Home Existence and regularity for a p-Laplacian problem in ℝN with singular, convective, and critical reaction
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Existence and regularity for a p-Laplacian problem in ℝN with singular, convective, and critical reaction

  • Laura Baldelli and Umberto Guarnotta EMAIL logo
Published/Copyright: November 26, 2024

Abstract

We prove an existence result for a p-Laplacian problem set in the whole Euclidean space and exhibiting a critical term perturbed by a singular, convective reaction. The approach used combines variational methods, truncation techniques, and concentration compactness arguments, together with set-valued analysis and fixed point theory. De Giorgi’s technique, a priori gradient estimates, and nonlinear regularity theory are employed to obtain local C 1 , α regularity of solutions, as well as their pointwise decay at infinity. The result is new even in the non-singular case, also for the Laplacian.

MSC 2010: 35J92; 35J20; 35B08; 35B45

1 Introduction

In this article, we consider the problem

Δ p u = λ w ( x ) f ( u , u ) + u p * 1 , in R N , u > 0 , in R N , ( P λ ) u ( x ) 0 , as x + ,

where 1 < p < N (whence N 2 ), Δ p is the p-Laplacian operator, λ > 0 , and p * N p N p is the Sobolev critical exponent. We assume the following hypotheses:

  1. The function f : ( 0 , + ) × R N ( 0 , + ) is a continuous function obeying

    c 1 s γ f ( s , ξ ) c 2 ( s γ + ξ r 1 ) , ( s , ξ ) ( 0 , + ) × R N ,

    for some 0 < γ < 1 < r < p and c 1 , c 2 > 0 .

  2. The function w : R N ( 0 , + ) belongs to L 1 ( R N ) L ( R N ) and satisfies the following conditions:

    (1.1) There exist c 3 , R > 0 and l > N + γ N p p 1 such that w ( x ) c 3 x l x B R e ;

    (1.2) There exist x 0 R N and ϱ , ω > 0 such that inf B ϱ ( x 0 ) w ω .

It is worth noticing that (1.2) can be relaxed to w 0 : indeed, it is used only in the proof of Lemma 3.5, where x 0 , ρ may be chosen such that B ρ ( x 0 ) w d x > 0 .

Describing, forecasting, and controlling the evolution of a variety of phenomena in physics, chemistry, finance, biology, ecology, medicine, sociology, and industrial activity cannot be done without taking into account nonlinear equations. For what concerns the principal part of the operator, the p-Laplacian arises in the theory of quasi-regular and quasi-conformal mappings, and it provides a mathematical model of non-Newtonian fluids ( 1 < p < 2 represents the pseudoplastic fluids, such as lava, while p > 2 describes the dilating fluids, such as blood) [1]. On the other hand, reaction terms exhibiting singular nonlinearities are important in natural sciences, such as in the study of heat conduction in electrically conducting materials [20] and for chemical heterogeneous catalysts [48]. Also, convective elliptic problems naturally arise from applicative questions, such as optimal stochastic control problems (cf. [26, p. 241]). Other models exploiting singular and convective elliptic problems can be found in the monography [26].

The behavior of equations in which a critical term is perturbed with a lower-order term is studied in many model problems, such as the Yamabe problem, the problem of searching an extremal function for the isoperimetric inequality, as well as the existence of non-minimal solutions of the Yang-Mills equation (see [10] and references therein): this is one of the motivations that inspired the present work.

The aim of this article is to prove the following result.

Theorem 1.1

Suppose ( H f ) –( H w ). Then, there exists Λ > 0 such that, for any λ ( 0 , Λ ) , problem ( P λ ) admits a weak solution in D 0 1 , p ( R N ) L ( R N ) C loc 1 , α ( R N ) , for some α ( 0 , 1 ] .

Problem ( P λ ) exhibits several features:

  • The perturbation f is singular, i.e., it blows up when the solution vanishes;

  • f encompasses also convection terms, i.e., depending on the gradient of the solution;

  • The “dominating” reaction term has critical growth;

  • The setting is the whole R N ;

  • Pointwise decay (at infinity) of the solutions is required.

1.1 Comparison with previous results

The main motivation behind the analysis of ( P λ ) is that it mixes variational problems with double lack of compactness, since the loss of compactness of Sobolev’s embedding occurs due to both the presence of the Sobolev critical exponent and the unboundedness of the domain, with non-variational problems, since convection terms destroy the variational structure. The multi-faced aspect of the problem suggests that it may be of interest to summarize the state of art of elliptic problems exhibiting, either separately or jointly, critical, singular, and convective reaction terms.

The pioneering article by Brezis and Nirenberg [10] for the Laplacian in a bounded domain paved the way for critical problems in the past 30 years. Later, existence and multiplicity of infinitely many solutions were obtained for the p-Laplacian in the critical case by Garcia Azorero and Peral Alonso [23] in bounded domains and by Huang [38] in R N , applying the mountain pass theorem and the theory of Krasnosel’skiǐ genus. More general operators were investigated by several authors [5,6,46]. In all of these articles the concentration compactness principles by Lions and Ben-naoum et al. [7,40] play a crucial role in recovering compactness.

In the same years, Choi et al. [13], Lazer and McKenna [39] gave the decisive boost to the thereafter florid line of research of singular problems. Often, existence of solutions to p-Laplacian singular problems is obtained either by combining variational methods with sub-super-solution and truncation techniques (see, e.g., [29,47]), or by regularizing the singular terms and using a priori estimates to recover compactness (see the appendix of [12]).

The presence of convection terms destroys the variational structure of even more basic problems than ( P λ ). For this reason, methods involving a priori estimates, Liouville-type theorems, and degree arguments [2,28,51] are widely employed in these situations when working on bounded domains; on the contrary, little is known in the entire Euclidean setting, and monotonicity techniques (as comparison and sub-super-solution theorems) are essential ingredients of the proofs [18].

Concerning the interaction of singular and convective nonlinearities, we address the reader to the survey [32] (see also [33] for systems), which contains a rich bibliography on this topic. However, to the best of our knowledge, [21,37] are the only articles involving singular quasilinear elliptic problems in the whole space and with convective terms, regarding equations and systems, respectively.

Finally, about singular and critical reactions, we refer to [27] for the case of bounded domains and [45] for the nonlocal setting; see also [25] for the fractional p-Laplacian. As far as we know, there are no results in unbounded domains. Theorem 1.1 is a first attempt at dealing with critical, convective, and singular elliptic equations in the entire R N . Moreover, up to our knowledge, our result is new even in the non-singular case, also for the Laplacian ( p = 2 ).

