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Submitted on 11 Oct 2019

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Some uniform estimates for scalar curvature type

equations

Samy Skander Bahoura

To cite this version:

Samy Skander Bahoura. Some uniform estimates for scalar curvature type equations. Pacific Journal of Mathematics, Mathematical Sciences Publishers, 2019, 301 (1), pp.55-65. �10.2140/pjm.2019.301.55�. �hal-02313839�

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dx.doi.org/10.2140/pjm.2019.301.55

SOME UNIFORM ESTIMATES

FOR SCALAR CURVATURE TYPE EQUATIONS

SAMYSKANDERBAHOURA

We consider the prescribed scalar curvature equation on an open set  of Rn, −1u = V u(n+2)/(n−2)+un/(n−2) with V ∈ C1,α (0< α ≤ 1), and we

prove the inequality supKu × infu ≤ c where K is a compact set of.

In dimension 4, we have an idea on the supremum of the solution of the prescribed scalar curvature if we control the infimum. For this case we suppose the scalar curvature C1,α (0< α ≤ 1).

1. Introduction and main result

In our work, we denote by1 = ∇i∇i the Laplace–Beltrami operator in dimension n ≥2.

Without loss of generality, we suppose = B = B2(0) the ball of radius 2

centered at 0 ofRn.

Here, we study some a priori estimates of type sup × inf for a perturbed prescribed scalar curvature equation in all dimensions n ≥ 4.

We have a counterexample to the sharp sup × inf inequality for the prescribed scalar curvature[Chen and Lin 1997, Proposition 4.3]. In our work the perturbation by a subcritical term is a sufficient condition to obtain such an inequality.

The sup × inf inequality is characteristic of those equations as the usual Harnack inequalities are for harmonic functions.

Note that the prescribed scalar curvature equation was studied a lot. We can find — see, for example, [Aubin 1998; Bahoura 2004; Brezis and Merle 1991;

Brezis et al. 1993;Chen and Lin 1997;1998;Li 1993;1995;1996;1999;Li and Shafrir 1994;Li and Zhang 2004;Li and Zhu 1999;Shafrir 1992] — many results about uniform estimates in dimensions n = 2 and n ≥ 3.

In dimension 2, the corresponding equation is

(E0) −1u = V eu.

Note that Shafrir[1992]obtained an inequality of type sup u + C inf u< c with only an L∞assumption on V .

MSC2010: 35B44, 35B45, 35B50, 35J60, 53C21.

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To obtain exactly the estimate sup u + inf u< c, Brezis, Li and Shafrir[Brezis et al. 1993]assumed that the prescribed scalar curvature V is Lipschitz continuous. Later, Chen and Lin[1998]proved that, if V is uniformly Hölder continuous, we can obtain a sup + inf inequality.

In dimension n ≥ 3, the prescribed curvature equation on general manifold M is (E0

0) −1u + Rgu = V u(n+2)/(n−2).

When M =Sn, Li[1993;1995;1996]proved a priori estimates for the solutions

of the previous equation. He used the notion of simple isolated points and some flatness conditions on V .

If we suppose n = 3, 4, we can find in[Li and Zhang 2004;Li and Zhu 1999]

a uniform bound for the energy and a sup × inf inequality. Note that Li and Zhu

[1999]proved the compactness of the solutions to the Yamabe problem using the positive mass theorem.

In[Bahoura 2004], we can see (on a bounded domain ofR4) that we have a uniform estimate for the solutions of(E00)(n = 4 and Euclidean case) by assuming that those solutions are bounded below by a positive constant; in this case we have assumed that the prescribed scalar curvature V is only Lipschitz.

Here we extend some result of[Bahoura 2004]to equations with nonlinear terms or with minimal condition on the prescribed scalar curvature.

For the Euclidean case, Chen and Lin[1997] got some a priori estimates for general equations

(E000) −1u = V u(n+2)/(n−2)+g(u)

with some assumption on g and the Li-flatness conditions on V .

Here, we give some a priori estimates with some minimal conditions on the prescribed curvature, for perturbed scalar curvature equation, in all dimensions n ≥4.

In our work, we use the blow-up analysis, the moving-plane method and a flatness condition (of order 1) for the prescribed scalar curvature. Note that the flatness condition which we use is also obtained by a moving-plane argument of Chen and Lin[1997]. The method of moving plane was developed in particular by Gidas, Ni and Nirenberg[Gidas et al. 1979]and Serrin[1971].

