Home Mathematics Optimal regularity of stable solutions to nonlinear equations involving the p-Laplacian
Article
Licensed
Unlicensed Requires Authentication

Optimal regularity of stable solutions to nonlinear equations involving the p-Laplacian

  • Xavier Cabré ORCID logo EMAIL logo , Pietro Miraglio ORCID logo and Manel Sanchón ORCID logo
Published/Copyright: October 7, 2020

Abstract

We consider the equation - Δ p u = f ( u ) in a smooth bounded domain of n , where Δ p is the p-Laplace operator. Explicit examples of unbounded stable energy solutions are known if n p + 4 p p - 1 . Instead, when n < p + 4 p p - 1 , stable solutions have been proved to be bounded only in the radial case or under strong assumptions on f. In this article we solve a long-standing open problem: we prove an interior C α bound for stable solutions which holds for every nonnegative f C 1 whenever p 2 and the optimal condition n < p + 4 p p - 1 holds. When p ( 1 , 2 ) , we obtain the same result under the nonsharp assumption n < 5 p . These interior estimates lead to the boundedness of stable and extremal solutions to the associated Dirichlet problem when the domain is strictly convex. Our work extends to the p-Laplacian some of the recent results of Figalli, Ros-Oton, Serra, and the first author for the classical Laplacian, which have established the regularity of stable solutions when p = 2 in the optimal range n < 10 .

MSC 2010: 35B65; 35B35; 35J60

Communicated by Juan Manfredi


Award Identifier / Grant number: MTM2017-84214-C2-1-P

Award Identifier / Grant number: 2017SGR1392

Funding statement: Xavier Cabré and Pietro Miraglio are supported by grant MTM2017-84214-C2-1-P (Government of Spain) and are members of the research group 2017SGR1392 (Government of Catalonia).

A Technical lemmata

The first lemma of this section is a simple estimate for the L 1 -norm of Δ p u . We assume that u is a regular solution of (1.1) in B R and that the nonlinearity f is nonnegative. Since we use this bound several times throughout the paper, we report it here together with its elementary proof.

Lemma A.1.

Let u be a regular solution of - Δ p u = f ( u ) in B R R n , with f C 1 ( R ) nonnegative. Then, for every ρ ( 0 , R ) , we have

B ρ | Δ p u | 𝑑 x C R - ρ B R | u | p - 1 𝑑 x ,

where C > 0 is a constant depending only on n.

Proof.

First, we recall that since u W σ , loc 1 , 2 ( B R ) – see Remark 2.2 – we can take the distributional divergence of | u | p - 2 u .

We choose a nonnegative function η C c 1 ( B R ) such that η 1 in B ρ and | η | C R - ρ . Then, since - Δ p u 0 , we have

B R | Δ p u | η 𝑑 x = - B R div ( | u | p - 2 u ) η 𝑑 x = B R | u | p - 2 u η d x C R - ρ B R | u | p - 1 𝑑 x ,

and this concludes the proof. ∎

In Section 4, we also need an elementary Rellich-type criterion to establish strong convergence in L p - 1 ( B 1 ) whenever p 2 . This result will be applied with w k in its statement being a partial derivative of a stable solution u k .

Lemma A.2.

Let p 2 and let ( w k ) k be a sequence of weakly differentiable functions in L p - 1 ( B 1 ) such that

w k L p - 1 ( B 1 ) C 𝑎𝑛𝑑 | w k | p - 2 w k L 1 ( B 1 ) C

for some constant C independent of k. Then there exists a subsequence of ( w k ) k that converges strongly in L p - 1 ( B 1 ) .

Proof.

For w ~ k := | w k | p - 2 w k we have that

w ~ k L 1 ( B 1 ) C and w ~ k L 1 ( B 1 ) C ,

where C does not depend on k. Thus, the sequence ( w ~ k ) k is bounded in W 1 , 1 ( B 1 ) and from the compactness of the immersion W 1 , 1 ( B 1 ) L 1 ( B 1 ) we obtain that, up to a subsequence,

w ~ k w ~ strongly in  L 1 ( B 1 )

for some w ~ L 1 ( B 1 ) .

