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We consider the following problem: u∈H2,2∩H01,2(Ω), n i,j=1 ai j(x)Di ju(x)=f(x), a.e.x∈Ω

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ANTONIO TARSIA

Received 12 December 2005; Revised 20 February 2006; Accepted 21 February 2006

The equivalence between some conditions concerning elliptic matrices is shown, namely, the Cordes condition, a generalized form of Campanato’s condition, and a generalized form of a condition of Buic˘a.

Copyright © 2006 Antonio Tarsia. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction

LetΩbe an open bounded set inRn,n >2, with a sufficiently regular boundary, and let A(x)= {ai j(x)}i,j=1,...,nbe a real matrix, with coefficients ai jL(Ω). We consider the following problem:

uH2,2H01,2(Ω), n

i,j=1

ai j(x)Di ju(x)=f(x), a.e.xΩ. (1.1) If f L2(Ω), it is known (see the counterexamples in [6]) that problem (1.1) is not well posed with the only hypothesis of uniform ellipticity on the matrixA(x): there exists a positive constant ¯νsuch that

n i,j=1

ai j(x)ηiηj¯νη2n, a.e. inΩ,η=

η1,...,ηnRn. (1.2) It is therefore essential, in order to be able to solve Problem (1.1), to assume some hy- potheses onA(x) stronger than (1.2). In this paper we consider some of these ones and compare them. More precisely, we will consider the following conditions and show that they are equivalent.

Hindawi Publishing Corporation Journal of Inequalities and Applications Volume 2006, Article ID 74171, Pages1–8 DOI10.1155/JIA/2006/74171

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Condition 1.1 (the Cordes condition, see [5,8]). A(x)Rn2=0, a.e. inΩ, and there exists ε(0, 1) such that

n

i,j=1aii(x)2 n

i,j=1a2i j(x) n1 +ε, a.e. inΩ. (1.3) Condition 1.2 (ConditionAxp). There exist four real constantsσ,γ,δ,pwithσ >0,γ >0, δ0,γ+δ <1,p1, and a functiona(x)L(Ω), witha(x)σa.e. inΩ, such that

n i=1

ξiia(x) n i,j=1

ai j(x)ξi j

p

γξnp2+δ

n i=1

ξii

p

(1.4)

for allξ= {ξi j}i,j=1,...,nRn2, a.e. inΩ.

Whenp=1, the above condition will be simply denoted by ConditionAx; it was defined in [10], where it has also been shown to be equivalent to the Cordes condition. Ifa(x) is constant onΩ, ConditonAx is the formulation for linear operators of Campanato’s condition A, (see [4]), which was defined for nonlinear operators. A particular version of ConditionAxp, that is, withp=2 and (x) constant, is stated in [7] for nonlinear operators.

Condition 1.3 (ConditionBx). There exist four real positive real constantsσ,c1,c2,c3and a functionβL(Ω) such that

(i) 0< c1c2c3<1, (ii)β(x)σa.e. inΩ, and moreover

β(x) n i,j=1

ai j(x)ξi j

n i=1

ξiic1

n

i=1

ξii

2

c2

n i=1

ξii

ξn2c3ξ2n2 (1.5)

for allξ= {ξi j}i,j=1,···,nRn2, a.e. inΩ.

Ifβ(x) is constant on Ω, we will denote this condition as Condition B; it has been defined by Buic˘a in [2].

The importance of ConditionsAxp orBx is in the fact that they allow to show in a relatively simple manner, by means of near operators theory (see [4,9]) or weakly near operators theory (see [1–3]), that problem (1.1) is well posed. The usefulness of showing the equivalence among these conditions is due to the fact that to verify whether a matrix satisfies ConditionAxp orBxis very complicated, even ifn=2, while to verify whether it satisfies the Cordes condition is much simpler.

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2. A procedure of decomposition for matrices

In this section we consider a short procedure of decomposition of the matricesAandI which has been developed in [10]. We set

Ω0= xΩ: there existsb(x)Rsuch thatb(x)A(x)=I;

Ω1=Ω\Ω0. (2.1)

Remark 2.1. SetM=supΩA(x), ¯ν=infΩA(x), accordinglyn¯ν(A(x)|I)nM.

Then, for eachxΩ0, we obtain 1/Mb(x)1/¯ν.