1.2 Sketch of the proof

Let us briefly summarize the proof of Theorem 1.1, exposing the main techniques adopted in the article.

First of all, we truncate and freeze the perturbation f , in order to cast the problem into a classical variational framework: indeed, freezing the convection terms (i.e., keeping them fixed) allows us to obtain rid of them, which makes the problem to fall into a variational setting, while truncation guarantees C 1 regularity of the associated energy functional. After truncating and freezing, we obtain the problem

Δ p u = λ a ( x , u ) + u + p * 1 , in R N , ( P ˆ λ )

where

a ( x , s ) w ( x ) f ( max { s , u ̲ λ ( x ) } , v ( x ) ) , ( x , s ) R N × R ,

being u ̲ λ a suitable function (see (3.1)) and v D 0 1 , p ( R N ) fixed.

The central part of this article is devoted to construct a solution u D 0 1 , p ( R N ) to ( P ˆ λ ) by applying the mountain pass theorem to the energy functional J associated with ( P ˆ λ ) (Theorem 3.6). This can be done in three steps:

  1. Detecting, through concentration compactness principles, a particular energy level c ˆ (3.12) under which compactness of J is recovered, i.e., proving that J satisfies the Palais-Smale condition below c ˆ (Lemma 3.3);

  2. Showing that, for small λ ’s, J satisfies the mountain pass geometry, “joining” the origin with a Talenti’s function (Lemma 3.4);

  3. Ensuring that the mountain pass level lies below the “critical” Palais-Smale level c ˆ , provided λ is small enough (Lemma 3.5).

Then, we come back to the original problem. Since the truncation was performed at the level of a sub-solution u ̲ λ (cf. Lemma 2.9 and (3.1)), any solution to ( P ˆ λ ) stays above u ̲ λ (Remark 3.7). It remains to unfreeze the convection terms: this is achieved by using set-valued analysis and fixed point theory. More specifically, the set-valued function S associating with each function v D 0 1 , p ( R N ) the set of solutions to ( P ˆ λ ) having “low” energy (see (4.2)) is compact (Lemma 4.3) and, for small values of λ , lower semi-continuous (Lemma 4.4), so its selection T obtained by minimality (see (4.14)) inherits compactness and continuity; thus, Schauder’s theorem guarantees the existence of a fixed point of T (Theorem 4.5), i.e., a solution to ( P λ ), provided a pointwise decay at infinity is ensured.

In order to conclude, both local C 1 , α regularity and pointwise decay for solutions u to ( P λ ) lying in any energy level below c ˆ are proved (Theorem 5.1). To do this, a global L estimate is ensured via both De Giorgi’s technique and the uniform equi-integrability provided by the concentration compactness principles (cf. Lemma 3.2); then, a quantitative local L gradient estimate guarantees local C 1 , α regularity of the solution, as well as a high global summability on the weighted gradient term w u r 1 , which, in turn, ensures a global L gradient estimate; finally, this information allows a comparison with a radial function that decays at infinity.

Before analyzing more technical aspects, it is worth mentioning that we provide quantitative estimates on the threshold Λ in Theorem 1.1: see (3.26), (3.29), (3.32), and (4.9).

1.3 Technical issues

Now, we discuss some technical details, explicitly pointed out to emphasize some delicate, and somehow innovative, points in the proofs along this study.

First, we observe that the concentration compactness argument, carried out in a general form in Lemma 3.2, is crucial in this setting. Indeed, it is applied four times: (i) to ensure the Palais-Smale condition on some energy levels, as customary when dealing with critical problems (cf. [3,5,23]); (ii) to obtain compactness of the set-valued function S , usually recovered by working in the C 1 topology via Ascoli-Arzelà’s theorem (cf. [34,36,41]; see also [2]); (iii) to guarantee the lower semi-continuity of S , which heavily relies on the compactness of the sub-level sets of energy functional; and (iv) to provide L estimates uniform with respect to the solution, using an equi-uniform integrability information, which is, in general, not available without restrictions on the energy levels (cf., e.g., [11]).

Second, it is worth pointing out that compactness and lower semi-continuity of S require additional work, compared to [34,36,41], and this is due not only to the concentration compactness issues mentioned earlier. About compactness, working in Beppo Levi spaces causes the loss of a.e. convergence of gradient terms ( v n ) with fixed ( v n ) , forcing the use of a monotonicity property, as the ( S + ) property for the p-Laplacian in D 0 1 , p ( R N ) (cf. [42]). Concerning lower semi-continuity, the super-linear growth of the reaction term requires the joint usage of a scaling argument and a fine recursive estimate to obtain suitable energy bounds.

Finally, we spend a few words about regularity and decay of solutions u to ( P λ ). Unlike the existence result, which requires only w u ̲ λ γ L ( p * ) ( R N ) , we need a decay on u ̲ λ to obtain C 1 , α local estimates. Indeed, the decay of u ̲ λ guarantees w u ̲ λ γ L ( R N ) , producing local L gradient estimates, which imply C 1 , α local regularity. The decay of u ̲ λ is a consequence of the decays of the fundamental solution of the p-Laplacian and w ; the latter is also used to refine L bounds of u , deducing global estimates from local ones, and to ensure the pointwise decay of u .

1.4 Structure of this article

In Section 2, we give a few classical definitions and state some basic results, such as the concentration compactness principles, the mountain pass theorem, and a fixed point theorem, together with minor lemmas, which will be useful in the sequel. Section 3 is devoted to the study of a truncated and frozen problem, which leads to an existence result. In Section 4, the unfreezing the convection term is carried out via set-valued analysis. Finally, Section 5 contains the last part of the proof of Theorem 1.1, concerning regularity and decay of solutions.

2 Preliminaries

2.1 Notations

We indicate with B r ( x ) the R N -ball of center x R N and radius r > 0 , omitting x when it is the origin. The symbols B ¯ , B , and B e stand, respectively, for the closure, the boundary, and the exterior of the ball B . Given any A R N , we write χ A to indicate the characteristic function of A . For any N -dimensional Lebesgue measurable set Ω , by Ω , we mean its N -dimensional Lebesgue measure.

Given a real-valued function φ , we indicate its positive (resp., negative) part with φ + max { φ , 0 } (resp., φ max { φ , 0 } ). We abbreviate with { u > v } the set { x R N : u ( x ) > v ( x ) } , and similarly for { u < v } , etc.

We indicate with X * the dual of a Banach space X , while , stand for the duality brackets. Given two Banach spaces X and Y , the continuous embedding of X into Y is indicated by X Y ; if the embedding is compact, we write X c Y . If a sequence ( u n ) strongly converges to u , we write u n u ; if the convergence is in weak sense, we use u n u . The letter S denotes the Sobolev constant; see the next subsection for details.

