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A compactness result for solutions to an equation with C0 condition.

Samy Skander Bahoura

Equipe d’Analyse Complexe et Géométrie.

Université Pierre et Marie Curie, 75005 Paris, France.

Abstract

We give a blow-up behavior for solutions to a variational problem with continuous regular weight (not Lipschitz and not Hölderian in one point) and Dirichlet condition. An application, we have a compactness of the solutions to this Problem, with regular weight and Lipschitz condition.

Keywords: Blow-up, boundary, a priori estimate, regular weight,C0 condition.

MSC: 35J05, 35J60, 35B44, 35B45

1 Introduction and Main Results

We set∆ =11+22 on an analytic domainR2. We consider the following equation:

(P)

−∆u= 1

log|x|

2d

V eu in R2,

u= 0 in ∂Ω.

Here:

d=diam(Ω), 0∂Ω, and,

0V b <+∞, 1

log|x|

2d

euL1(Ω), uW01,1(Ω).

The previous equation was studied by many authors, with or without the boundary condition, also for Riemannian surfaces, see [1-14], we can find some existence and compactness results.

Among other results, we can see in [7] the following important Theorem, Theorem.(Brezis-Merle [7]).If(ui)iand(Vi)iare two sequences of functions relatively to the problem (P)with,0< aVi b <+∞, then, for all compact setK ofΩ,

e-mails: [email protected], [email protected]

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sup

K

uic=c(a, b, K,Ω).

If we assumeV with more regularity, we can have another type of estimates, asup + inftype inequalities. It was proved by Shafrir see [14], that, if(ui)i,(Vi)i

are two sequences of functions solutions of the previous equation without as- sumption on the boundary and, 0 < a Vi b < +∞, then we have the following interior estimate:

Ca b

sup

K

ui+ inf

uic=c(a, b, K,Ω).

Now, if we suppose(Vi)i uniformly Lipschitzian with A the Lipschitz con- stant, then,C(a/b) = 1andc=c(a, b, A, K,Ω), see [5].

Here we give the behavior of the blow-up points on the boundary and a proof of a Problem with Lipschitz condition.

Here, we write an extension of Brezis-Merle Problem (see [7]) is:

Problem. Suppose thatViV inC0( ¯Ω), with, 0Vi. Also, we consider a sequence of solutions(ui)of(P)relatively to(Vi)such that,

Z

1

log|x|

2d

euidxC,

is it possible to have:

||ui||L C?

Here, we give a caracterization of the behavior of the blow-up points on the boundary and also a proof of the compactness theorem when the prescribed curvature are uniformly Lipschitzian. For the behavior of the blow-up points on the boundary, the following condition is enough,

0Vib, The conditionVi V inC0( ¯Ω)is not necessary.

But for the proof for the Brezis- Merle type problem we assume that:

||∇Vi||L A.

We have the following caracterization of the behavior of the blow-up points on the boundary.

Theorem 1.1 Assume thatmaxui+∞, Where(ui)are solutions of the probleme (P) with:

0Vib, and Z

1

log|x|

2d

euidxC, i,

then; after passing to a subsequence, there is a finction u, there is a number N Nand there are N pointsx1, x2, . . . , xN ∂Ω, such that,

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νuiνu+

N

X

j=1

αjδxj, αj 4π, weakly in the sense of measures

and,

uiu in Cloc1 ( ¯− {x1, . . . , xN}).

In the following theorem, we have a compactness result which concern the problem(P).

Theorem 1.2 Assume that (ui)are solutions of (P) relatively to(Vi) with the following conditions:

d=diam(Ω), 0∂Ω,

0Vib, ||∇Vi||LA, and Z

1

log|x|

2d

eui C,

We have,

||ui||Lc(b, A, C,Ω),

2 Proof of the theorems

Proof of theorem 1.1:

We have,

uiW01,1(Ω),

By [7],eui Lk, ∀k1. By the elliptic estimates:

uiW2,k(Ω)C1,ǫ( ¯Ω), ǫ >0.

We denoteνuithe inner derivative ofui. By the maximum principleνui 0. By the Stokes formula:

Z

∂Ω

νuiC,

Thus, (using the weak convergence in the space of Radon measures), we have the existence of a non-negative Radon measureµsuch that,

Z

∂Ω

νuiφdσµ(φ), φC0(∂Ω).

We take anx0 ∂Ωsuch that,µ(x0)<4π. Without loss of generality, we can assume that the following curve,B(x0, ǫ)∂Ω :=Iǫ is an interval.(In this

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case, it is more simple to construct the following test functionηǫ). We choose a function ηǫ such that,

ηǫ1, on Iǫ, 0< ǫ < δ/2, ηǫ0, outside I,

0ηǫ1,

||∇ηǫ||L(I)C0(Ω, x0)

ǫ .