Now, defining w := | w ~ | p - 2 w ~ , we have that

| w k - w | p - 1 C n , p | | w k | p - 2 w k - | w | p - 2 w | = C n , p | w ~ k - w ~ | ,

where we used that for p 2 we have | a - b | p C n , p ( | a | p - 2 a - | b | p - 2 b ) ( a - b ) if a and b belong to n ; see [19, Chapter 1, Lemma 4.4]. As a consequence, up to subsequences, from the strong convergence of w ~ k to w ~ in L 1 ( B 1 ) we deduce that

w k w strongly in  L p - 1 ( B 1 ) .

This finishes the proof. ∎

The following result is a new interpolation inequality adapted to the p-Laplacian which holds for p 2 and every nice function in B 1 n , independently of its boundary values. It gives a control on the L p - 1 -norm of u in terms of the weighted L 1 -norm of the second derivatives of u plus the L p - 1 -norm of the function. We assume some regularity hypotheses on the function which are fulfilled by every stable regular solutions to - Δ p u = f ( u ) with f C 1 ( ) , by Remark 2.2. Note that, as for the interpolation inequalities of [26, Theorem 7.28], its validity in n follows immediately once it is proved in dimension one.

Proposition A.3.

Let p 2 , ε ( 0 , 1 ) , let B 1 be the unit ball of R n , and let u ( C 1 W 1 , p - 1 ) ( B 1 ) satisfy u W σ 1 , 1 ( B 1 ) with σ = | u | p - 2 . Then

(A.1) B 1 | u | p - 1 𝑑 x ε B 1 | u | p - 2 | D 2 u | 𝑑 x + C ε 1 - p B 1 | u | p - 1 𝑑 x ,

where C depends only on n and p.

Proof.

First, we observe that the regularity assumptions on u ensure that all the integrals in (A.1) are well defined.

We first prove (A.1) in dimension n = 1 . Given ε > 0 , let u have the regularity assumed in the statement with B 1 replaced by ( 0 , ε ) . We claim that

(A.2) inf ( 0 , ε ) | u | p - 1 C ε - p 0 ε | u | p - 1 𝑑 x ,

where the constant C > 0 depends only on p.

The inequality is trivial if inf ( 0 , ε ) | u | = 0 . Therefore, we assume that inf ( 0 , ε ) | u | > 0 and, by Bolzano’s theorem, either u > 0 in ( 0 , ε ) or u < 0 in ( 0 , ε ) . By eventually changing u to - u , we may assume that u > 0 in ( 0 , ε ) . For a , b satisfying 0 < a < ε 4 < 3 ε 4 < b < ε , we have

ε 2 inf ( 0 , ε ) u ( b - a ) inf ( 0 , ε ) u ( b - a ) inf ( a , b ) u a b u 𝑑 x = u ( b ) - u ( a ) .

Integrating this inequality in b ( 3 ε 4 , ε ) , we get

ε 2 8 inf ( 0 , ε ) u 3 ε 4 ε u 𝑑 x - ε 4 u ( a ) 0 ε | u | 𝑑 x - ε 4 u ( a ) .

Integrating now in a ( 0 , ε 4 ) ,

ε 3 32 inf ( 0 , ε ) u ε 4 0 ε | u | 𝑑 x - ε 4 0 ε 4 u 𝑑 x ε 2 0 ε | u | 𝑑 x .

Thus

inf ( 0 , ε ) | u | = inf ( 0 , ε ) u 16 ε 2 0 ε | u | 𝑑 x ,

and raising this inequality to p - 1 1 , we get

inf ( 0 , ε ) | u | p - 1 C ε - 2 ( p - 1 ) ( 0 ε | u | 𝑑 x ) p - 1 C ε - p 0 ε | u | p - 1 𝑑 x ,

where C depends only on p. This proves (A.2).

Therefore, by (A.2), there exists a point x 0 ( 0 , ε ) such that

(A.3) | u ( x 0 ) | p - 1 2 C ε - p 0 ε | u | p - 1 𝑑 x .

Let x ( 0 , ε ) and let I 0 ( 0 , ε ) be the interval with end points x 0 and x. Then

| | u ( x ) | p - 1 - | u ( x 0 ) | p - 1 | = | I 0 ( | u | p - 1 ) 𝑑 x | ,

and hence

| u ( x ) | p - 1 ( p - 1 ) 0 ε | u | p - 2 | u ′′ | 𝑑 x + | u ( x 0 ) | p - 1 .