Let M ( R N , R ) be the space of all finite signed Radon measures. Concerning convergence of measures ( μ n ) M ( R N , R ) , we write μ n * μ and μ n μ to signify tight and weak convergence, respectively (the definitions are given in the next subsection). The symbol δ x indicates the Dirac delta of mass 1 concentrated at x R N .

The letter C denotes a positive constant, which may change its value at each passage; subscripts on C emphasize its dependence from the specified parameters. For the sake of readability, we also write “in R N ” instead of “a.e. in R N .”

2.2 Functional setting

We denote by C c ( R N ) the space of the compactly supported test functions on R N , while C loc 1 , α ( R N ) , being α ( 0 , 1 ] , denotes the space of continuously differentiable functions whose gradient is locally α -Hölder continuous.

Given any measurable set Ω R N and q [ 1 , + ] , L q ( Ω ) stands for the standard Lebesgue space, whose norm will be indicated with L q ( Ω ) , or simply q when Ω = R N . For p ( 1 , N ) , we will also make use of the Beppo Levi space D 0 1 , p ( R N ) , which is the closure of C c ( R N ) with respect to the norm

u D 0 1 , p ( R N ) u p .

Beppo Levi spaces are reflexive, separable Banach spaces; we indicate with D 1 , p ( R N ) the dual of D 0 1 , p ( R N ) . Sobolev’s theorem ensures that D 0 1 , p ( R N ) L p * ( R N ) ; the best constant c in the Sobolev inequality u L p * ( R N ) c u D 0 1 , p ( R N ) is S 1 p , being

S inf u D 0 1 , p ( R N ) \ { 0 } u p p u p * p .

According to Sobolev’s theorem, one has

D 0 1 , p ( R N ) = { u L p * ( R N ) : u L p ( R N ) } .

Incidentally, we recall that D 0 1 , p ( R N ) c L q ( Ω ) for all bounded, measurable sets Ω and all q [ 1 , p * ) (this is a consequence of Rellich-Kondrachov’s theorem; cf. [9, Theorem 9.16]).

A sequence of measures ( μ n ) M ( R N , R ) converges tightly to a measure μ , written as μ n * μ , if

(2.1) R N f d μ n R N f d μ , for all f C b ( R N ) ,

where C b ( R N ) is the space of the bounded, continuous functions on R N . On the other hand, ( μ n ) M ( R N , R ) is said to converge weakly to μ , written as μ n μ , if (2.1) holds for all f C 0 ( R N ) , being C 0 ( R N ) the space of the continuous functions that vanish at infinity. Since C 0 ( R N ) C b ( R N ) , tight convergence implies weak convergence. Moreover, if ( μ n ) M ( R N , R ) is bounded, then (up to sub-sequences) μ n μ for some μ M ( R N , R ) : see [19, Proposition 1.202]. Note that weak convergence is the “natural” convergence in the space M ( R N , R ) , since M ( R N , R ) = ( C 0 ( R N ) ) . It is worth pointing out that tight convergence can be seen as non-concentration at infinity [3,4].

Let ( X , X ) be a Banach space and J be a functional of class C 1 (hereafter indicated as J C 1 ( X ) ). A sequence ( u n ) X is a Palais-Smale sequence of level c R if J ( u n ) c in R and J ( u n ) 0 in X * . If each Palais-Smale sequence of level c admits a strongly convergent sub-sequence, then J is said to satisfy the Palais-Smale condition at level c ; briefly, J satisfies (PS) c .

A poset (i.e., a partially ordered set) ( A , ) is said to be downward directed if for any a , b A , there exists c A such that c a and c b . We recall that, if a is a minimal element of the downward directed poset A , then a = min A : indeed, since A is downward directed, for any b A , there exists c A such that c a and c b , and minimality of a forces c = a , so that c b for all b A , i.e., c = min A .

Let ( X , d X ) and ( Y , d Y ) be two metric spaces. A set-valued function S : X 2 Y is said to be lower semi-continuous if, for any x n x in X and y S ( x ) , there exists ( y n ) Y such that y n y Y and y n S ( x n ) for all n N ; it is said to be compact if, for any bounded K X , the set S ( K ) is relatively compact in Y .

2.3 Some tools

First of all, we recall a simple result concerning weak convergence of the positive part of functions; although it is folklore, we make its proof.

Lemma 2.1

Let 1 < p < N and ( u n ) D 0 1 , p ( R N ) , u D 0 1 , p ( R N ) be such that u n u in D 0 1 , p ( R N ) . Then, ( u n ) + u + in D 0 1 , p ( R N ) .

Proof

Fix any R > 0 . Since D 0 1 , p ( R N ) c L p ( B R ) , we have u n u in L p ( B R ) . Then, up to sub-sequences, u n u in B R , and there exists U L p ( B R ) such that u n U in B R for all n N (see [9, Theorem 4.9]). Thus, Lebesgue’s dominated convergence theorem and the continuity of the real function t t + imply ( u n ) + u + in L p ( B R ) .

We observe that ( u n ) is bounded in D 0 1 , p ( R N ) . Stampacchia’s lemma (cf., e.g., [17, Theorem 4.4]) guarantees that ( v + ) = χ { v > 0 } v for all v D 0 1 , p ( R N ) , and this implies that ( ( u n ) + ) is bounded in D 0 1 , p ( R N ) . By reflexivity, there exists v D 0 1 , p ( R N ) such that ( u n ) + v in D 0 1 , p ( R N ) . Reasoning as above, we infer ( u n ) + v in L p ( B R ) , forcing v = u + . Arbitrariness of R gives ( u n ) + u + in D 0 1 , p ( R N ) .□

Let us introduce two lemmas, which are useful to handle concentration of compactness at points and at infinity, respectively.

Lemma 2.2

(Lions, [40, Lemma I.1]) Let 1 p < N . Suppose ( u n ) D 0 1 , p ( R N ) to be such that u n u in D 0 1 , p ( R N ) , and both u n p μ , u n p * * ν in the sense of measures, for some u D 0 1 , p ( R N ) and μ , ν bounded non-negative measures on R N . Then, there exist some at most countable set A , a family of distinct points ( x j ) j A R N , and two families of numbers ( ν j ) j A , ( μ j ) j A ( 0 , + ) fulfilling

(2.2) ν = u p * + j A ν j δ x j , μ u p + j A μ j δ x j , S ν j p p * μ j , f o r a l l j A .

Note that Lemma 2.2 requires the tight convergence of the measures involving the critical Sobolev exponent, but the proof of this condition reveals to be rather difficult and technical. Thus, Ben-Naoum et al. established a version of Lemma 2.2 known as escape to infinity principle, where the concentration at infinity is enclosed in the parameters ν and μ .