We can assume measΩ1>0, since otherwise as we will see in the following it is easy to show the equivalence between the above conditions. We set for allxΩ1:W(x)= {B(x) : B(x)=sI+rA(x),s,rR}x=W(x)S(I, 1) (whereS(I, 1)= {B:BIRn2<1}).

Letv1,w2W(x) be the projections ofI on the lines through the zero vector ofRn2 and tangent toΣx. Moreover letv2be the projection ofI on the line through the zero vector ofRn2and perpendicular tov1, and letw1be the projection ofIon the line through the zero vector ofRn2 and perpendicular tow2. In this manner we find two systems of orthogonal vectors{v1,v2},{w1,w2}, withvi=vi(x) ,wi=wi(x),i=1, 2. Each of them is a basis in the planeW(x).ThenI=v1+v2=w1+w2, and there areLfunctionsai= ai(x) andbi=bi(x),i=1, 2, such that

A(x)=a1(x)v1(x) +a2(x)v2(x)=b1(x)w1(x) +b2(x)w2(x). ( Asv1=w2= n1 andv2 = w1 =1, then fori=1, 2,a2i a21(n1) +a22=(a1v1+a2v2|a1v1+a2v2)= (A(x)|A(x))= A(x)2; here ifB= {bi j}i,j=1,···,nandC= {ci j}i,j=1,···,n, we set (B|C)= n

i,j=1bi jci j.) Set

Qv(x,ν,τ)= ξRn2:ξ=sv1+tv2, 0s,tτ, Qw(x,ν,τ)= ξRn2:ξ=sw1+tw2, 0s,tτ, Rx,ν00

= ξRn2:ξ=sw2+tv1, 00s,tτ0

, CΣx

= v:vW(x) such thatzΣx,t >0 for whichv=tz, Cρ(x)= v:vCΣx

:t >0 such thatItv< ρ, 0< ρ <1.

(2.2)

The following propositions are proved in [10].

Proposition 2.2. For allτ,ν>0 withντ,τ00, 0< τ00, such that for allxΩ1, Qv(x,ν,τ)Qw(x,ν,τ)Rx,ν00

. (2.3)

Proposition 2.3. For allτ0,ν0, 0< τ00, there existsρ(0, 1) such that for allxΩ1, Rx,ν00

Cρ(x). (2.4)

3. ConditionBx

Proposition 3.1. ConditionAxand ConditionBxare equivalent.

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Proof. We assume thatA satisfies Condition Ax. It follows (from (1.4) with p=1) by squaring both members

I|ξ22a(x)A|ξI|ξγ2ξ2+ 2γδ|

I|ξ|ξ+δ2I|ξ2 (3.1) then

2a(x)A|ξI|ξ(1δ2)I|ξ22γδ|

I|ξ|ξγ2ξ2. (3.2) This is ConditionBxwithb(x)=2a(x),c1=1δ2,c2=2γδ,c3=γ2. Conversely, we set A(x)=β(x)A(x) and assume that Condition B holds for A, then we will show that A also satisfies ConditionAx. To this purpose we write Condition B in the following form: there exist four real positive constantsM,c1,c2,c3with 0< c1c2c3<

1, supxΩA(x)Msuch that A(x)|ξI|ξc1

I|ξ2c2I|ξξc3ξ2, (3.3) for allξRn2, a.e. inΩ. Then we obtain the thesis by using the decomposition of A and Istated inSection 2. For this we distinguish two cases:xΩ0andxΩ1.

IfxΩ0, that is, there existsb(x) such thatb(x)A(x)=I, then ConditionAxis trivially true (take in (1.4)a(x)=b(x)).

Instead, ifxΩ1, with measΩ1>0, we observe that (3.3) holds in particulcular for ξW(x). So we can writeξas a linear combination of the basis{v1(x),v2(x)}. Now, let t1,t2Rbe such thatξ=t1v1(x) +t2v2(x), accordinglyξ2=|ξ)=t12(n1) +t22, then

A|ξ=

a1(x)v1+a2(x)v2|t1v1+t2v2

=a1t1(n1) +a2t2, I|ξ=

v1+v2|t1v1+t2v2

=t1(n1) +t2. (3.4) Now, (3.4) and the above remarks yield the following form of Condition B: for eachξ W(x),

A|ξI|ξ=

a1t1(n1) +a2t2][t1(n1) +t2

c1

t1(n1) +t2

2

c2

t1(n1) +t2

t12(n1) +t22c3

t12(n1) +t22

. (3.5) Put

Ft1,t2

=

a1t1(n1) +a2t2

t1(n1) +t2

c1

t1(n1) +t22

+c2

t1(n1) +t2

t12(n1) +t22+c3

t21(n1) +t22

. (3.6)

Remark that

Ft1,t2

0, t1,t2

R2(by (3.5)). (3.7)

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In particular F

1

n1, 0

=a1(n1)c1(n1) +c2

n1 +c30 (3.8)

from which

a1(x)c1c2

n1 c3

n1 c1c2c3>0. (3.9) While the inequalityF(0, 1)=a2(x)c1+c2+c30 impliesa2(x)c1c2c3>0.