We take aη˜ǫsuch that,

(−∆˜ηǫ= 0 in

˜

ηǫ=ηǫ on∂Ω.

We take a cutoff functionη0 inB(0,2)or B(x0,2):

We setηǫ(x) =η0(|xx0|/ǫ)in the case of the unit disk it is sufficient.

We use a chart[f, B1(0)]withf(0) =x0.

We can take: µǫ(x) = η0(x/ǫ) and ηǫ(y) = µǫ(f−1(y)), we extend it by 0 outside f(B1(0)). We have f(B1(0)) = D1(x0), f(Bǫ(0)) = Dǫ(x0) and f(Bǫ+) =D+ǫ(x0)withf andf−1smooth diffeomorphism.

ηǫ1, on a the connected set Jǫ=f(Iǫ), 0< ǫ < δ/2, ηǫ0, outside Jǫ=f(I),

0ηǫ1,

||∇ηǫ||L(Jǫ)C0(Ω, x0)

ǫ .

And, H1(Jǫ) C1H1(I) = C14ǫ, since f is Lipschitz. Here H1 is the Hausdorff measure.

We solve the Dirichlet Problem:

(∆¯ηǫ= ∆ηǫ in R2,

¯

ηǫ= 0 in ∂Ω.

and finaly we setη˜ǫ =−¯ηǫ+ηǫ. Also, by the maximum principle and the elliptic estimates we have :

||∇˜ηǫ||L C(||ηǫ||L+||∇ηǫ||L+||∆ηǫ||L) C1

ǫ2, withC1 depends onΩ.

We use the following estimate, see [8],

||∇ui||Lq Cq, iand 1< q <2.

We deduce from the last estimate that, (ui) converge weakly in W01,q(Ω), almost everywhere to a function u 0 and R

1

log|x|

2d

eu < +∞ (by Fatou lemma). Also, Vi weakly converge to a nonnegative function V in L. The function uis inW01,q(Ω)solution of :

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−∆u= 1

log|x|

2d

V euL1(Ω) in Ω

u= 0 on∂Ω,

As in the corollary 1 of Brezis-Merle result, see [7], we haveekuL1(Ω), k >

1. By the elliptic estimates, we haveuC1( ¯Ω).

We can write,

−∆((uiu)˜ηǫ) = 1

log|x|

2d

(VieuiV euηǫ+ 2<∇(uiu)|∇˜ηǫ> . (1)

We use the interior esimate of Brezis-Merle, see [7],

Step 1: Estimate of the integral of the first term of the right hand side of (1).

We use the Green formula betweenη˜ǫ andu, we obtain, Z

1

log|x|

2d

V euη˜ǫdx= Z

∂Ω

νǫC14ǫ||∂νu||L = (2) We have,

−∆ui= 1

log|x|

2d

Vieui in Ω

ui = 0 on∂Ω,

We use the Green formula betweenui andη˜ǫ to have:

Z

1

log|x|

2d

Vieuiη˜ǫdx= Z

∂Ω

νuiηǫµ(ηǫ)µ(Jǫ)ǫ0, ǫ0>0 (3)

From (2) and (3) we have for all ǫ > 0 there is i0 = i0(ǫ) such that, for ii0,

Z

1

log|x|

2d

|(VieuiV euηǫ|dxǫ0+ (4)

Step 2: Estimate of integral of the second term of the right hand side of(1).

LetΣǫ={xΩ, d(x, ∂Ω) =ǫ3} and ǫ3 ={xΩ, d(x, ∂Ω)ǫ3},ǫ >0.

Then, forǫsmall enough,Σǫ is hypersurface.

The measure ofǫ3 isk2ǫ3µL(Ωǫ3)k1ǫ3.

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Remark: for the unit ballB(0,¯ 1), our new manifold isB(0,¯ 1ǫ3).

(Proof; let’s considerd(x, ∂Ω) =d(x, z0), z0∂Ω, this imply that(d(x, z0))2 (d(x, z))2 for allz∂Ωwhich it is equivalent to(zz0)·(2xzz0)0 for allz∂Ω, let’s consider a chart aroundz0 andγ(t)a curve in∂Ω, we have;

(γ(t)γ(t0)·(2xγ(t)γ(t0))0 if we divide by(tt0)(with the sign and tendt tot0), we haveγ(t0)·(xγ(t0)) = 0, this imply thatx=z00

whereν0is the outward normal of∂Ωatz0))

With this fact, we can say thatS ={x, d(x, ∂Ω)ǫ}={x=z0z0, z0

∂Ω, −ǫ s ǫ}. It is sufficient to work on ∂Ω. Let’s consider a charts (z, D=B(z,z), γz)withz∂Ωsuch thatzB(z, ǫz)is cover of∂Ω. One can extract a finite cover(B(zk, ǫk)), k= 1, ..., m, by the area formula the measure ofSB(zk, ǫk)is less than a(aǫ-rectangle). For the reverse inequality, it is sufficient to consider one chart around one point of the boundary).