First, consider the equation

(E1) −1u = V u(n+2)/(n−2)+un/(n−2)

with 0< a ≤ V (x) ≤ b and kV kC1,α ≤ A, 0< α ≤ 1. We have:

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Theorem 1. For all a, b, A, α > 0 (0 < α ≤ 1), and all compact sets K of  of dimension n ≥4, there is a positive constant c = c(a, b, A, α, K, , n) such that

sup

K

u ×inf

 u ≤ c

for all solutions u of(E1)relative to V .

Now, if we suppose V ∈ C1() and V ≥ a > 0, we have:

Theorem 2. For all a> 0, V and all compact K of  of dimension n ≥ 4, there is a positive constant c = c(a, V, K, , n) such that

sup

K

u ×inf

 u ≤ c

for all solutions u of(E1)relative to V .

Now, we suppose n = 4, and we consider the equation (prescribed scalar curvature equation)

(E2) −1u = V u3 on ⊂R4

with 0< a ≤ V (x) ≤ b and kV kC1,α ≤ A, 0< α ≤ 1. We have:

Theorem 3. For all a, b, m, A, α > 0 (0 < α ≤ 1) and all compact K of , there is a positive constant c = c(a, b, m, A, α, K, ) such that

sup

K

u ≤ c if min

 u ≥ m

for all solutions u of(E2)relative to V .

If we suppose n = 4 and V ∈ C1() and V ≥ a > 0 on , we have:

Theorem 4. For all a, m > 0, V ∈ C1() and all compact K ∈ , there is a positive

constant c = c(a, m, V, K, ) such that sup

K

u ≤ c if min

 u ≥ m

for all solutions u of(E2)relative to V .

2. Proofs of the theorems Proof of Theorems1and2.

Proof ofTheorem 1.Without loss of generality, we suppose = B1 the unit ball

ofRn. We want to prove an a priori estimate around 0. Let(ui) and (Vi) be sequences of functions on  such that

−1ui=Viui(n+2)/(n−2)+u n/(n−2)

i , ui > 0,

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We argue by contradiction, and we suppose that the sup × inf is not bounded. We have that for all c, R > 0 there exists uc,R a solution of(E1)such that

(H ) Rn−2 sup

B(0,R)

uc,R×inf M uc,R

≥c.

Proposition (blow-up analysis). There is a sequence of points(yi)i, yi →0, and

two sequences of positive real numbers(li)i and(Li)i (see below), li →0 and

Li → +∞, such that, if we setvi(y) = ui(y + yi)/ui(yi), we have

0< vi(y) ≤ βi ≤2(n−2)/2, βi →1, vi(y) →  1 1 + |y|2 (n−2)/2

uniformly on all compact sets ofRn,

l(n−2)/2i ui(yi) × inf B1

ui → +∞,

Proof. We use the hypothesis(H ); we take two sequences Ri > 0, Ri →0, and

ci → +∞such that Ri(n−2) sup B(0,Ri) ui×inf B1 ui ≥ci → +∞.

Let xi ∈ B(x0, Ri) be a point such that supB(0,Ri)ui = ui(xi) and si(x) = (Ri− |x − xi|)(n−2)/2ui(x), x ∈ B(xi, Ri). Then xi →0. We have max B(xi,Ri) si(x) = si(yi) ≥ si(xi) = Ri(n−2)/2ui(xi) ≥ √ ci → +∞. We set li=Ri−|yi−xi|, ui(y)=ui(yi+y), vi(z)= ui[yi+(z/[ui(yi)]2/(n−2))] ui(yi) . Clearly, we have yi →x0. We take Li = li (ci)1/2(n−2) [ui(yi)]2/(n−2)= [si(yi)]2/(n−2) c1i/2(n−2) ≥ c 1/(n−2) i c1i/2(n−2) =ci1/2(n−2)→ +∞. If |z| ≤ Li, then y = [yi+z/[ui(yi)]2/(n−2)] ∈B(yi, δili) with δi=1/(ci)1/2(n−2)

and |y − yi|< Ri− |yi−xi|; thus, |y − xi|< Ri and si(y) ≤ si(yi). We can write

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But |y − yi| ≤δili, Ri > li and Ri− |y − xi| ≥ Ri− |xi−yi| −δili> li−δili= li(1 − δi). We obtain 0< vi(z) = ui(y) ui(yi) ≤  li li(1 − δi) (n−2)/2 ≤2(n−2)/2. We setβi =(1/(1 − δi))(n−2)/2; clearly, we haveβi →1.

The functionvi satisfies

−1vi =Veivi(n+2)/(n−2)+

vn/(n−2) i

[ui(yi)]2/(n−2)

,

where eVi(y) = Vi[y + y/[ui(yi)]2/(n−2)]. Without loss of generality, we can suppose

that eVi →V(0) = n(n − 2).

