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HAL Id: hal-01823210

https://hal.archives-ouvertes.fr/hal-01823210v2

Preprint submitted on 4 Jul 2018

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A uniform result in dimension 2

Samy Skander Bahoura

To cite this version:

Samy Skander Bahoura. A uniform result in dimension 2. 2018. �hal-01823210v2�

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A uniform result in dimension 2.

Samy Skander Bahoura

Université Pierre et Marie Curie, 75005, Paris, France.

Abstract

We give a uniform result in dimension 2 for the solutions to an equation on compact Riemannian surface without boundary.

Keywords: dimension 2, Riemannian surface without boundary. Uniform result.

1 Introduction and Main result

We set ∆ = −∇ i (∇ i ) the Laplace-Beltrami operator. We are on compact Rie- mannian surface (M, g) without boundary.

We start with the following example: for all ǫ > 0 the constant functions z ǫ = log ǫ

a with a > 0, are solutions to ∆z ǫ +ǫ = ae z

ǫ

and tend to −∞ uniformly on M .

Question: What’s about the solutions u ǫ to the following equation

∆u ǫ + ǫ = V ǫ e u

ǫ

, (E ǫ ) with 0 < a ≤ V ǫ (x) ≤ b < +∞ on M ?

Next, we assume V ǫ Hölderian and V ǫ → V in L

The equation (E ǫ ) is of prescribed scalar curvature type equation. The term ǫ replace the scalar curvature.

Theorem 1.1 . If ǫ → 0, the solutions u ǫ to (E ǫ ) satisfy:

sup

M

u ǫ → −∞.

By using the same arguments of the next theorem, we have:

E-mails: samybahoura@yahoo.fr, samybahoura@gmail.com

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Theorem 1.2 . If ǫ → 0, the solutions u ǫ to (E ǫ ) satisfy:

u ǫ − log ǫ → k ∈ R.

uniformly on M .

Thus, we have a unifrom bound for the solutions:

k

1

+ log ǫ ≤ u ǫ ≤ log ǫ + k

2

.

We also have another proof of the uniqueness result which appear in [2].

This proof uses Brezis Merle arguments.

Theorem 1.3 . If ǫ → 0, the solutions u ǫ to (E ǫ ) with V ǫ ≡ 1, are such:

u ǫ ≡ log ǫ.

2 Proof of the theorems 1,2,3.

Proof of theorem 1:

We have:

Z

M

V ǫ e u

ǫ

→ 0. (∗)

Let’s consider x ǫ a point such that max M u ǫ = u ǫ (x ǫ ), then x ǫ → x

0

. We consider a neighborhood of x

0

and we use isothermal coordinates around x

0

(see [6]), there exists α > 0 and a regular function φ such that:

E

u ǫ + ǫe φ = V ǫ e φ e u

ǫ

in B(0, α).

The metric g of M satisfies g = e φ (dx

2

+ dy

2

).

Let’s consider u

0

such that:

E

u

0

= e φ in B(0, α).

(with Dirichlet condition for example).

The function v ǫ = u ǫ + ǫu

0

satisfies:

E

v ǫ = ˜ V ǫ e v

ǫ

, with V ˜ ǫ = V ǫ e φ−ǫu

0

. We use (∗) to have:

Z

B(0,α)

e v

ǫ

→ 0 and 0 < a ˜ ≤ V ˜ ǫ ≤ ˜ b. (∗∗)

with α > 0.

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The sequence v ǫ satisfies all the conditions of the theorem of Brezis and Merle, see [4].

As v ǫ satisfy (∗∗), the last condtion of the theorem of [4] is not possible.

Now, suppose that the first assertion of the theorem of Brezis and Merle is true. We have the local boundedness result. We can say that u ǫ converge uniformly on M to a fonction u and in C

2

topology by the elliptic estimates.

If we tend ǫ to 0 we get that u satisfies in the sense of distributions:

∆u = V e u .

If we integrate the equation, we have a contradiction (since 0 < a ≤ V ≤ b < +∞.

Thus, u ǫ satisfies the second assertion of the theorem of [4] and thus u ǫ

diverge uniformly to −∞ on M . Proof of Theoreme 2,3:

We set,

w ǫ = u ǫ − log ǫ.

Then, w ǫ is solution to:

∆w ǫ + ǫ = ǫV ǫ e w

ǫ

.

We use Brezis and Merle’s theorem and the previous arguments of theoerm 1, to have a convergence to a constant:

w ǫ → w

= ct, uniformly on M .

In isothermal coordinates around x

0

= lim x ǫ with x ǫ such that, w ǫ (x ǫ ) = max M w ǫ , as in the previous case

E

w ǫ + ǫe φ = ǫe φ V ǫ e w

ǫ

in B(0, α).

The metric g of M satisfies g = e φ (dx

2

+ dy

2

). Let’s consider u

0

such that:

E

u

0

= e φ in B(0, α).

(with Dirichlet condition for example).

The function v ǫ = w ǫ + ǫu

0

satisfies:

E

v ǫ = ˜ V ǫ e v

ǫ

, with V ˜ ǫ = ǫV ǫ e φ−ǫu

0

.

One can apply the theorem of Brezis and Merle, see [4].

First we have,

Z

M

V ǫ e w

ǫ

= |M |,

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which imply,

w ǫ 6→ −∞, and,

Z

M

ǫV ǫ e w

ǫ

= ǫ|M | → 0, which imply the non-concentration.

And,

w ǫ → w

, in the C

2

topology with,

∆w

= 0 ⇒ w

≡ k ∈ R.

For the third theorem we have:

Z

M

e w

ǫ

= |M | ⇒ k = 0.

We write:

w ǫ = ¯ w ǫ + f i , with the fact that,

Z

M

f i = 0,

and, f i is solution to:

∆f i = ǫ i (e w

¯i+fi

− 1) = ǫ i (e w

¯i

(1 + f i + O(f i

2

)) − 1), We multiply the equation by f i and we integrate, we obtain:

||∇f i ||

2

L

2

= o(||f i ||

2

L

2

).

This is in contradiction with the Poincaré inequality if f i 6≡ 0.

Thus,

f i ≡ 0, w i ≡ w ¯ i = 0.

References

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

[2] Bartolucci, D. Uniqueness and bifurcation for seminilinear elliptic equations

on closed surfaces. Calculus of Variations and PDEs, 2010, Volume 38, Issue

3,4, pp 503-519.

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

[4] H.Brezis and F.Merle, Uniform estimates and blow-up bihavior for solutions of −∆u = V e u in two dimensions, Commun Partial Differential Equations 16 (1991), 1223-1253.

[5] C.C.Chen, C.S. Lin. A sharp sup+inf inequality for a nonlinear elliptic equation in R

2

. Commun. Anal. Geom. 6, No.1, 1-19 (1998).

[6] C.C. Chern. An elementary proof of the existence of isothermal parameters on a surface. Proc. Am. Math. Soc. 6, 771-782 (1955).

[7] O. Druet, E. Hebey, F.Robert, Blow-up theory in Riemannian Geometry, Princeton University Press.

[8] D. Gilbarg, N.S. Trudinger. Elliptic Partial Differential Equations of Sec- ond order, Berlin Springer-Verlag, Second edition, Grundlehern Math.

Wiss.,224, 1983.

[9] E. Hebey, Analyse non lineaire sur les Variétés, Editions Diderot.

[10] YY. Li. Harnack Type Inequality: the Method of Moving Planes. Commun.

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

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

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

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