Combining this inequality with (A.3) and integrating in x ( 0 , ε ) , we obtain

(A.4) 0 ε | u | p - 1 𝑑 x ( p - 1 ) ε 0 ε | u | p - 2 | u ′′ | 𝑑 x + C ε 1 - p 0 ε | u | p - 1 𝑑 x .

Note that we have not required any specific boundary values for u. Hence, given any bounded open interval I , for k we divide I into k disjoint intervals of length ε := | I | k . Now, using (A.4) in each of these intervals of length ε and adding up all the inequalities given by (A.4), we deduce

(A.5) I | u | p - 1 𝑑 x ( p - 1 ) ε I | u | p - 2 | u ′′ | 𝑑 x + C ε 1 - p I | u | p - 1 𝑑 x

for ε = | I | k . Since k is an arbitrary integer, as large as wished, we conclude that (A.5) holds for every I and ε > 0 . This establishes the proposition in dimension one – after replacing ε by ε p - 1 .

Finally, let B 1 be the unit ball of n , B 1 n - 1 the unit ball of n - 1 , u ( C 1 W 1 , p - 1 ) ( B 1 ) satisfy u W σ 1 , 1 ( B 1 ) , and denote x = ( x 1 , x ) × n - 1 and I x := { x 1 : ( x 1 , x ) B 1 } . Then, using (A.5), we have

B 1 | u x 1 | p - 1 𝑑 x = B 1 n - 1 𝑑 x I x 𝑑 x 1 | u x 1 ( x ) | p - 1
( p - 1 ) ε B 1 n - 1 𝑑 x I x 𝑑 x 1 | u x 1 ( x ) | p - 2 | u x 1 x 1 ( x ) | + C ε 1 - p B 1 n - 1 𝑑 x I x 𝑑 x 1 | u ( x ) | p - 1
= ( p - 1 ) ε B 1 | u x 1 ( x ) | p - 2 | u x 1 x 1 ( x ) | 𝑑 x + C ε 1 - p B 1 | u ( x ) | p - 1 𝑑 x ,

where C depends only on p. Since the same inequality holds for the partial derivatives with respect to each variable x k instead of x 1 (and we can replace ε by ε / ( p - 1 ) ), we conclude (A.1). ∎

We conclude this appendix with the statement of a general abstract lemma due to Simon [36] – see also [15, Lemma 3.1]. It is extremely useful to “absorb errors” in larger balls of quantities controlled in smaller balls.

Lemma A.4.

Let β R and C 0 > 0 . Let S : B [ 0 , + ] be a nonnegative function defined on the class B of open balls B R n and satisfying the following subadditivity property:

𝑖𝑓 B j = 1 N B j , then  𝒮 ( B ) j = 1 N 𝒮 ( B j ) .

Assume also that S ( B 1 ) < . Then there exists δ, depending only on n and β, such that if

ρ β 𝒮 ( B ρ / 4 ( y ) ) δ ρ β 𝒮 ( B ρ ( y ) ) + C 0 whenever  B ρ ( y ) B 1 ,

then

𝒮 ( B 1 / 2 ) C C 0 ,

where C depends only on n and β.

B An alternative proof of the higher integrability result (Lemma 3.2) using the Michael-Simon and Allard inequality

We present here an alternative proof of Lemma 3.2 based on using the Sobolev inequality of Michael-Simon and Allard on the level sets of a stable regular solution u. It gives a control on the L p + γ -norm of the gradient of u in terms of its L p -norm in a larger ball, with γ = 2 ( p - 1 ) n - 1 when n 4 and γ = 2 ( p - 1 ) 3 when n 3 – see Remark 3.3 for a comparison with the values of γ given by our other proof.

We first recall the celebrated Michael-Simon and Allard inequality, in the form presented in [31] – see also [12, Section 2] for a quick and easy-to-read proof of this important result. As pointed out in the beginning of the Introduction of [31], as well as in its Example 3, the inequality holds in C 2 hypersurfaces. This will be useful for our purposes.

Theorem B.1 (Michael-Simon [31] and Allard [2] inequality).