We use the elliptic estimates of the Ascoli and Ladyzhenskaya theorems to have the uniform convergence of(vi) to v on a compact set ofRn. The functionv satisfies

−1v = n(n − 2)vN −1, v(0) = 1, 0 ≤v ≤ 1 ≤ 2(n−2)/2, N = 2n n −2. By the maximum principle, we havev > 0 onRn. If we use the result of Caffarelli, Gidas and Spruck[Caffarelli et al. 1989], we obtainv(y) = (1/(1 + |y|2))(n−2)/2.

We have the same properties as in[Bahoura 2004]. 

Remark. When we use the convergence on compact sets of the sequence(vi), we

can take an increasing sequence of compact sets and we see that we can obtain a sequence(i) such that i →0 and after we choose(eRi) such that eRi → +∞and

finally

e

Rin−2kvi−vkB(0,

e Ri)≤i.

We can say that we are in the case of[Chen and Lin 1997, step 1 of the proof of Theorem 1.2].

Fundamental point (a consequence of the blow-up). According to the work of Chen and Lin[1997, step 2 of the proof of Theorem 1.3], in the blow-up point, the prescribed scalar curvature V is such that

(P0) lim

i →+∞

|∇Vi(yi)| = 0.

Polar coordinates (moving-plane method). Now we must use the same method as in[Bahoura 2004, Theorem 1]. We will use the moving-plane method.

We must prove[Bahoura 2004, Lemma 2]. We set t ∈ ]−∞, − log 2] and θ ∈Sn−1:

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We consider the operator L =∂t t+1σ−(n−2)2/4, with 1σthe Laplace–Beltrami

operator onSn−1.

The functionwi satisfies

−Lwi =ViwiN −1+et×win/(n−2), N =

2n n −2.

Remark. Here wi is a solution to the previous equation with a perturbed term

which contains et. The term et is fundamental in the computations; it corrects the variation of Vi.

Forλ ≤ 0, we set

tλ=2λ − t, wλ

i(t, θ) = wi(tλ, θ), Vλi(t, θ) = Vi(tλ, θ).

First, like in[Bahoura 2004], we have the following lemma. Lemma 5. Let Aλbe the property

Aλ= {λ ≤ 0 | there exists (tλ, θλ) ∈ ]λ, ti] ×Sn−1, wiλ(tλ, θλ) − wi(tλ, θλ) ≥ 0}. Then there isν ≤ 0 such that, for λ ≤ ν, Aλis not true.

Remark. Here we choose ti =log

li, where li is chosen as in the proposition.

Like in proof of the Theorem 1 of[Bahoura 2004], we want to prove the following lemma.

Lemma 6. Forλ ≤ 0 we have

wiλ−wi ≤0 =⇒ −L(wiλ−wi) ≤ 0

on ]λ, ti] ×Sn−1.

Like in[Bahoura 2004], we have:

A useful point. Letξi =sup{λ ≤ λi =2 + logηi|wiλ−wi < 0 on ]λ, ti] ×Sn−1}.

The realξi exists.

First,

wi(2ξi−t, θ) = wi[(ξi−t +ξi−logηi−2) + (log ηi+2)].

Proof ofLemma 6. In fact, for each i we haveλ = ξi ≤logηi +2, whereηi =

[ui(yi)](−2)/(n−2).

Note that

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if we use the definition ofwi, then forξi ≤t, wi(2ξi−t, θ) =e[(n−2)(ξi−t +ξi−logηi−2)]/2en−2v i[θe2e(ξi−t)+(ξi−logηi−2)] ≤2(n−2)/2en−2=c. We know that −L(wξi i −wi) = [Vξi i (w ξi i )(n+2)/(n−2)−Viwi(n+2)/(n−2)] + [et ξi (wξi i ) n/(n−2) etwin/(n−2)].

We denote by Z1and Z2the terms

Z1=(Vξii−Vi)(w ξi i )(n+2)/(n−2)+Vi[(w ξi i )(n+2)/(n−2)−wi(n+2)/(n−2)] and Z2=et ξi [(wξi i ) n/(n−2)w in/(n−2)] +win/(n−2)(et ξi −et). Like in the proof of Theorem 1 of[Bahoura 2004], we have

wiξi ≤wi and wiξi(t, θ) ≤ c for all (t, θ) ∈ [ξi, − log 2] ×Sn−1,

where c is a positive constant independent of i andwξi

i forξi ≤logηi+2.

