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STRONG UNIQUE CONTINUATION OF EIGENFUNCTIONS FOR p-LAPLACIAN OPERATOR
ISLAM EDDINE HADI and N. TSOULI (Received 28 January 2000)
Abstract.We show the strong unique continuation property of the eigenfunctions for p-Laplacian operator in the casep < N.
2000 Mathematics Subject Classification. Primary 35J15.
1. Introduction. This paper is primarily concerned with the problem:
−div
|∇u|p−2∇u
+V|u|p−2u=0 inΩ, (1.1)
whereΩis a bounded domain inRNand the weight functionsVis assumed tobe not equivalent tozeroand tolie inLN/p(Ω).
Also, we know that the unique continuation property is defined by a different form.
In this work, we are interested to study a family of functions which enjoys the strong unique continuation property (SUCP), that is, functions besides possibly the zero func- tions has a zero of infinite order.
Definition1.1. A functionu∈Lp(Ω)has a zero of infinite order inp-mean at x0∈Ω, if for eachn∈N,
|x−x0|≤R|u|p=0 Rn
asR →0. (1.2)
There is an extensive literature on unique continuation. We refer to the work of Jerison-Kenig on the unique continuation for Shrödinger operators (cf. [3]). The same work is done by Gossez and Figueiredo, but for linear elliptic operator in the caseV∈ LN/2, whereN >2, (cf. [1]). Also, Loulit extended this property toN=2 by introducing Orlicz’s space, (cf. [2, 5]). In this work, we generalize this property for thep-Laplacian in the caseV∈LN/p(Ω)andp < N.
2. Strong unique continuation theorem. In this section, we proceed to establish the strong unique continuation property of the eigenfunctions for thep-Laplacian operator in the caseV∈LN/p(Ω)andp < N.
Theorem 2.1. Letu∈Wloc1,p(Ω) solution of (1.1). If u=0 on a setE of positive measure, thenuhas a zero of infinite order inp-mean.
214 I. E. HADI AND N. TSOULI To prove this theorem we need the following lemmas.
Lemma2.2. Letg∈W01,p(Ω)andV∈LN/p. Then for each >0there exists a positive constantksuch that
ΩV|g|p≤
Ω|∇g|p+k
Ω|g|p. (2.1)
Proof. Set
G= x∈ Ω
V(x)≥c
. (2.2)
So
ΩV|g|p≤
GV|g|p+k
Ω|g|p. (2.3)
By using the Hölder and Poincaré’s inequalities, we get
ΩV|g|p≤cχGVN/pL
Ω|∇g|p+k
Ω|g|p. (2.4)
But·is absolutely continuous. So, given >0, there existsksuch thatcχGV ≤. Which gives immediately the inequality (2.1).
Lemma2.3. LetBr andB2r be two concentric balls contained inΩ. Then
Br|∇u|p≤ c rp
B2r|u|p, (2.5)
where the constantcdoes not depend onr.
Proof. Takeϕ∈C0∞(Ω), with suppϕ⊂B2r,ϕ(x)=1 fo rx∈Br and|∇ϕ| ≤c/r. Usingϕpuas a test function in (1.1), we get
B2r−div
|∇u|p−2∇u ϕpu+
B2rV|u|p−2uϕpu=0. (2.6)
So
B2r
|∇u|pϕp= −p
B2r
|∇u|p−2ϕp−2∇u·∇ϕ(ϕu)−
B2r
V|ϕu|p. (2.7) Using Young’s inequalities for(((p−1)/p)+1/p=1), we can estimate the first inte- gral in the right-hand side of (2.7) by
(p−1)p/(p−1)
B2r|∇u|pϕp+−p
B2r|∇ϕ|p|u|p. (2.8) Also by the result of Lemma 2.2, we can estimate the second integral in the right-hand side of (2.7) by
B2r
∇(ϕu)p+c
B2r|ϕu|p. (2.9)
Using these estimates in (2.7), we have
B2r|∇u|pϕp≤
(p−1)p/(p−1)+
B2r|∇u|p|ϕ|p +
−p+
B2r
|u|p|∇ϕ|p+c
B2r
|u|p|ϕ|p. (2.10) Using the fact that|∇ϕ| ≤c/r, |ϕ| ≤c/r, andϕ=1 inBr, we have immediately inequality (2.5).
