procedure
of thisproof
is the same as the one ofProposition
3.4. The
log-factor
arises in the estimation of II. Other estimates remainunchanged.
PROPOSITION 3.6. Let m be a
non-negative integer.
Assumef
ECm-2, supp( f )
C01,
1and Kl
whereh(t)
is thegiven function
in Lemma 3.1(iii).
Thenfor I x >
1where C =
C(m,
n,Kl, K2).
PROOF. As we did in the
preceding proof,
the outline of thisproof
followsthe one of
Proposition
3.4. This time it differsonly
in the estimation of III.We have
by Proposition 3.3,
PROOF OF LEMMA 3.1. Let v E 0
3(z)
1,3(z)
= 0 forI x
1and
3(z)
= 1 forlxl
> 2. Set(In
case(iii)
weput
in(3.8)).
ThenA~ = (1 - ~)/+~/ = /.
The firstterm of the
right
hand side of(3.8)
isbounded,
while the second one has therequired growth by Propositions
3.4. 3.5 and 3.6. It remains to show that incase
(ii)
thelog-factor
isindispensable.
Letpm(x)
be ahomogeneous
harmonicpolynomial
ofdegree
m andput
Then Au E
Cm-2. Now,
suppose there exixts a solution of theequation
Dul = Auwhich has a lower
growth
then u in(3.9).
As a result u 1 - u isequal
to aharmonic
polynomial
ofdegree
m. Hence u 1 has the samegrowth
as u, butthat contradicts our
assumption
on ul. Theproof
of Lemma 3.1 iscomplete.p
REMARK. Let m be a
non-negative integer
and consider theoperator
We showed that if u is the function
given
in(3.9),
then Au does notbelong
tothe range of
operator (3.10). Thus,
unlikeoperator (3.1 ) (for
0 61), (3.10)
is not
surjective. Furthermore,
we can deduce from the above that the range of(3.10)
has an infinite co-dimension. I do not know whetheroperator (3.10)
hasa closed range.
The lemma below will be needed in Section 5. Its
proof
is similar to theproof
of Lemma 3.1(iii)
and it also relies on theweighted
Schauder estimates(2.1 ).
We leave theproof
for the reader.LEMMA 3.7. Let m be a
non-negative integer.
Assumef
Esupp(f)Ci2,=Ix : lxl > r}
and whereh(t)
isthe
function given
in Lemma 3.1(iii).
Then there arepositive
constantsK3
andK4,
and u EC2m,"
such thatwhere
4. - The null spaces of
elliptic operators
in RnNirenberg
and Walker studied the null spaces ofelliptic operators
inweighted
Sobolev spaces[18].
Their resultsinspired
us to showTHEOREM 4.1. Let m be a
non-negative integer
and 0 ~ 1.If
Psatisfies
conditions( 1.5)-( 1.7),
then operatorhas a
finite
dimensional null space.PROOF. We first prove the theorem for 0 e 1. We do it
by showing
that any bounded sequence C has a
Cauchy subsequence
For the rest of this section we will not differ between sequences and
subsequences,
and all of them will be denotedby
It follows from
(1.7)
that for anypositive
p there exists r such thatr will be determined later on.
We denote
by Ck,, (Br)
the space ofkth
differentiable functions in the ballBr equiped
with the standard normClearly
there are two constantsc(r, 6)
andC(r, 6)
such thatBy
thatequivalence
andby
theweighted
Schauder estimate(2.1 ),
Let 3 be
infinitely
differeniable function such that 0v(x) _
1,3(z)
= 1for Ixl
r andsupp(3)
cB,, 1.