The(P0)hypothesis. Now we use(P0)(this hypothesis is the same hypothesis as in

the first part of the paper: |∇ Vi(yi)| → 0). We write

|∇Vi(yi+etθ) − ∇Vi(yi)| ≤ Aeαt, Thus, Vi(yi+et ξi θ)−Vi(yi+etθ)−h∇Vi(yi) | θi(et ξi −et) ≤ A 1 +α[e (1+α)tξi −e(1+α)t]. Then |Vξi i −Vi| ≤ |o(1)|(e t etξi). Thus, Z1≤ |o(1)|(wiξi)(n+2)/(n−2)(e tetξi) and Z 2≤(wiξi) n/(n−2) ×(etξi −et). Then −L(wξi i −wi) ≤ (wξii) n/(n−2)[(|o(1)|wξi i 2/(n−2) −1)(et−etξi)] ≤ 0.

The lemma is proved. 

We set

ξi =sup{µ ≤ log ηi+2 |wiµ(t, θ) − wi(t, θ) ≤ 0 for all (t, θ) ∈ [µ, ti] ×Sn−1},

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Like in the proof of Theorem 1 of[Bahoura 2004], the maximum principle implies min θ∈Sn−1 wi(ti, θ) ≤ max θ∈Sn−1 wi(2ξi−ti). But wi(ti, θ) = etiui(yi+etiθ) ≥ eti min ui and wi(2ξi−ti) ≤ c0 ui(yi) ; thus, li(n−2)/2ui(yi) × min ui≤c.

The proposition is contradicted. 

Proof ofTheorem 2.The proof ofTheorem 2is similar to the proof ofTheorem 1. Only the “fundamental point” changes.

According to the work of Chen and Lin[1997, step 2 of the proof of Theorem 1.1], in the blow-up point, the prescribed scalar curvature V is such that

∇V(0) = 0.

The function ∇ V is continuous on Br(0) (with r small enough), so it is uniformly

continuous and we write (because yi →0)

|∇V(yi+y) − ∇V (yi)| ≤  for |y| ≤ δ  r for all i.

Thus,

|Vξi V | ≤ o(1)(etetξi).

We see that we have the same computations as in the “polar coordinates” in the

proof ofTheorem 1. 

Proof of Theorems3and4. Here, only the “polar coordinates” change; the propo-sition of the first theorem stays true. First, we have:

Fundamental point (a consequence of the blow-up). According to the work of Chen and Lin[1997, step 2 of the proof of Theorem 1.3], in the blow-up point, the prescribed scalar curvature V is such that:

Case 1(Theorem 3). limi →+∞|∇Vi(yi)| = 0.

We write |∇Vi(yi+etθ) − ∇Vi(yi)| ≤ Aeαt. Thus, |Vξi i −Vi| ≤ |o(1)|(e t etξi). Case 2(Theorem 4). ∇V(0) = 0.

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The function ∇ V is continuous on Br(0) (for r small enough), so it is uniformly

continuous and we write (because yi →0)

|∇V(yi+y) − ∇V (yi)| ≤  for |y| ≤ δ  r for all i.

Thus,

|VξiV | ≤ o(1)(etetξi),

Conclusion of the proofs of Theorems3and4. Finally, we can note that we are in the case of Theorem 2 of[Bahoura 2004]. We have the same computations if we consider the function

wi(t, θ) = wi(t, θ) −

m 2e

t.

We set L =∂t t+1σ−1, where1σ is the Laplace–Beltrami operator onS3, and

Vi(t, θ) = Vi(yi+etθ).

Like in[Bahoura 2004], we want to prove the following lemma.

Lemma 7. wξi

i −wi ≤0 =⇒ −L(w ξi

i −wi) ≤ 0.

Proof ofLemma 7.We have −L(wξi i −wi) = Vξii(wξ i i )3−Viw3i. Then −L(wξi i −wi) = (Vξii−Vi)(wiξi) 3+ [(wξi i ) 3w3 i]Vi. For t ∈ [ξi, ti]andθ ∈S3, |Vξi i (t, θ) − Vi(t, θ)| = |Vi(yi+e2ξi−tθ) − Vi(yi+etθ)| ≤ |o(1)|(et−e2ξi−t).

The real ti = log

li → −∞, where li is chosen as in the proposition of

Theorem 1. But ifwξi i −wi≤0, we obtain wξi i −wi ≤ m 2(e 2ξi−tet) < 0. Using the fact that 0< wξi

i < wi, we have (wξi i ) 3w3 i =(wξ i i −wi)[(w ξi i ) 2+wξi i wi+(wi) 2] ≤3(wξi i −wi) × (w ξi i ) 2.