In the same way, by taking the system of orthogonal vectors{w1,w2}as basis ofW(x), it follows that

bi(x)c1c2c3>0, i=1, 2,xΩ1. (3.10) So we have shown (seeSection 2) that A(x)Qv(x,ν,τ)Qw(x,ν,τ). This implies, by Proposition 2.2, A(x)R(x,ν00), then by Proposition 2.3, A(x)Cρ(x), which is equivalent to say that ConditionAxis valid withδ=0.

Taking into account this proposition and the equivalence between the Cordes condition and ConditionAx, shown in [10], we have the following.

Corollary 3.2. ConditionBxand the Cordes condition are equivalent.

The following example states that Condition B is stronger than ConditionAxand there- fore is also stronger than the Cordes condition.

Example 3.3. LetΩ=Ω1Ω2, whereΩ1= {(x1,x2)R2: 0< x1<1, 0< x21}and Ω2= {(x1,x2)R2: 0< x1<1, 1< x2<2}, moreover

A(x)=

A1, ifxΩ1,

A2, ifxΩ2, A1= 1 0

0 1

, A2=

200 150

150 200

. (3.11) Ais uniformly elliptic onΩand, sincen=2, this implies the Cordes condition and there- fore also ConditionAx(see [10]). NeverthelessAdoes not satisfy Condition B. Indeed, we considerxΩ1, thenA(x)=A1. We observe that ifA1satisfied Condition B, it would be

A1|ξI|ξc1

I|ξ2c2I|ξξc3ξ2 (3.12) for eachξR4, that is,

1c1

I|ξ2+c2I|ξξ+c3ξ20. (3.13) The bilinear formΦ(X,Y)=(1c1)X2+c2XY+c3Y2, where (X,Y)R2, is nonneg- ative if (1c1)c3c22/4. In particular it must holdc1<1. Otherwise ifA(x) satisfied Condition BonΩ2it would be

A2|ξI|ξc1

I|ξ2c2I|ξξc3ξ2, (3.14)

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wherec1,c2,c3are the above determined constants for the matrixA1. Now we consider the matrix

ξ=

1 0

2 0

, (3.15)

by replacing it in (3.14), we obtain100c1c2

55c3, that is,c2(51) + 4c3 c1c2c3+ 100; that implies (because by hypothesis it holdsc1> c2+c3) 4c1>4(c2+ c3)100, thenc125. This contradicts what we have obtained forA1, that is,c1<1.

4. ConditionAxp

We prove equivalence between the Cordes condition and ConditionAxpin the same way used in [10] for the proof of equivalence between Condition A and the Cordes condition.

The first step is following.

Lemma 4.1. ConditionAxpwithδ=0 is equivalent to Cordes Condition.

Proof (see also [10]). We can write ConditionAxp, ifδ=0, as follows:

Ia(x)A(x)|ξγ1/ pξ (4.1) for allξRn2, andp1. This is just ConditionAxwithδ=0 and, accordingly to what proved in [10], this is equivalent to the Cordes condition.

The second step for the achievement of our goal is following.

Lemma 4.2. IfA(x) satisfies ConditionAxpfor some functiona(x) and some constantsσ,γ, δ, then it satisfies the same condition withδ=0 and possibly differentσ,γ,a(x).