Notice that for any u Eker(P, C,’ ,," ) +6
we haveby (2.1 )
and(4.3),
Let now be a sequence in with I. Then
(4.4) implies
that 1 is bounded in andby
thecompactness
of theembedding (cf. [ 1;
Theorem1.31]),
1 is aCauchy
sequence inBy
the laterinequality,
1 is aCauchy
sequence in and it is bounded in
We turn now to show that
{(l-~)~}~i is
aCauchy
inBy inequality (3.3),
weget
that for any u EBy Proposition 1.3, (1.4)
and(4.2),
Thus, choosing
rsufficiently large
so thatpCC2 1/2,
we obtainby (4.5)
thatfor any u E
ker(P,
The sequence
{A((l - (1 -
1 issupported
inB,,,
and it is bounded in Hence it is aCauchy
sequence inUsing
theequivalence (4.3),
the fact that1 is Cauchy
inC,2,,,’ ,
and thecompactness
ofnm,
we obtainby (4.6)
that{(1 -
i isCauchy
inC,2,,,’,. Therefore,
Cauchy
sequence in that space and thiscompletes
theproof
in thecase 0 e 1. Fore = 0 we have
by
the inclusion C5. - The range of
elliptic operators
In order to show that
operator P
= A +Q
issurjective,
allassumptions (1.5)-(1.9)
on P have to be fulfilled. Condition(1.8) implies
that P has a Green’s function In[20]
Pinchoverproved
that if in addition P satisfies thedecay assumption (1.9),
thenG p (x, y)
isequivalent
to the Green’s function of theLaplacian,
whichimplies
the existence of apositive
constantCl
such thatInequality (5.1 )
is the reason forconsidering
Rn with n > 3 in thepresent
paper.THEOREM 5.l. Let m be a
non-negative integer
and 0 e: 1. Assume Psatisfies (1.5)-(1.9),
then -is a
surjective
operator.PROOF. We write P = A+
Q
+Q2, where Q’
i =E (i = 1, 2)
|a|2
supp(Q 1)
CB,+,
and CQr.
As we did in theprevious section,
wehave
by Proposition
1.3 and(1.4)
thatif
Therefore,
in view of(1.7)
we may choose r so that6C2
issufficiently
smallfor A +
Q 2 being
Fredholm with the same Fredholm’s index as theLaplace
operator. Since the
Laplace operator
issurjective (Theorem 3.2),
and since(cf. [22;
page115]),
it follows that0 + Q 2
issurjective. Hence,
for anyf
eC~+ê-2
there is v E which is asolution of the
equation (A+
=f.
Let be the Green’s function ofP and set ..
then P w =
Putting u
= v - w,yields
Thus,
in order tocomplete
theproof
it remains to show that w EC;~ê. By Proposition 1.3, (1.4)
and(1.6),
where A is the constant in
(1.6). Hence,
Using inequality (5.1 )
andperforming
similar calculations as we did in theproof
ofProposition 3.4,
we obtainThe Schauder estimate
(2.1 ) implies
that w EC~~ê.
DOur next aim is to prove an
analogous
result to Lemma 3.1(iii)
foroperator P,
thatis, equation
Pu =,f
E~’,.~,.t_2
has a solution u EC;t’
iff
satisfies
where
h(t)
is anon-increasing
functionsatifying
According
to Lemma3.7,
there are two constantsK3
andK4
so that if(5.3)
isfulfilled,
andsupp( f ) car,
then there exists u E such thatwhere
As we did in the
previous proof,
we writeP - ta, + Q 1 + Q 2,
whereC
Br+1
I andsupp(Q)
CQr.
In view of(1.7), (5.2)
and(5.4)
we havethat
if r is
sufficiently large.
LEMMA 5.2. Let m be a
non-negative integer
and assume Psatisfies
condition
(1.5)-(1.9). Suppose f
EC,,,-21 f satisfies (5.3),
andsupp( f )
cOr
with rsufficiently large
so that(5.5) holds,
thenequation
has a solution v E
C;"u.