Lemma2.4. Letu∈W1,1(Br), whereBr is the ball of radius r inRN and letE= {x∈Br:u(x)=0}. Then there exists a constantβdependingonly onNsuch that
A|u| ≤βrN
|E||A|1/N
Br|∇u| (2.11)
for all ballBr,uas above and all measurable setsA⊂Br. Toprove this lemma see [4].
Proof of Theorem2.1. We know that almost every point ofEis a point of den- sity ofE. Letx0∈Ebe such a point. This means that
limr→0
E∩Br
Br =1, (2.12)
whereBr denotes the ball of radiusr centered atx0and|S|denotes the Lebesgue measure of a setS. So, given >0 there is anr0=r0()such that
Ec∩Br
Br < , E∩Br
Br >1− forr≤r0, (2.13) whereEcdenotes the complement of the setE. Takingr0smaller, if necessary, we can assumeBr0⊂Ω. Sinceu=0 o nE, by Lemma 2.4 and (2.13) we have
Br|u|p=
Br∩Ec|u|p≤β rN
E∩Br|Ec∩Br|1/N
Br
∇(u)p
≤pβ rN
Br(1−1/N)1/N 1−
Br|u|p−1|∇u|.
(2.14)
By Hölder’s inequality
Br|u|p≤c1/N 1−r
Br|∇u|p 1/p
Br|u|p (p−1)/p, (2.15) and by using the Young’s inequality, we get
Br|u|p≤c1/N 1−r
rp−1
Br|∇u|p+p−1 r
Br|u|p . (2.16) Finally, by Lemma 2.3, we have
Br|u|p≤c1/N 1−
B2r|u|p, (2.17)
wherecis independent ofand ofrasr→0.
216 I. E. HADI AND N. TSOULI Now let us introduce the following functions:
f (r )=
Br|u|p. (2.18)
And let us fix n∈N, choose >0 such that c1/N
/(1−)≤2−n. Observe that consequentlyr0depends onn. Then (2.17) can be written as
f (r )≤2−nf (2r ) forr≤r0. (2.19) Iterating (2.19), we get
f (ρ )≤2−knf 2kρ
, if 2k−1ρ≤r0. (2.20) Now given 0< r < r0(n)and choosek∈Nsuch that
2−kr0≤r≤2−k+1r0. (2.21) From (2.20), we obtain
f (r )≤2−knf 2kr
≤2−knf 2r0
. (2.22)
Since 2−k≤r /r0, we finally obtain f (r )≤
r r0
nf 2r0
, (2.23)
which shows thatx0is a zeroinfinite order inp-mean.
References
[1] D. G. de Figueiredoand J.-P. Gossez, Strict monotonicity of eigenvalues and unique continuation, Comm. Partial Differential Equations 17 (1992), no. 1-2, 339–346.
MR 93b:35098. Zbl 777.35042.
[2] J.-P. Gossez and A. Loulit,A note on two notions of unique continuation, Bull. Soc. Math.
Belg. Sér. B45(1993), no. 3, 257–268. MR 96k:35034. Zbl 828.35035.
[3] D. Jerison and C. E. Kenig,Unique continuation and absence of positive eigenvalues for Schrödinger operators.With an appendix by E. M. Stein, Ann. of Math. (2)121(1985), no. 3, 463–494. MR 87a:35058. Zbl 593.35119.
[4] O. A. Ladyzhenskaya and N. N. Ural’tseva,Linear and Quasilinear Elliptic Equations, Trans- lated from the Russian by Scripta Technica, Inc. Leon Ehrenpreis (trans. ed.), Aca- demic Press, New York, London, 1968. MR 39#5941. Zbl 164.13002.
[5] A. Loulit,Inégalités avec Poids et Problèmes de Continuation Unique, Thèse de Doctorat, Université Libre de Bruxelles, 1995 (French).
Islam Eddine Hadi: Département de Mathématiques et Informatique Faculté des Sci- ences, Université MohamedI, Oujda, Morocco
E-mail address:hadi@sciences.univ-oujda.ac.ma
N. Tsouli: Département de Mathématiques et Informatique Faculté des Sciences, Université MohamedI, Oujda, Morocco
E-mail address:tsouli@sciences.univ-oujda.ac.ma
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