Lemma 2.3

(Ben-Naoum et al. [7, Lemma 3.3]) Let 1 p < N . Suppose that ( u n ) D 0 1 , p ( R N ) is bounded and define

ν lim R + limsup n B R e u n p * d x , μ lim R + limsup n B R e u n p d x .

Then, it holds S ν p p * μ and

limsup n R N u n p * d x = R N d ν + ν , limsup n R N u n p d x = R N d μ + μ ,

where ν and μ are as in Lemma 2.2.

We will use Lemmas 2.22.3 to avoid concentration both at points, i.e., ν j = μ j = 0 for all j A , and at infinity, i.e., ν = μ = 0 .

Remark 2.4

Although not explicitly stated in [40, Lemma I.1], for all j A , one has ν j = ν ( { x j } ) and one can assume μ j = μ ( { x j } ) in Lemma 2.2 (see, e.g., [43, Theorem 2.5]). Indeed, for all ε > 0 , (2.2) implies

ν ( B ε ( x j ) ) = B ε ( x j ) u p * d x + i A ν i δ x i ( B ε ( x j ) ) , for all j A ,

so letting ε 0 produces ν ( { x j } ) = ν j for all j A . On the other hand, it is readily seen that μ μ ( { x j } ) δ x j for all j A . Since { u p } { δ x j : j A } is a set consisting of pairwise mutually singular measures, as well as (2.2) ensures μ u p , one has

μ u p + j A μ ( { x j } ) δ x j .

Using (2.2) again, one has μ ( { x j } ) μ j S ν j p p * . Thus, replacing μ j with μ ( { x j } ) for all j A leaves (2.2) unaltered.

Now, we state the refined versions of two pivotal theorems in nonlinear analysis.

Theorem 2.5

(Ambrosetti, Rabinowitz; cf. [44, Theorem 5.40]) Let ( X , X ) be a Banach space and J C 1 ( X ) . Let u 0 , u 1 X , ρ > 0 such that the “mountain pass geometry” is fulfilled, i.e.,

max { J ( u 0 ) , J ( u 1 ) } < inf B ρ ( u 0 ) J b a n d u 1 u 0 X > ρ .

Set

Φ { ϕ C 0 ( [ 0 , 1 ] ; X ) : ϕ ( 0 ) = u 0 , ϕ ( 1 ) = u 1 } , c M inf ϕ Φ sup t [ 0 , 1 ] J ( ϕ ( t ) ) .

If J satisfies (PS) c M , then c M b and there exists u X such that both J ( u ) = c M and J ( u ) = 0 . Moreover, if c M = b , then u can be taken on B ρ ( u 0 ) .

Theorem 2.6

(Schauder; cf. [30, Theorem 6.3.2 p. 119]) Let K be a non-empty bounded convex subset of a normed linear space E, and let T : K K be a compact map. Then, T has a fixed point.

We will need also the following result about boundedness of sequences defined by recursion.

Lemma 2.7

Let ( b k ) k = 0 [ 0 , + ) satisfy, for some c > 0 and K , α > 1 , the recursion

b k c + K b k 1 α , f o r a l l k N .

If

(2.3) K b 0 α 1 1 2 a n d K c α 1 < 2 α ,

then ( b k ) is bounded.

Proof

By iteration, we obtain

b k c + K b k 1 α c + K ( c + K b k 2 α ) α c + 2 α K ( c α + K α b k 2 α 2 ) c + 2 α K c α + 2 α K 1 + α ( c + K b k 3 α ) α 2 c + 2 α K c α + 2 α + α 2 K 1 + α ( c α 2 + K α 2 b k 3 α 3 ) c + j = 1 k 1 2 i = 1 j α i K i = 0 j 1 α i c α j + 2 i = 1 k 1 α i K i = 0 k 1 α i b 0 α k = j = 0 k 1 2 α j + 1 α α 1 K α j 1 α 1 c α j + 2 α k α α 1 K α k 1 α 1 b 0 α k j = 0 k 1 ( 2 α α 1 K 1 α 1 c ) α j + ( 2 1 α 1 K 1 α 1 b 0 ) α k .

The conclusion then follows by (2.3) observing that, for all k N ,

b k j = 0 ( 2 α α 1 K 1 α 1 c ) α j + 1 < + ,

since j = 0 q α j is convergent for all q ( 0 , 1 ) .□

We conclude this section by proving the existence of a sub-solution to ( P λ ) (Remark 3.7). We permit a straightforward adaptation of the weak comparison principle (cf. [49, Theorem 3.4.1]) to the setting of Beppo Levi spaces.

Lemma 2.8

Let u , v D 0 1 , p ( R N ) satisfy

(2.4) Δ p u , φ Δ p v , φ ,

for all φ D 0 1 , p ( R N ) such that φ 0 in R N and φ 0 on { u v } . Then, u v in R N .

Proof

Testing (2.4) with ( u v ) + D 0 1 , p ( R N ) , besides recalling Stampacchia’s lemma (cf., e.g., [17, Theorem 4.4]), yields

{ u > v } ( u p 2 u v p 2 v ) ( u v ) d x 0 .

Hence, [14, Lemma 2.1] entails ( u v ) + = 0 in R N , which implies ( u v ) + = 0 in R N , since ( u v ) + D 0 1 , p ( R N ) .□

Lemma 2.9

Let w satisfy ( H w ) and let γ ( 0 , 1 ) . Then, there exists a unique u C loc 1 , α ( R N ) solution to

(2.5) Δ p u = w ( x ) u γ , i n R N , u > 0 , i n R N , u ( x ) 0 , a s x + .

Moreover, w u γ L 1 ( R N ) L ( R N ) .

Proof

For all n N , consider the regularized problems

Δ p u n = w ( x ) ( u n ) + + 1 n γ , in R N . P ̲ n

Fix any n N . Direct methods of calculus of variations (see [52, Theorem I.1.2]) ensure that there exists u n D 0 1 , p ( R N ) solution to ( P ̲ n ). Note that

0 w ( u n ) + + 1 n γ n γ w L ( R N ) ,

so u n C loc 1 , α ( R N ) according to nonlinear regularity theory [15, Corollary p. 830]. Moreover, by the strong maximum principle (cfr. [49, Theorem 1.1.1]), u n > 0 in R N .