PROOF. We may assume without loss of
generality
that 1. Wesolve
equation (5.6) by
iteration. Define the sequence as follows:We claim that
We show
(5.7) by
induction.By
Lemma3.7,
By (1.9),
Combining
the laterinequality
with(5.2)
and with the fact thatsupp( Q)
we obtain
by
Lemma3.7,
Thus
(5.7)
isproved.
Setting
gives
that v satisfiesequation (5.6)
and from(5.7)
it follows thatLEMMA 5.3. Retain all the
hypotheses of
Lemma5.3,
thenequation
has a solution u E
PROOF. Let v be a solution of
equation (5.6),
and set u = v - w. Then P u =
f.
The rest of theproof
is conductedprecisely
as it was done in the
proof
of Theorem 5.1. 0 THEOREM 5.4. Let m be anon-negative integer. Suppose
Psatisfies (1.5)-(1.9), f
ECom’-2, and f satisfies (5.3).
Then there exists u EC2m,,,
such thatPROOF. We write P = and we choose r so that
(5.5)
is fulfilled.Let v E 0
v(x)
1,3(z)
= 1 forIxl
r and3(z)
= 0 forIxl >
r + 1.Let u 1 be the solution of
equation p u
=(1 - ~)/,
which existsaccording
to Lemma 5.3. Let ° ..
where is the Green’s function of P. Then
PU2
andby inequalities (2.1 )
and(5.1), ~2!!m,2,~ Clearly,
is a solution ofequation
(5.8),
and theproof
iscomplete.
D6. - Proofs of the main results
PROOF OF THEOREM 1.1. Let =
min{qo(x), 0}, q£(z)
=max{qo(x), 0}
and
Consider a
family
ofoperators,
Then Pt
isuniformly
continuousin t, Pt
= Aand Pt
is subcritical in Rnby
thefirst Remark in Section 1.
Furthermore,
conditions(1.5)-(1.9)
are fulfilled forPt,
where A is
replaced by At
:=min{ 1, a}
and A isreplaced by At
:=max{l,A},
and all other
parameters
remainsunchanged. Therefore,
in view of Theorems 4.1 and5.1, Pt
is asurjective
Fredholmoperator
for each 0 t 1. Since the Fredholm’s index is a continuous function of t,Let
now Pt = A
+ t~(.). Then Po
=Pl , P,
= Pand Pt
is subcritical for 0 t 1since P is subcritical.
Using
the samearguments
as above we obtainPROOF OF THEOREM 1.2. Set
km
=dm -
i for m > 1 andko
=do.
We conduct theproof by showing
that for any m > 0 there are u 1, ... , ukmlinearly independent
functions whichbelong
toker(P, ker(P, Cm’° 1).
Consider the
operator
where
Nm
is the space ofhomogeneous
harmonicpolynomials
ofdegree
m. Set1 := dim
ker( Q , Nm)
and let pl , ... , pl be a basis forker( Q , Mm).
Then pjbelongs
to
for j
=1, ... , l.
Let pl+ 15 ..., pk,. be a basis forJIm Bker(Q, JIm),
then
using assumption (1.10)
wehave,
is finitefor j
=~+1,..., Therefore, by
Theorem5.1, equation
has a
solution V.
ESetting
pjfor j - l
+ we have that Ujbelongs
tosince Vj E C2m,,,
andhence vj
is nota
polynomial
ofdegree
m.Clearly,
ul+1, ... , u, arelinearly independent. Thus,
form a basis for
ker(P, C;,(’).
7. -
Weighted
Sobolev spacesOur
goal
in this section is to show ananalogous
result to Theorem 1.1 inweighted
Sobolev spaces. These spaces are definedby
thecompletion
ofwith
respect
to the normwhere 11 - lip
is the standard LP-norm. We denote themby W: 15.