We write, Z

|<∇(uiu)|∇˜ηǫ>|dx= Z

ǫ3

|<∇(uiu)|∇˜ηǫ>|dx+

+ Z

Ω−Ωǫ3

<∇(uiu)|∇˜ηǫ>|dx. (5)

Step 2.1:Estimate of R

Ω−Ωǫ3|<∇(uiu)|∇˜ηǫ>|dx.

First, we know from the elliptic estimates that ||∇˜ηǫ||L C12, C1 de- pends on

We know that(|∇ui|)iis bounded inLq,1< q <2, we can extract from this sequence a subsequence which converge weakly tohLq. But, we know that we have locally the uniform convergence to|∇u|(by Brezis-Merle theorem), then, h=|∇u|a.e. Letq be the conjugate ofq.

We have,∀f Lq(Ω) Z

|∇ui|f dx Z

|∇u|f dx

If we takef = 1Ω−Ωǫ3, we have:

forǫ >0i1=i1(ǫ)N, ii1, Z

Ω−Ωǫ3

|∇ui| ≤ Z

Ω−Ωǫ3

|∇u|+ǫ3.

Then, forii1(ǫ), Z

Ω−Ωǫ3

|∇ui| ≤meas(Ωǫ3)||∇u||L+ǫ3=3. Thus, we obtain,

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Z

Ω−Ωǫ3

|<∇(uiu)|∇˜ηǫ>|dxǫC1(2k1||∇u||L+ 1) (6) The constantC1 does not depend onǫbut onΩ.

Step 2.2:Estimate of R

ǫ3|<∇(uiu)|∇˜ηǫ>|dx.

We know that,ǫ⊂⊂Ω, and ( because of Brezis-Merle’s interior estimates) uiuinC1(Ωǫ3). We have,

||∇(uiu)||L(Ωǫ3)ǫ3,forii3=i3(ǫ).

We write,

Z

ǫ3

|<∇(uiu)|∇˜ηǫ>|dx≤ ||∇(uiu)||L(Ωǫ3)||∇˜ηǫ||L C1ǫforii3,

Forǫ >0, we have foriN,imax{i1, i2, i3}, Z

|<∇(uiu)|∇˜ηǫ>|dxǫC1(2k1||∇u||L+ 2) (7) From (4) and (7), we have, for ǫ > 0, there is i3 = i3(ǫ) N, i3 = max{i0, i1, i2} such that,

Z

|∆[(uiu)˜ηǫ]|dxǫ0+ǫ2C1(2k1||∇u||L+ 2 +C) (8) We chooseǫ >0small enough to have a good estimate of(1).

Indeed, we have:

(−∆[(uiu)˜ηǫ] =gi,ǫ in Ω, (uiu)˜ηǫ= 0 on ∂Ω.

with||gi,ǫ||L1(Ω)ǫ0.

We can use Theorem 1 of [7] to conclude that there isqq >˜ 1such that:

Z

Vǫ(x0)

eq|u˜ i−u|dx Z

eq|ui−u|˜ηǫdxC(ǫ,Ω).

where,Vǫ(x0)is a neighberhood ofx0 inΩ.¯

Thus, for eachx0∂Ω− {x¯1, . . . ,x¯m} there isǫx0>0, qx0>1 such that:

Z

B(x0x0)

eqx0uidxC, i.

Now, we consider a cutoff functionηC(R2)such that:

η1 on B(x0, ǫx0/2) and η0 on R2B(x0,x0/3).

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We write,

−∆(uiη) = 1

log|x|

2d

Vieuiη2<∇ui|∇η >−ui∆η.

By the elliptic estimates,(uiη)iis uniformly bounded inW2,q1(Ω)and also, in C1( ¯Ω).

Finaly, we have, for someǫ >0small enough,

||ui||C1,θ[B(x0,ǫ)]c3 i. (9) We have proved that, there is a finite number of pointsx¯1, . . . ,x¯msuch that the squence(ui)i is locally uniformly bounded in¯− {x¯1, . . . ,x¯m}.

And, finaly, we have:

νuiνu+

N

X

j=1

αjδxj, αj weakly in the sense of measures. (10) Proof of theorem 1.2:

Without loss of generality, we can assume that 0 = x1 is a blow-up point (either, we are in the regular case). Also, by a conformal transformationγ, we can assume that Ω =B1+, the half ball, and+B1+ is the exterior part, a part which not contain 0 and on which ui converge in the C1 norm to u. Let us considerB+ǫ, the half ball with radiusǫ >0.