Testing ( P ̲ n ) with u n , besides using Hölder’s and Sobolev’s inequalities, yields

u n p p = R N w u n + 1 n γ u n d x R N w u n 1 γ d x w ζ u n p * 1 γ S 1 γ p w ζ u n p 1 γ ,

being ζ > 1 such that 1 ζ + 1 γ p * = 1 . We deduce u n p ( S 1 γ p w ζ ) 1 p 1 + γ , so that ( u n ) is bounded in D 0 1 , p ( R N ) . By reflexivity, u n u in D 0 1 , p ( R N ) for some u D 0 1 , p ( R N ) , up to sub-sequences.

Observing that u n + 1 n > u n + 1 + 1 n + 1 on { u n > u n + 1 } , we obtain the weak inequality

Δ p u n = u n + 1 n γ u n + 1 + 1 n + 1 γ = Δ p u n + 1 , on { u n > u n + 1 } .

According to Lemma 2.8, it turns out that u n u n + 1 in R N . Thus, we can define a measurable function u ˜ such that u n u ˜ in R N .

We show that u = u ˜ in R N . For all k N , D 0 1 , p ( R N ) c L p ( B k ) , so u n u in L p ( B k ) and u n u in B k , up to sub-sequences. A diagonal argument ensures that u n u in R N , whence u = u ˜ in R N (see, e.g., [21, p. 3044] for details).

Now, we prove that we can pass to the limit in the weak formulation of ( P ̲ n ). Taking any φ D 0 1 , p ( R N ) , we have

(2.6) lim n R N u n p 2 u n φ d x = R N u p 2 u φ d x ,

according to [21, Proposition 1] applied to the sequence ( u n p 2 u n ) L p ( R N ) . On the other hand, splitting φ = φ + φ , Beppo Levi’s monotone convergence theorem guarantees

lim n R N w u n + 1 n γ φ + d x = R N w u γ φ + d x .

In the same way,

lim n R N w u n + 1 n γ φ d x = R N w u γ φ d x ,

producing

(2.7) lim n R N w u n + 1 n γ φ d x = R N w u γ φ d x .

Hence, (2.6)–(2.7) ensure that u solves (2.5), once we prove that u 0 as x + . To do this, note that Δ p u 0 in B R e , where R > 0 stems from (1.1). Given σ > 0 , set Φ σ ( x ) σ x p N p 1 and observe that Δ p Φ σ = 0 in B R e . According to the weak comparison principle in exterior domains (see, e.g., [22, Proposition A.12]), there exists σ > 0 small enough such that u Φ σ in B R e . This, together with ( H w ), implies that u solves

Δ p u c 3 σ γ x γ N p p 1 l , in B R e .

Choosing M > u ( R ) large enough, [22, Lemma 4.2] ensures the existence of Ψ D 0 1 , p ( R N ) solving

Δ p Ψ = c 3 σ γ x γ N p p 1 l , in B R e , Ψ = M , on B R e , Ψ ( x ) 0 , as x + .

Thus, applying the aforementioned weak comparison principle to u and Ψ , we infer u Ψ in R N ; in particular, u ( x ) 0 as x + .

Recalling that u u 1 in R N and inf B r u 1 > 0 for all r > 0 , we deduce w u γ L loc ( R N ) , implying that u C loc 1 , α ( R N ) by regularity theory (see [15, Corollary p. 830]). On the other hand, exploiting the fact that w u γ c 3 σ γ x γ N p p 1 l in B R e and l > N + γ N p p 1 , we infer w u γ L 1 ( B R e ) L ( B R e ) . Summarizing, w u γ L 1 ( R N ) L ( R N ) .

Uniqueness of u can be proved by comparison as follows. If u 1 , u 2 D 0 1 , p ( R N ) are two solutions of (2.5) then Lemma 2.8 yields u 1 u 2 in R N , since w u 1 γ < w u 2 γ on { u 1 > u 2 } . Reversing the roles of u 1 and u 2 leads to u 2 u 1 in R N , whence u 1 = u 2 in R N .□

3 Truncated, frozen problem

Hereafter, we will tacitly suppose ( H f ) –( H w ). Let u ̲ λ C loc 1 , α ( R N ) be the solution to

Δ p u = λ c 1 w ( x ) u γ , in R N , u > 0 , in R N , u ( x ) 0 , as x + ,

whose existence and uniqueness are guaranteed by Lemma 2.9, replacing w with λ c 1 w . According to the scaling properties of the p-Laplacian and the singularity u γ , we have

(3.1) u ̲ λ = λ 1 p 1 + γ u ̲ ,

where u ̲ solves (2.5) with c 1 w in place of w . For any fixed v D 0 1 , p ( R N ) , set

(3.2) a ( x , s ) w ( x ) f ( max { s , u ̲ λ ( x ) } , v ( x ) ) , ( x , s ) R N × R ,

and consider the “truncated and frozen” problem

(Pˆλ) Δ p u = λ a ( x , u ) + u + p * 1 , in R N .

Problem ( P ˆ λ ) has variational structure: its energy functional is

(3.3) J : D 0 1 , p ( R N ) R , J ( u ) 1 p u p p λ R N A ( x , u ) d x 1 p * u + p * p * u D 0 1 , p ( R N ) ,

being A ( x , s ) 0 s a ( x , t ) d t . Analogously, we define a n , A n , J n , replacing v with v n D 0 1 , p ( R N ) .

By ( H f ) , we deduce the following estimates, valid for all ( x , s ) R N × R :

(3.4) c 1 w ( x ) max { s , u ̲ λ ( x ) } γ a ( x , s ) c 2 w ( x ) ( max { s , u ̲ λ ( x ) } γ + v ( x ) r 1 ) ,

(3.5) A ( x , s ) c 2 w ( x ) ( u ̲ λ ( x ) γ + v ( x ) r 1 ) s , A ( x , s ) c 2 1 γ w ( x ) s 1 γ + c 2 w ( x ) ( u ̲ λ ( x ) γ + v ( x ) r 1 ) s .

In the sequel, we will make use of ζ , θ ( 1 , + ) defined as

1 ζ + 1 γ p * = 1 and 1 θ + r 1 p + 1 p * = 1 .

According to (3.5), it is readily seen that J is well defined and of class C 1 , with

J ( u ) , φ = R N u p 2 u φ d x λ R N a ( x , u ) φ d x R N u + p * 1 φ d x , u , φ D 0 1 , p ( R N ) .

First, we prove two general results concerning, in particular, Palais-Smale sequences associated with the functionals J n : Lemma 3.1 provides an energy estimate, while Lemma 3.2 detects a “critical” energy level under which compactness is recovered.

Lemma 3.1

(Energy estimate) Suppose λ ( 0 , 1 ] . Let c R , L > 0 , and ( u n ) , ( v n ) D 0 1 , p ( R N ) such that

(3.6) limsup n J n ( u n ) c , lim n J n ( u n ) = 0 , i n D 1 , p ( R N ) , limsup n v n p L .