When k = 0they
are theweighted LP-spaces
which are denotedby LP
’
The
Laplacian
is considered as theoperator
A
complete description
ofoperator (7.1 )
wasgiven by
McOwen[11]
andLockhart
[9]. They proved
thatoperator (7.1)
is Fredholm if andonly
ifwhere
1 / p + 1 / p’
= 1 and 1 p oo.Furthermore,
if 6> - n / p,
then(7.1 )
is
injective
and its Fredholm’s index isequal
to is thelargest integer 1).
Let
be a
perturbation
of theLaplacian.
THEOREM
(Lockhart [9]
and McOwen[12]). Suppose P
isuniformly elliptic
operator in Rn and 6
satisfies (7.2). If
then
is Fredholm with the same index as the
Laplace
operator(7.1 ).
Lockhart and McOwen
assumed qa E
for= 2, however,
thatcondition may be removed
by
means of aperturbation. Imposing
additionalrestrictions on
P,
we obtain astronger
result for 6 >-n/p.
THEOREM 7.1. Let P be
uniformly elliptic
and subcritical operator in Assume qa are a -Hölder continuous and00
where
h(t) is a non-increasing function satisfying J
1K2.
If 6
>-n/p,
thenis an
injective
operator.COROLLARY 1. Retain the
hypotheses of
Theorem 7.1 and assume 8satisfies (7.2).
Then there is apositive
constant C such thatREMARK. In
[4]
Avellaneda and Lin showed that ifA4J
E thenfor ,~
being
a second-orderelliptic operator
in thedivergence
form withperiodics
coefficients.
COROLLARY 2. Let P* be the
formal adjoint
operatorof
P. Assume Psatisfies
thehypotheses of
Theorem 7.1, and 6 >-n/p satisfying (7.2).
Thenis a
surjective
Fredholm operator and its index isequal
toAs a consequence of
Corollary 2,
we have that if E thenequation
P*u =f
has a solution u such that(x)-~-ZU
EMoreover,
anytwo solutions U2 E
LP~,-21
differby
a linear combination offinitely
many functions fromker(P*, Lp~ 6-2 ).
PROOF OF THEOREM 7.1. It suffices to show that
CO’(Rn)
annihilates Sofix p
E and letG p * (x, y)
be the Green’s function ofP *. Define ..
then
Since the Green’s function of p * is
given by G p* (x, y)
=(see
e.g.[14;
Theorem
20.6]),
we haveby
Pinchover’s estimate(5.1 ),
where the constant
C~ depents
on p.Therefore,
it follows from the laterinequality
that if 6 >-n/p,
thenSuppose
now u Eker(P,
then there is a sequence1 C
so that u in
WiD
andPuk
--+ 0 in as k --> oo.Therefore, by (7.3)
and
(7.4),
’
The
proof
iscompleted.
D8. - Failure of the Liouville
type
theorems for fourth-orderelliptic operators
It is known that the classical Liouville’s theorem holds true for the
BiLaplace operator A’ (cf. [6;
Theorem2.28]). Nevertheless,
it ispossible
to construct a
perturbation
ofBiLaplace
such that all qa are
compactly supported (and
hence conditions(1.7)
and(1.9)
are
fulfilled),
while dimker(P)
islarge
as we wish in any of the spacesC2.,,, +16
and
W2p,,
*Our construction is similar to the one
given
in[18]
of anelliptic
operator which has an infinite dimension null space, and is based upon thefollowing example
due to Plis. In[21]
he showed the existence of anoperator
such that:
(i)
GLa EC1°(Bi (0))
(ii)
there is uo ECo (B1 (0)) satisfying Pouo
= 0.For any
integer
N let 1 be adisjoint
sequence ofballs, {x :
Set
and
are
linearly independent
sincesupp(uj)
CBj
andBj
aredisjoint.
Inaddition,
= 0. Thus dimker(P )
> N.Acknowledgments
I am very
grateful
to Yehuda Pinchover for hisstimulations
and manyvaluable
suggestions.
REFERENCES
[1] R.A. ADAMS, Sobolev Spaces, Academic Press, New York, 1975.