Thus, we have for t ∈ [ξi, ti]andθ ∈S3

(wξi i ) 3w i3≤3 m 2 (w ξi i ) 2(e2ξi−tet). We can write (∗∗) −L(wξi i −wi) ≤ (wξii) 2 3 2m Vi− |o(1)|wiξ i(e2ξi−tet).

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We know that, for t ≤ log(li) − log 2 + log ηi, we have wi(t, θ) = et× ui(yi+etθ/ui(yi)) ui(yi) ≤2et. We find wiξi(t, θ) ≤ 2e2 r 8 a, becauseξi−logηi ≤2 +12log(8/V (0)) and ξi ≤t ≤ ti.

Finally,(∗∗)is negative and the lemma is proved. 

Now, if we use the Hopf maximum principle, we obtain min

θ∈S3wi(ti, θ) ≤ maxθ∈S3wi(2ξi

−ti, θ),

which implies that

liui(yi) ≤ c.

It is a contradiction. 

References

[Aubin 1998] T. Aubin,Some nonlinear problems in Riemannian geometry, Springer, 1998. MR Zbl [Bahoura 2004] S. S. Bahoura,“Majorations du type sup u × inf u ≤ c pour l’équation de la courbure scalaire prescrite sur un ouvert deRn, n ≥ 3”, J. Math. Pures Appl.(9) 83:9 (2004), 1109–1150. MR Zbl

[Brezis and Merle 1991] H. Brezis and F. Merle,“Uniform estimates and blow-up behavior for solutions of −1u = V (x)eu in two dimensions”, Comm. Partial Differential Equations 16:8-9 (1991), 1223–1253. MR Zbl

[Brezis et al. 1993] H. Brezis, Y. Y. Li, and I. Shafrir,“A sup + inf inequality for some nonlinear elliptic equations involving exponential nonlinearities”, J. Funct. Anal. 115:2 (1993), 344–358. MR Zbl

[Caffarelli et al. 1989] L. A. Caffarelli, B. Gidas, and J. Spruck,“Asymptotic symmetry and local behavior of semilinear elliptic equations with critical Sobolev growth”, Comm. Pure Appl. Math. 42:3 (1989), 271–297. MR Zbl

[Chen and Lin 1997] C.-C. Chen and C.-S. Lin,“Estimates of the conformal scalar curvature equation via the method of moving planes”, Comm. Pure Appl. Math. 50:10 (1997), 971–1017. MR Zbl [Chen and Lin 1998] C.-C. Chen and C.-S. Lin,“A sharp sup + inf inequality for a nonlinear elliptic

equation inR2”, Comm. Anal. Geom. 6:1 (1998), 1–19. MR Zbl

[Gidas et al. 1979] B. Gidas, W. M. Ni, and L. Nirenberg,“Symmetry and related properties via the maximum principle”, Comm. Math. Phys. 68:3 (1979), 209–243. MR Zbl

[Li 1993] Y. Y. Li, “Prescribing scalar curvature onSnand related problems”, C. R. Acad. Sci. Paris Sér. I Math.317:2 (1993), 159–164. MR Zbl

[Li 1995] Y. Y. Li,“Prescribing scalar curvature onSnand related problems, I”, J. Differential Equations120:2 (1995), 319–410. MR Zbl

[Li 1996] Y. Y. Li,“Prescribing scalar curvature onSnand related problems, II: Existence and compactness”, Comm. Pure Appl. Math. 49:6 (1996), 541–597. MR Zbl

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[Li 1999] Y. Y. Li,“Harnack type inequality: the method of moving planes”, Comm. Math. Phys. 200:2 (1999), 421–444. MR Zbl

[Li and Shafrir 1994] Y. Y. Li and I. Shafrir,“Blow-up analysis for solutions of −1u = V euin dimension two”, Indiana Univ. Math. J. 43:4 (1994), 1255–1270. MR Zbl

[Li and Zhang 2004] Y. Y. Li and L. Zhang,“A Harnack type inequality for the Yamabe equation in low dimensions”, Calc. Var. Partial Differential Equations 20:2 (2004), 133–151. MR Zbl [Li and Zhu 1999] Y. Y. Li and M. Zhu,“Yamabe type equations on three-dimensional Riemannian

manifolds”, Commun. Contemp. Math. 1:1 (1999), 1–50. MR Zbl

[Serrin 1971] J. Serrin,“A symmetry problem in potential theory”, Arch. Rational Mech. Anal. 43 (1971), 304–318. MR Zbl

[Shafrir 1992] I. Shafrir, “A Sup + Inf inequality for the equation −1u = V eu”, C. R. Acad. Sci.

Paris Sér. I Math.315:2 (1992), 159–164. MR Zbl

SAMYSKANDERBAHOURA

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