Then, there exists C ˆ = C ˆ ( p , N , w , γ , r , c 1 , c 2 ) > 0 such that

limsup n u n p p 2 N C ˆ λ p p 1 + γ ( L p ( r 1 ) + 1 ) + c .

Proof

According to (3.6), we have

(3.7) c + o ( 1 ) ( 1 + u n p ) J n ( u n ) 1 p * J n ( u n ) , u n = 1 N u n p p λ R N A n ( x , u n ) d x + λ p * R N a n ( x , u n ) u n d x .

By means of (3.4)–(3.5) and (3.1), as well as Hölder’s and Sobolev’s inequalities, besides taking into account that λ ( 0 , 1 ) , we obtain

(3.8) R N A n ( x , u n ) d x c 2 1 γ R N w u n 1 γ d x + c 2 R N w ( u ̲ λ γ + v n r 1 ) u n d x c 2 1 γ w ζ u n p * 1 γ + c 2 ( λ γ p 1 + γ w u ̲ γ ( p * ) + w θ v n p r 1 ) u n p * c 2 1 γ S 1 γ p w ζ u n p 1 γ + c 2 λ γ p 1 + γ S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 + o ( 1 ) ) u n p

and

(3.9) R N a n ( x , u n ) u n d x R N a n ( x , u n ) u n d x c 2 R N w ( u ̲ λ γ + v n r 1 ) u n d x c 2 λ γ p 1 + γ S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 + o ( 1 ) ) u n p .

Inserting (3.8)–(3.9) into (3.7) produces

c + o ( 1 ) ( 1 + u n p ) 1 N u n p p λ c 2 1 γ S 1 γ p w ζ u n p 1 γ λ p 1 p 1 + γ c 2 S 1 p 1 + 1 p * ( w u ̲ γ ( p * ) + w θ L r 1 + o ( 1 ) ) u n p .

Re-absorbing the terms u n p on the right via Peter-Paul’s inequality[1], we obtain

(3.10) 1 N ε u n p p C ε λ p p 1 + γ ( L p ( r 1 ) + 1 ) + c + o ( 1 ) ,

for a suitable C ε = C ε ( ε , p , N , w , γ , r , c 1 , c 2 ) (since S is a function of only p , N and u ̲ depend uniquely on p , w , γ , and c 1 ). Choosing ε = 1 2 N and setting C ˆ C ε , (3.10) become

(3.11) 1 2 N u n p p C ˆ λ p p 1 + γ ( L p ( r 1 ) + 1 ) + c + o ( 1 ) .

Passing to limsup for n concludes the proof.□

Lemma 3.2

(Concentration compactness) Assume the hypotheses of Lemma 3.1. If

(3.12) c < S N p N C ˆ λ p p 1 + γ ( L p ( r 1 ) + 1 ) c ˆ ,

then there exists u D 0 1 , p ( R N ) such that, up to sub-sequences, u n u in D 0 1 , p ( R N ) and

(3.13) ( u n ) + u + , i n L p * ( R N ) .

In particular, ( ( u n ) + ) is uniformly equi-integrable in L p * ( R N ) , i.e.,

(3.14) Ω ( u n ) + p * d x 0 a s Ω 0 , u n i f o r m l y i n n N .

Proof

By Lemma 3.1, we deduce that ( u n ) is bounded in D 0 1 , p ( R N ) . Hence, there exists u D 0 1 , p ( R N ) such that, up to sub-sequences, u n u in D 0 1 , p ( R N ) , which implies ( u n ) + u + in D 0 1 , p ( R N ) by Lemma 2.1. In particular, ( u n ) + u + in L p ( R N ) , ensuring that the sequence of measures ( ( u n ) + p ) is bounded. Thus, ( u n ) + p μ for some bounded measure μ ; analogously, ( u n ) + p * ν for an opportune bounded measure ν . According to Lemmas 2.22.3, applied to ( ( u n ) + ) in place of ( u n ) , there exist some at most countable set A , a family of points ( x j ) j A R N , and two families of numbers ( μ j ) j A , ( ν j ) j A ( 0 , + ) satisfying

(3.15) ν = u + p * + j A ν j δ x j , μ u + p + j A μ j δ x j , limsup n R N ( u n ) + p * d x = R N d ν + ν , limsup n R N ( u n ) + p d x = R N d μ + μ ,

and

(3.16) S ν j p p * μ j , for all j A , S ν p p * μ ,

being

ν lim R + limsup n B R e ( u n ) + p * d x and μ lim R limsup n B R e ( u n ) + p d x .

We claim that A = . By contradiction, let j A and ψ C c ( R N ) be a standard cut-off function fulfilling ψ 1 in B ¯ 1 2 , ψ 0 in B 1 e , and 0 ψ 1 in R N . For each ε ( 0 , 1 ) , set

ψ ε ( x ) ψ x x j ε .

By hypothesis, we have J n ( u n ) , ( u n ) + ψ ε 0 , i.e.,

(3.17) R N ( u n ) + p ψ ε d x + R N ( u n ) + u n p 2 u n ψ ε d x = λ R N a n ( x , u n ) ( u n ) + ψ ε d x + R N ( u n ) + p * ψ ε d x + o ( 1 ) .

Since D 0 1 , p ( R N ) c L p ( B ε ( x j ) ) , we have (up to sub-sequences) u n u both in L p ( B ε ( x j ) ) and in R N . Reasoning as for (3.9), besides recalling that ( u n ) is bounded in L p ( R N ) , one has

(3.18) lim ε 0 lim n R N a n ( x , u n ) ( u n ) + ψ ε d x c 2 lim ε 0 lim n B ε ( x j ) w ( u ̲ λ γ + v n r 1 ) u n d x c 2 λ γ p 1 + γ S 1 p ( sup n N u n p ) lim ε 0 ( w u ̲ γ L ( p * ) ( B ε ( x j ) ) + w L θ ( B ε ( x j ) ) L r 1 ) = 0 .

Since ψ ε is bounded and compactly supported in B ε ( x j ) , we deduce u n ψ ε u ψ ε in L p ( R N ) as n . By Hölder’s inequality and a change of variable, we infer

(3.19) lim ε 0 lim n R N u n u n p 2 u n ψ ε d x lim ε 0 lim n u n p p 1 u n ψ ε p ( sup n N u n p ) p 1 lim ε 0 u ψ ε p ( sup n N u n p ) p 1 ψ N lim ε 0 u L p * ( B ε ( x j ) ) = 0 .