We know that:

uiW2,k(Ω)C1,ǫ( ¯Ω).

Thus we can use integrations by parts (Gauss-Green-Riemann-Stokes for- mula). The second Pohozaev identity applied around the blow-up0 =x1gives:

Z

B+ǫ

∆ui(x· ∇ui)dx= Z

+B+ǫ

g(∇ui)dσ, (11)

with,

g(∇ui) = (ν· ∇ui)(x· ∇ui)x·ν|∇ui|2 2 . After integration by parts, we obtain:

Z

Bǫ+

1

log|x|

2d

Vieuidx+

Z

Bǫ+

< x|∇Vi > 1

log|x|

2d

Vieuidx+

Z

∂B+ǫ

1

log|x|

2d

Vieui(x·ν) =

= Z

+Bǫ+

g(∇ui)dσ, (12)

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Z

Bǫ+

1

log|x|

2d

V eudx+

Z

B+ǫ

< x|∇V > 1

log|x|

2d

V eudx+

Z

∂Bǫ+

1

log|x|

2d

V eu(x·ν) =

= Z

+B+ǫ

g(∇u)dσ, (13)

Thus,

Z

B+ǫ

1

log|x|

2d

Vieuidx Z

B+ǫ

1

log|x|

2d

V eudx+

+ Z

Bǫ+

< x|∇Vi> 1

log|x|

2d

Vieuidx Z

B+ǫ

< x|∇V > 1

log|x|

2d

V eudx+

+ Z

∂B+ǫ

1

log|x|

2d

Vieui(x·ν) Z

∂B+ǫ

1

log|x|

2d

V eu(x·ν) =

= Z

+B+ǫ

g(∇ui)g(∇u)dσ=o(1),

First, we tendito infinity afterǫto 0, we obtain:

ǫ→0lim lim

i→+∞

Z

B+ǫ

1

log|x|

2d

Vieuidx= 0, (14)

But,

Z

γ(Bǫ+)

1

log|x|

2d

Vieuidx= Z

∂γ(Bǫ+)

νui+o(ǫ) +o(1)α1>0.

A contradiction.

References

[1] T. Aubin. Some Nonlinear Problems in Riemannian Geometry. Springer- Verlag, 1998.

[2] C. Bandle. Isoperimetric Inequalities and Applications. Pitman, 1980.

[3] Bartolucci, D. A "sup+Cinf” inequality for Liouville-type equations with singular potentials. Math. Nachr. 284 (2011), no. 13, 1639ÃŘ1651.

[4] Bartolucci, D. A ‘sup+Cinf’ inequality for the equation−∆u=V eu/|x|. Proc. Roy. Soc. Edinburgh Sect. A 140 (2010), no. 6, 1119ÃŘ1139

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[5] H. Brezis, YY. Li and I. Shafrir. A sup+inf inequality for some nonlin- ear elliptic equations involving exponential nonlinearities. J.Funct.Anal.115 (1993) 344-358.

[6] Brezis. H, Marcus. M, Ponce. A. C. Nonlinear elliptic equations with mea- sures revisited. Mathematical aspects of nonlinear dispersive equations, 55- 109, Ann. of Math. Stud., 163, Princeton Univ. Press, Princeton, NJ, 2007.

[7] H. Brezis, F. Merle. Uniform estimates and Blow-up behavior for solutions of−∆u=V(x)euin two dimension. Commun. in Partial Differential Equa- tions, 16 (8 and 9), 1223-1253(1991).

[8] H. Brezis, W. A. Strauss. Semi-linear second-order elliptic equations in L1.

J. Math. Soc. Japan 25 (1973), 565-590.

[9] W. Chen, C. Li. A priori estimates for solutions to nonlinear elliptic equa- tions. Arch. Rational. Mech. Anal. 122 (1993) 145-157.

[10] C-C. Chen, C-S. Lin. A sharp sup+inf inequality for a nonlinear elliptic equation inR2. Commun. Anal. Geom. 6, No.1, 1-19 (1998).

[11] YY. Li, I. Shafrir. Blow-up analysis for solutions of−∆u=V eu in dimen- sion two. Indiana. Math. J. Vol 3, no 4. (1994). 1255-1270.

[12] YY. Li. Harnack Type Inequality: the method of moving planes. Commun.

Math. Phys. 200,421-444 (1999).

[13] L. Ma, J-C. Wei. Convergence for a Liouville equation. Comment. Math.

Helv. 76 (2001) 506-514.

[14] I. Shafrir. A sup+inf inequality for the equation −∆u = V eu. C. R.

Acad.Sci. Paris Sér. I Math. 315 (1992), no. 2, 159-164.

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