Proof. We proceed on the line of the proof of [10, Lemma 3.3]. We follow the notations ofSection 2. ConditionAxp, withδ=0, yields ConditionAxpwithδ=0, by replacing the coefficienta(x) of the first condition with a new coefficient ¯a(x), defined by

a(x)¯ =

b(x), ifxΩ0,

c(x), ifxΩ1. (4.2)

IfxΩ0, then ConditionAxpwithδ=0 is trivially satisfied. Moreover, byRemark 2.1, 1/Mb(x)1/ν. Now let¯ xΩ1. We prove the existence of a functionc(x) by means of the decomposition of matricesA(x),I stated inSection 2and replacing the expressions obtained in ConditionAxp:

Ia(x)A(x)|ξp=v1+v2a(x)a1v1+a2v2

|ξp

=

takeξ=vi,i=1, 2

=v1+v2a(x)a1v1+a2v2

|vip=vi2a(x)aivi2p

=1a(x)aipvi2pγvipv1+v2|vi

p

=γvip+δvi2p. (4.3)

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From this 1 a(x)

1 p

γ+δvip vi

ai 1 a(x)

1 + p

γ+δvip vi

. (4.4)

We observe that

1(γ+δ)1/ p1 p

γ+δvip

vi , 1 + p

γ+δvip

vi 1 + (γ+δ)1/ p. (4.5) Usingv1 =

n1,v2=1, we can write γ+δvip

vip γ+δ, i=1, 2. (4.6)

We conclude, from (4.4), by setting M1=sup

Ω a(x), ν= 1 M1

1(γ+δ)1p

, τ=1

σ

1 + (γ+δ)1/ p

(4.7) for allxΩ1,A(x)Qv(x,ν,τ). Then by takingξ=wi(i=1, 2) in ConditionAxp, with similar calculations, we obtain for all xΩ1,A(x)Qw(x,ν,τ). Then for all xΩ1, A(x)Qv(x,ν,τ)Qw(x,ν,τ). FromProposition 2.2it follows that there existν00, with 00< τ0, such thatA(x)R(x,ν00). ByProposition 2.3there existsρ(0, 1) such thatA(x)Cρ(x), that is, there existc(x)>0 andρ(0, 1) such that

Ic(x)A(x)ρ. (4.8)

(This inequality also implies (n1)/M < c(x)<(n+ 1)/ν,¯ xΩ1.) From Lemmas4.1and4.2we have the following.

Theorem 4.3. The Cordes condition and ConditionAxpare equivalent.

This theorem andCorollary 3.2imply the following.

Corollary 4.4. ConditionBxand ConditionAxpare equivalent.

Theorem 4.3andCorollary 3.2, by the results proved in [10], imply the following.

Corollary 4.5. Letn=2. Then every uniformly elliptic symmetric matrix satisfies Condi- tionAxpand ConditionBx.

References

[1] A. Buic˘a, Some properties preserved by weak nearness, Seminar on Fixed Point Theory Cluj Napoca 2 (2001), 65–70.

[2] , Existence of strong solutions of fully nonlinear elliptic equations, Proceedings of Confer- ence on Analysis and Optimization of Differential Systems, Constanta, September 2002.

[3] A. Buic˘a and A. Domokos, Nearness, accretivity, and the solvability of nonlinear equations, Nu- merical Functional Analysis and Optimization 23 (2002), no. 5-6, 477–493.

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[4] S. Campanato, A Cordes type condition for nonlinear nonvariational systems, Rendiconti Ac- cademia Nazionale delle Scienze detta dei XL. Serie V. Memorie di Matematica. Parte I 13 (1989), no. 1, 307–321.

[5] H. O. Cordes, Zero order a priori estimates for solutions of elliptic differential equations, Proceed- ings of Symposium in Pure Math., vol. 4, American Mathematical Society, Rhode Island, 1961, pp. 157–166.

[6] O. A. Ladyzhenskaya and N. N. Ural’tseva, Linear and Quasilinear Elliptic Equations, Academic Press, New York, 1968.

[7] A. Maugeri, D. K. Palagachev, and L. G. Softova, Elliptic and Parabolic Equations with Discontin- uous Coefficients, Wiley-VCH, Berlin, 2000.

[8] G. Talenti, Sopra una classe di equazioni ellittiche a coefficienti misurabili, Annali di Matematica Pura ed Applicata. Serie Quarta 69 (1965), 285–304.

[9] A. Tarsia, Some topological properties preserved by nearness between operators and applications to P.D.E, Czechoslovak Mathematical Journal 46 (1996), no. 4, 607–624.

[10] , On Cordes and Campanato conditions, Archives of Inequalities and Applications 2 (2004), no. 1, 25–39.

Antonio Tarsia: Dipartimento di Matematica “L. Tonelli,” Universit`a di Pisa, Largo Bruno Pontecorvo 5, 56127 Pisa, Italy

E-mail address:[email protected]

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