[2] S. AGMON, On Positivity and decay of solutions of second order elliptic equations
on Riemannian manifolds, Methods of Functional
Analysis
and Theory ofElliptic
Equations (D. Greco ed.), Liguari Editore, Napoli, 1982, 19-52.[3] M. AVELLANEDA - F.H. LIN, Une théorème de Liouville pour des équations elliptiques
à coefficients périodiques, C. R. Acad. Sci. Paris Sér. I Math. 309 (1989), 245-250.
[4] M. AVELLANEDA - F.H. LIN, LP bounds on singular integrals in homogenization,
Comm. Pure Appl. Math. 44 (1991), 897-910.
[5] H. BEGEHR - G.N. HILE, Schauder estimates and existence theory of entire solutions
of linear elliptic operator, Proc. Roy. Soc.
Edinburgh
Sect. A 110 (1988), 101-123.[6] Yu. V. EGOROV - M.A. SHUBIN, Linear Partial Differential Equations. Foundations
of Classical Theory, Partial Differential Equations I (Yu. V. Egorov and M.A. Shubin, eds),
Encyclopedia
of Math. Sci., 30,Springer-Verlaga, Berlin-Heildelberg-New
York,1991.
[7] A. FRIEDMAN, Bounded entire solutions of elliptic equations, Pacific J. Math. 44
(1973), 497-507.
[8] L. KARP, Generalized Newton potential and its applications, J. Math. Anal.
Appl.
174 (1993), 480-497.
[9] R.B. LOCKHART, Fredholm properties of a class of elliptic operators on non-compact manifolds, Duke Math. J. 48 (1981), 289-312.
[10] R.B. LOCKHART - R.C. MCOWEN, On elliptic system in Rn, Acta Math. 150 (1983),
125-135.
[11] R.C. MCOWEN, The behavior of the Laplacian on weighted Sobolev spaces, Comm.
Pure
Appl.
Math. 32 (1979), 785-795.[12] R.C. MCOWEN, On elliptic operators in Rn, Comm. Partial Differential
Equations
5 (1980), 913-933.[13] N. MEYERS, An expansion about infinity for solutions of linear elliptic equations, J.
Math. Mech. 12 (1963), 247-264.
[14] C. MIRANDA, Partial Differential Equations of
Elliptic
Type, second edition, Sprin- ger-Verlag,Berlin-Heildelberg-New
York, 1970.[15] J. MOSER - M. STRUWE, On a Liouville type theorem for linear and nonlinear
equations on a tours, Bol. Soc. Brasil. Mat. 23 (1992), 1-20.
[16] M. MURATA, Isomorphism theorems for elliptic operators in Rn, Comm. Partial Differential Equations 9 (1984), 1085-1105.
[17] M. MURATA, On construction of Martin boundaries for second order elliptic equations,
Publ. Res. Inst. Math. Sci. 26 (1990), 585-627.
[18] L. NIRENBERG - H.F. WALKER, The null spaces of elliptic partial differential operators in Rn, J. Math. Anal. Appl. 42 (1973), 271-301.
[19] Y. PINCHOVER, On positive solutions of second second order elliptic equations, stability results and classification, Duke Math. J. 57 (1988), 955-980.
[20] Y PINCHOVER, On the equivalence Green functions of second order elliptic equations
in Rn, Differential Integral
Equation
5 (1992), 481-493.[21] A. PLI015B, A smooth linear elliptic differential equations without any solution in a
sphere, Comm. Pure Appl. Math. 14 (1961), 599-617.
[22] M. SCHECTER, Principles of Functional Analysis, Academic Press, New York, 1971.
[23] E. STEIN - G. WEISS, Fourier Analysis on Euclidean Spaces, Princeton University Press, Princeton, New Jersey, 1971.
Department of Theoretical Mathematics Weizmann Institute of Science
Rehovot 76100 ISRAEL and
Department of Mathematics