Let M be an ( n - 1 ) -dimensional C 2 -hypersurface of R n , q [ 1 , n - 1 ) , and let φ C 1 ( M ) have compact support in M. If M is compact without boundary, any function φ C 1 ( M ) is allowed. Then there exists a positive constant C, depending only on n and q, such that

(B.1) φ L q * ( M ) q C M { | T φ | q + | H φ | q } 𝑑 n - 1 ,

where q * = ( n - 1 ) q n - 1 - q is the Sobolev exponent, T denotes the tangential gradient to M, and H is the mean curvature of M, i.e., the sum of its n - 1 principal curvatures.

Alternative proof of Lemma 3.2.

We divide the proof into three steps.

Step 1. If n 3 , we can add additional artificial variables and reduce to the case n > 3 , by Remark 1.7. We thus assume that n > 3 and claim that

(B.2) 𝑑 t ( { u = t } B 1 / 2 | u | ( p - 1 ) ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1 C u L p ( B 1 ) p ,

where C depends only on n and p.

In order to prove (B.2), observe that the surface integral on the left-hand side of (B.2) can be equivalently computed over { u = t } B 1 / 2 or over { u = t } B 1 / 2 { | u | > 0 } . We use the Michael-Simon and Allard inequality (B.1) on the C 2 hypersurface[16] M = { u = t } { | u | > 0 } . We would like to apply the inequality to the function

φ = | u | p - 1 2 η ,

where η C c ( B 3 / 4 ) satisfies 0 η 1 and η 1 in B 1 / 2 ; however, this function will not have, in general, compact support in M = { u = t } { | u | > 0 } . Thus, in (B.1) we take the test function

φ ε = | u | p - 1 2 η ϕ ( | u | ε )

with ε > 0 , where ϕ C ( ) takes values into [ 0 , 1 ] , ϕ ( t ) = 1 if t 2 , and ϕ ( t ) = 0 if t 1 . Note that ϕ ( | u | ε ) is the cut-off function that we already used in the proof of Lemma 2.3. Using Fatou’s lemma, (B.1) with q = 2 < n - 1 , and the coarea formula, we obtain

(B.3)

𝑑 t ( { u = t } B 1 φ 2 ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1 lim inf ε 0 𝑑 t ( { u = t } B 1 φ ε 2 ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1
C lim inf ε 0 𝑑 t { u = t } B 1 { | u | > 0 } ( | T φ ε | 2 + H 2 φ ε 2 ) 𝑑 n - 1
= C lim inf ε 0 B 1 { | u | > 0 } | u | ( | T φ ε | 2 + H 2 φ ε 2 ) 𝑑 x .

Here the tangential gradient T and the mean curvature H are referred to the level set of u passing through a given point x. For the square modulus of the tangential gradient of φ ε , the Cauchy–Schwarz inequality gives

| T φ ε | 2 3 ( p - 1 ) 2 4 | u | p - 3 | T | u | | 2 η 2 ϕ 2 ( | u | ε ) + 3 | u | p - 1 | T η | 2 ϕ 2 ( | u | ε ) + 3 | u | p - 1 η 2 | T ϕ ( | u | ε ) | 2 .

Plugging this inequality into (B.3), using | T ϕ ( | u | ε ) | 2 | ϕ ( | u | ε ) | 2 , (2.7), the fact that | ϕ ( | u | ε ) | is bounded independently of ε and it is supported in { ε | u | 2 ε } , and that | u | 2 4 ε 2 in this set, we obtain

𝑑 t ( { u = t } B 1 ( | u | p - 1 2 η ) 2 ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1
C lim sup ε 0 B 1 { | u | > 0 } { 3 ( p - 1 ) 2 4 | u | p - 2 | T | u | | 2 η 2 + 3 | u | p | T η | 2 + H 2 | u | p η 2 } ϕ 2 ( | u | ε ) 𝑑 x
+ C lim sup ε 0 B 1 { ε < | u | < 2 ε } | u | p - 2 | D 2 u | 2 η 2 𝑑 x .

Now, using (2.4) and dominated convergence, we deduce that the last term is zero. Using that ϕ 2 1 in the first integral on the right-hand side of the inequality, we get

𝑑 t ( { u = t } B 1 ( | u | p - 1 2 η ) 2 ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1 C B 1 { | u | > 0 } { 3 ( p - 1 ) 2 4 | u | p - 2 | T | u | | 2 + H 2 | u | p } η 2 𝑑 x
+ C B 1 | u | p | T η | 2 𝑑 x .