Passing to the limit in (3.17) via (3.18)–(3.19), we obtain

lim ε 0 lim n R N ( u n ) + p ψ ε d x = lim ε 0 lim n R N ( u n ) + p * ψ ε d x .

Recalling Remark 2.4, we obtain

(3.20) μ j = ν j .

Combining (3.20) with (3.16) entails S ν j p p * 1 1 , whence

(3.21) μ j = ν j S N p .

Now, using (3.21) and arguing as in (3.11), we have

(3.22) c + o ( 1 ) J n ( u n ) 1 p * J n ( u n ) , u n 1 N u n p p + λ 1 p * R N a n ( x , u n ) u n d x R N A n ( x , u n ) d x S N p N + 1 N u p p + λ 1 p * R N a n ( x , u ) u d x R N A n ( x , u ) d x + o ( 1 ) S N p N + 1 2 N u p p C ˆ λ p p 1 + γ ( L p ( r 1 ) + 1 ) + o ( 1 ) S N p N C ˆ λ p p 1 + γ ( L p ( r 1 ) + 1 ) + o ( 1 ) ,

contradicting (3.12) as n . This forces A = .

A similar argument proves that concentration cannot occur at infinity, i.e., ν = μ = 0 : indeed, using a cut-off function ψ R C ( R N ) such that ψ R 0 in B ¯ R , ψ R 1 in B 2 R e , and 0 ψ R 1 in R N , one arrives at ν = μ , and then, the conclusion follows as in (3.22). According to (3.15), besides A = and ν = 0 , we obtain

limsup n R N ( u n ) + p * d x = R N u + p * d x ,

i.e., (3.13), by uniform convexity (see [9, Proposition 3.32]); in turn, (3.13) forces (3.14) by Vitali’s convergence theorem (see, e.g., [8, Corollary 4.5.5]).□

Problem ( P ˆ λ ) exhibits double lack of compactness, due to the setting R N and the presence of a reaction term with critical growth. The aim of the next lemma is to recover compactness on the energy levels that lie under the critical level c ˆ defined in (3.12).

Lemma 3.3

(Palais-Smale condition) Let λ ( 0 , 1 ] , L > 0 , and v D 0 1 , p ( R N ) be such that v p L . Then, J satisfies the ( PS ) c condition for all c R fulfilling (3.12).

Proof

Take any c R as in (3.12) and consider an arbitrary (PS) c sequence ( u n ) associated with the functional J . Applying Lemma 3.2 with v n v and J n J entails u n u in D 0 1 , p ( R N ) and ( u n ) + u + in L p * ( R N ) . Let us evaluate

(3.23) J ( u n ) , u n u = R N u n p 2 u n ( u n u ) d x λ R N a ( x , u n ) ( u n u ) d x R N ( u n ) + p * 1 ( u n u ) d x .

Since D 0 1 , p ( R N ) L p * ( R N ) , we have u n u in L p * ( R N ) and u n u in R N , up to sub-sequences (see, e.g., [21, p.3044]). Thus, observing that (3.13) forces ( u n ) + p * 1 u + p * 1 in L ( p * ) ( R N ) , we obtain

(3.24) lim n R N ( u n ) + p * 1 ( u n u ) d x = 0 .

Reasoning as for (3.9), one has

w ( u ̲ λ γ + v r 1 ) ( p * ) λ γ p 1 + γ w u ̲ γ ( p * ) + w θ L r 1 < + ,

so the linear functional ψ R N w ( u ̲ λ γ + v r 1 ) ψ d x is continuous in L p * ( R N ) . Moreover, [21, Proposition 1] guarantees that u n u 0 in L p * ( R N ) . Accordingly, ( H f ) ensures

(3.25) lim n R N a ( x , u n ) ( u n u ) d x c 2 lim n w ( u ̲ λ γ + v r 1 ) u n u d x = 0 .

Using (3.24)–(3.25) and recalling that J ( u n ) , u n u 0 , due to the fact that ( u n ) is a (PS) c sequence, by (3.23) we conclude

lim n Δ p u n , u n u = lim n R N u n p 2 u n ( u n u ) d x = 0 .

Then, the ( S + ) property of ( Δ p , D 0 1 , p ( R N ) ) (see [42, Proposition 2.2]) yields u n u in D 0 1 , p ( R N ) .□

The next two lemmas are devoted to verify the mountain pass geometry for the functional J and ensure the mountain pass level c M (Theorem 2.5) lies below the critical Palais-Smale level c ˆ (3.12), provided λ is small enough.

Lemma 3.4

(Mountain pass geometry) Let L > 0 and v D 0 1 , p ( R N ) be such that v p L . Then, there exists Λ 1 ( 0 , 1 ) such that, for every λ ( 0 , Λ 1 ) , the functional J satisfies the mountain pass geometry. More precisely, there exists C ˜ = C ˜ ( p , N , w , γ , r , c 1 , c 2 ) > 1 such that, for all λ satisfying

(3.26) 0 < λ < Λ 1 S N p C ˜ N ( S N p 2 + 1 ) ( 1 + L r 1 ) p 1 + γ p 1 ,

one has

J ( u ˆ ) < J ( 0 ) = 0 < inf B ρ J a n d u ˆ p > ρ , b e i n g ρ S N p 2 ,

for any u ˆ D 0 1 , p ( R N ) such that u ˆ + 0 and u ˆ p is sufficiently large.

Proof

Fix C ˜ = C ˜ ( p , N , w , γ , r , c 1 , c 2 ) > 1 such that

c 2 1 γ S 1 γ p w ζ + c 2 S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 ) C ˜ ( 1 + L r 1 ) .

Let λ fulfill (3.26) and pick any t > 0 . Reasoning as in (3.8), besides recalling the choice of C ˜ , we obtain

inf B t J inf u B t 1 p u p p λ c 2 1 γ R N w u 1 γ d x λ c 2 R N w ( u ̲ λ γ + v r 1 ) u d x 1 p * u p * p * inf u B t 1 p u p p λ c 2 1 γ S 1 γ p w ζ u p 1 γ c 2 λ p 1 p 1 + γ S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 ) u p 1 p * S p * p u p p * = 1 p t p λ c 2 1 γ S 1 γ p w ζ t 1 γ c 2 λ p 1 p 1 + γ S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 ) t 1 p * S p * p t p * 1 p t p λ c 2 1 γ S 1 γ p w ζ ( t + 1 ) c 2 λ p 1 p 1 + γ S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 ) ( t + 1 ) 1 p * S p * p t p * 1 p t p λ p 1 p 1 + γ ( t + 1 ) c 2 1 γ S 1 γ p w ζ + c 2 S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 ) 1 p * S p * p t p * 1 p t p C ˜ λ p 1 p 1 + γ ( 1 + L r 1 ) ( t + 1 ) 1 p * S p * p t p * ,

since u p = t whenever u B t . Let us consider the real-valued function g : ( 0 , + ) R defined as

g ( t ) 1 p t p ε ( t + 1 ) 1 p * S p * p t p * ,

where ε C ˜ λ p 1 p 1 + γ ( 1 + L r 1 ) . Condition (3.26) forces ε < S N p N ( S N p 2 + 1 ) , so that

g ( S N p 2 ) = S N p N ε ( S N p 2 + 1 ) > 0 .