Since H 2 ( n - 1 ) | A | 2 , we deduce that

𝑑 t ( { u = t } B 1 ( | u | p - 1 2 η ) 2 ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1
C B 1 { | u | > 0 } { ( p - 1 ) | u | p - 2 | T | u | | 2 + | A | 2 | u | p } η 2 𝑑 x + C B 1 | u | p 𝑑 x .

Finally, we use the stability condition in its geometric form, Theorem 1.8, to obtain

𝑑 t ( { u = t } B 1 ( | u | p - 1 2 η ) 2 ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1 C B 1 | u | p | η | 2 𝑑 x + C B 1 | u | p 𝑑 x C u L p ( B 1 ) p .

This proves (B.2).

Step 2. Now we show that, for almost every t ,

(B.4) { u = t } B 1 / 2 | u | p - 1 𝑑 n - 1 C u L p - 1 ( B 1 ) p - 1 C u L p ( B 1 ) p - 1 ,

where the constants C depend only on n and p. Note that this estimate is similar to (3.24), where we assumed u L p ( B 1 ) = 1 , but we cannot deduce (B.4) from (3.24) through Hölder’s inequality, since we do not have a control on the measure of { u = t } B 1 / 2 . However, the proofs of both estimates rely on the same idea.

First, we take η as defined in Step 1 and we claim that, for almost every t ,

(B.5) { u = t } B 1 | u | p - 1 η 𝑑 n - 1 = - { u > t } B 1 div ( η | u | p - 2 u ) 𝑑 x .

Observe that u is not regular enough to apply Sard’s theorem and deduce regularity of { u = t } for a.e. t, and hence we cannot integrate by parts in the set { u > t } B 1 . However, as in the proof of (3.25), we can use a smooth approximation K ε ( s ) of the characteristic function of + , and then send ε 0 , to establish (B.5).

From (B.5) we obtain that

{ u = t } B 1 | u | p - 1 η 𝑑 n - 1 B 1 | Δ p u | η 𝑑 x + B 1 | u | p - 2 | u η | 𝑑 x .

Now, since 0 η 1 has compact support in B 3 / 4 , we can use Lemma A.1 to obtain

B 1 | Δ p u | η 𝑑 x B 3 / 4 | Δ p u | 𝑑 x C u L p - 1 ( B 1 ) p - 1 .

Combining this with the previous bound, we conclude the proof of (B.4).

Step 3. Finally, from (B.2) and (B.4) we deduce (3.17). For this, we use Hölder’s inequality with exponents q = n - 1 n - 3 and q = n - 1 2 , as well as the coarea formula, to obtain

B 1 / 2 | u | p + 2 ( p - 1 ) n - 1 𝑑 x = 𝑑 t { u = t } B 1 / 2 | u | p - 1 | u | 2 ( p - 1 ) n - 1 𝑑 n - 1
𝑑 t ( { u = t } B 1 / 2 | u | ( p - 1 ) ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1 ( { u = t } B 1 / 2 | u | p - 1 𝑑 n - 1 ) 2 n - 1
C u L p ( B 1 ) 2 ( p - 1 ) n - 1 𝑑 t ( { u = t } B 1 / 2 | u | ( p - 1 ) ( n - 1 ) n - 3 𝑑 n - 1 ) n - 3 n - 1
C u L p ( B 1 ) p + 2 ( p - 1 ) n - 1 .

This concludes the alternative proof of Lemma 3.2. ∎

Acknowledgements

The authors would like to thank Lucio Boccardo and Luigi Orsina for a simplification in the proof of Lemma A.2.

References

[1] D. R. Adams, A note on Riesz potentials, Duke Math. J. 42 (1975), 765–778. 10.1215/S0012-7094-75-04265-9Search in Google Scholar

[2] W. K. Allard, On the First Variation of a Varifold, Ann. of Math. 95 (1972), 417–491. 10.2307/1970868Search in Google Scholar

[3] H. Brezis, Is there failure of the inverse function theorem?, Morse Theory, Minimax Theory and Their Applications to Nonlinear Differential Equations, New Stud. Adv. Math. 1, International Press, Somerville (2003), 23–33. Search in Google Scholar

[4] H. Brezis, T. Cazenave, Y. Martel and A. Ramiandrisoa, Blow up for u t - Δ u = g ( u ) revisited, Adv. Differential Equations 1 (1996), 73–90. 10.57262/ade/1366896315Search in Google Scholar

[5] H. Brezis and J. L. Vázquez, Blow-up solutions of some nonlinear elliptic problems, Rev. Mat. Complut. 10 (1997), 443–469. 10.5209/rev_REMA.1997.v10.n2.17459Search in Google Scholar

[6] X. Cabré, Regularity of minimizers of semilinear elliptic problems up to dimension 4, Comm. Pure Appl. Math. 63 (2010), 1362–1380. 10.1002/cpa.20327Search in Google Scholar

[7] X. Cabré, Boundedness of stable solutions to semilinear elliptic equations: A survey, Adv. Nonlinear Stud. 17 (2017), 355–368. 10.1515/ans-2017-0008Search in Google Scholar

[8] X. Cabré, A new proof of the boundedness results for stable solutions to semilinear elliptic equations, Discrete Contin. Dyn. Syst. 39 (2019), 7249–7264. 10.3934/dcds.2019302Search in Google Scholar

[9] X. Cabré, A. Capella and M. Sanchón, Regularity of radial minimizers of reaction equations involving the p-Laplacian, Calc. Var. Partial Differential Equations 34 (2009), 475–494. 10.1007/s00526-008-0192-3Search in Google Scholar

[10] X. Cabré and F. Charro, The optimal exponent in the embedding into the Lebesgue spaces for functions with gradient in the Morrey space, preprint (2019), https://arxiv.org/abs/1907.12982. 10.1016/j.aim.2021.107592Search in Google Scholar

[11] X. Cabré, A. Figalli, X. Ros-Oton and J. Serra, Stable solutions to semilinear elliptic equations are smooth up to dimension 9, Acta Math. 224 (2020), 187–252. 10.4310/ACTA.2020.v224.n2.a1Search in Google Scholar

[12] X. Cabré and P. Miraglio, Universal Hardy–Sobolev inequalities on hypersurfaces of Euclidean space, preprint (2019), https://arxiv.org/abs/1912.09282. 10.1142/S0219199721500632Search in Google Scholar

[13] X. Cabré and M. Sanchón, Semi-stable and extremal solutions of reaction equations involving the p-Laplacian, Comm. Pure Appl. Anal. 6 (2007), 43–67. 10.3934/cpaa.2007.6.43Search in Google Scholar

[14] D. Castorina and M. Sanchón, Regularity of stable solutions of p-Laplace equations through geometric Sobolev type inequalities, J. Eur. Math. Soc. 17 (2015), 2949–2975. 10.4171/JEMS/576Search in Google Scholar

[15] E. Cinti, J. Serra and E. Valdinoci, Quantitative flatness results and BV-estimates for stable nonlocal minimal surfaces, J. Differential Geom. 112 (2019), 447–504. 10.4310/jdg/1563242471Search in Google Scholar

[16] M. G. Crandall and P. H. Rabinowitz, Some continuation and variational methods for positive solutions of nonlinear elliptic eigenvalue problems, Arch. Ration. Mech. Anal. 58 (1975), 207–218. 10.1007/BF00280741Search in Google Scholar

[17] L. Damascelli and B. Sciunzi, Regularity, monotonicity and symmetry of positive solutions of m-Laplace equations, J. Differential Equations 206 (2004), 483–515. 10.1016/j.jde.2004.05.012Search in Google Scholar

[18] E. DiBenedetto, C 1 + α local regularity of weak solutions of degenerate elliptic equations, Nonlinear Anal. 8 (1983), 827–850. 10.21236/ADA120990Search in Google Scholar

[19] E. DiBenedetto, Degenerate Parabolic Equations, Universitext, Springer, New York, 1993. 10.1007/978-1-4612-0895-2Search in Google Scholar

[20] L. Dupaigne, Stable Solutions of Elliptic Partial Differential Equations, Chapman & Hall/CRC Monogr. Surv. Pure Appl. Math. 143, CRC Press, Boca Raton, 2011. 10.1201/b10802Search in Google Scholar

[21] A. Farina, B. Sciunzi and E. Valdinoci, On a Poincaré type formula for solutions of singular and degenerate elliptic equations, Manuscripta Math. 132 (2010), 335–342. 10.1007/s00229-010-0349-1Search in Google Scholar

[22] A. Farina, B. Sciunzi and E. Valdinoci, Bernstein and De Giorgi type problems: New results via a geometric approach, Ann. Sc. Norm. Super. Pisa Cl. Sci. (5) 7 (2008), 741–791. 10.2422/2036-2145.2008.4.06Search in Google Scholar

[23] A. Ferrero, On the solutions of quasilinear elliptic equations with a polynomial-type reaction term, Adv. Differential Equations 9 (2004), 1201–1234. 10.57262/ade/1355867901Search in Google Scholar

[24] J. García Azorero and I. Peral Alonso, On an Emden–Fowler type equation, Nonlinear Anal. 18 (1992), 1085–1097. 10.1016/0362-546X(92)90197-MSearch in Google Scholar

[25] J. García Azorero, I. Peral Alonso and J.-P. Puel, Quasilinear problems with exponential growth in the reaction term, Nonlinear Anal. 22 (1994), 481–498. 10.1016/0362-546X(94)90169-4Search in Google Scholar

[26] D. Gilbarg and N. S. Trudinger, Elliptic Partial Differential Equations of Second Order, Springer, Berlin, 2001. 10.1007/978-3-642-61798-0Search in Google Scholar

[27] E. H. Lieb and M. Loss, Analysis, Grad. Stud. Math. 14, American Mathematical Society, Providence, 1997. Search in Google Scholar

[28] G. M. Lieberman, Boundary regularity for solutions of degenerate elliptic equations, Nonlinear Anal. 12 (1988), 1203–1219. 10.1016/0362-546X(88)90053-3Search in Google Scholar

[29] P. Lindqvist, Notes on the p-Laplace equation, Report. University of Jyväskylä Department of Mathematics and Statistics 102, University of Jyväskylä, Jyväskylä, 2006. Search in Google Scholar

[30] H. Lou, On singular sets of local solutions to p-Laplace equations, Chin. Ann. Math. Ser. B 29 (2008), 521–530. 10.1007/s11401-007-0312-ySearch in Google Scholar

[31] J. H. Michael and L. M. Simon, Sobolev and mean value inequalities on generalized submanifolds of R n , Comm. Pure Appl. Math. 26 (1973), 361–379. 10.1002/cpa.3160260305Search in Google Scholar

[32] P. Miraglio, Boundedness of stable solutions to nonlinear equations involving the p-Laplacian, J. Math. Anal. Appl. 489 (2020), Article ID 124122. 10.1016/j.jmaa.2020.124122Search in Google Scholar

[33] G. Nedev, Regularity of the extremal solution of semilinear elliptic equations, C. R. Acad. Sci. Paris Sér. I Math. 330 (2000), 997–1002. 10.1016/S0764-4442(00)00289-5Search in Google Scholar

[34] M. Sanchón, Boundedness of the extremal solution of some p-Laplacian problems, Nonlinear Anal. 67 (2007), 281–294. 10.1016/j.na.2006.05.010Search in Google Scholar

[35] M. Sanchón, Regularity of the extremal solution of some nonlinear elliptic problems involving the p-Laplacian, Potential Anal. 27 (2007), 217–224. 10.1007/s11118-007-9053-5Search in Google Scholar

[36] L. Simon, Schauder estimates by scaling, Calc. Var. Partial Differential Equations 5 (1997), 391–407. 10.1007/s005260050072Search in Google Scholar

[37] P. Sternberg and K. Zumbrun, Connectivity of phase boundaries in strictly convex domains, Arch. Ration. Mech. Anal. 141 (1998), 375–400. 10.1007/s002050050081Search in Google Scholar

[38] P. Tolksdorf, Regularity for a more general class of quasilinear elliptic equations, J. Differential Equations 51 (1984), 126–150. 10.1016/0022-0396(84)90105-0Search in Google Scholar

Received: 2020-06-02
Revised: 2020-09-04
Accepted: 2020-09-09
Published Online: 2020-10-07
Published in Print: 2022-10-01

© 2020 Walter de Gruyter GmbH, Berlin/Boston

Downloaded on 31.12.2025 from https://www.degruyterbrill.com/document/doi/10.1515/acv-2020-0055/html
Scroll to top button