Setting ρ S N p 2 , we obtain

inf B ρ J g ( ρ ) > 0 .

Given any u D 0 1 , p ( R N ) such that u + 0 , we have J ( t u ) as t + : indeed, according to (3.5) and the fact that u + p * > 0 ,

limsup t + J ( t u ) lim t + t p p u p p + c 2 λ t R N w ( u ̲ λ γ + v r 1 ) u d x t p * p * u + p * p * = .

Hence, setting u ˆ t u , we have J ( u ˆ ) < 0 < inf B ρ J and u ˆ p > ρ , provided t is sufficiently large.□

Lemma 3.5

Assume the hypotheses of Lemma 3.4. Then, there exists Λ 2 ( 0 , 1 ) such that for all λ ( 0 , Λ 2 ) , one has

inf ϕ Φ sup t [ 0 , 1 ] J ( ϕ ( t ) ) < c < c ˆ , Φ { ϕ C 0 ( [ 0 , 1 ] ; X ) : ϕ ( 0 ) = 0 , ϕ ( 1 ) = u ˆ } ,

for an opportune c = c ( λ , p , N , w , γ , c 1 ) > 0 , where c ˆ is defined in (3.12) and u ˆ is the Talenti function

u ˆ ( x ) = N 1 p N p p 1 1 + x p N p p .

Proof

First, we note that u ˆ p p = u ˆ p * p * = S N p (see [50] for details). Next, we observe that the path ϕ ( u ) t u ˆ , t [ 0 , 1 ] , belongs to Φ , so

inf ϕ Φ sup t [ 0 , 1 ] J ( ϕ ( t ) ) sup t [ 0 , 1 ] J ( t u ˆ ) sup t [ 0 , + ) J ( t u ˆ ) .

Accordingly, let us compute the maximizer t ¯ of the function t J ( t u ˆ ) , being t 0 .

0 = d d t ( J ( t u ˆ ) ) t = t ¯ = J ( t ¯ u ˆ ) , u ˆ = t ¯ p 1 u ˆ p p λ R N a ( x , t ¯ u ˆ ) u ˆ d x t ¯ p * 1 u ˆ p * p * ,

whence

(3.27) t ¯ p * 1 u ˆ p * p * = t ¯ p 1 u ˆ p p λ R N a ( x , t ¯ u ˆ ) u ˆ d x .

From (3.27), we deduce

t ¯ p * 1 u ˆ p * p * t ¯ p 1 u ˆ p p = t ¯ p 1 u ˆ p * p * ,

forcing t ¯ [ 0 , 1 ] .

Fix any Λ 2 ( 0 , 1 ) and define

ϒ 1 λ ( 0 , Λ 2 ) : t ¯ 1 2 , 1 , ϒ 2 λ ( 0 , Λ 2 ) : t ¯ 0 , 1 2 .

Suppose λ ϒ 1 . Exploiting the monotonicity of A ( x , ) and

max t ( 0 , + ) t p p t p * p * = 1 N ,

we obtain

(3.28) J ( t ¯ u ˆ ) = t ¯ p p u ˆ p p λ R N A ( x , t ¯ u ˆ ) d x t ¯ p * p * u ˆ p * p * = t ¯ p p t ¯ p * p * u ˆ p p λ R N A ( x , t ¯ u ˆ ) d x u ˆ p p N λ R N A x , u ˆ 2 d x .

Let m inf B ϱ ( x 0 ) u ˆ > 0 , being x 0 , ϱ as in (1.2). Imposing

(3.29) Λ 2 m 4 u ̲ p 1 + γ ,

one has u ̲ λ Λ 2 1 p 1 + γ u ̲ m 4 . Accordingly, by (3.4) and (1.2),

R N A x , u ˆ 2 d x { u ˆ 2 > u ̲ λ } u ̲ λ u ˆ 2 a ( x , t ) d t d x c 1 { u ˆ 2 > u ̲ λ } u ̲ λ u ˆ 2 w t γ d t d x = c 1 1 γ { u ˆ 2 > u ̲ λ } w ( x ) u ˆ 2 1 γ u ̲ λ 1 γ d x c 1 1 γ B ϱ ( x 0 ) w ( x ) u ˆ 2 1 γ u ̲ λ 1 γ d x c 1 1 γ m 2 1 γ m 4 1 γ B ϱ ( x 0 ) w ( x ) d x c 1 1 γ m 2 1 γ m 4 1 γ ω B ϱ 2 C ˇ ,

since B ϱ ( x 0 ) { u ˆ 2 > u ̲ λ } . Incidentally, note that C ˇ depends only on p , N , w , γ , and c 1 . From (3.28), we deduce

(3.30) J ( t ¯ u ˆ ) S N p N 2 λ C ˇ .

Now, assume λ ϒ 2 . Setting

c ˇ max t 0 , 1 2 t p p t p * p * < 1 N ,

we deduce

(3.31) J ( t ¯ u ˆ ) = t ¯ p p u ˆ p p λ R N A ( x , t ¯ u ˆ ) d x t ¯ p * p * u ˆ p * p * t ¯ p p t ¯ p * p * u ˆ p p c ˇ S N p .

Recalling that

c ˆ = S N p N λ p p 1 + γ C ˆ ( 1 + L p ( r 1 ) )

and noting that p p 1 + γ > 1 , we can impose the additional bound

(3.32) Λ 2 min 1 N c ˇ N C ˇ S N p , C ˇ C ( 1 + L p ( r 1 ) ) ˆ p 1 + γ 1 γ ,

so that

J ( t ¯ u ˆ ) max c ˇ S N p , S N p N 2 λ C ˇ < S N p N λ C ˇ < c ˆ

by (3.30) and (3.31). The proof is concluded by choosing c = S N p N λ C ˇ .□

Now, we are ready to prove the existence of solutions to the truncated and frozen problem ( P ˆ λ ).

Theorem 3.6

Let L > 0 and v D 0 1 , p ( R N ) be such that v p L . Suppose λ ( 0 , Λ ) with Λ min { Λ 1 , Λ 2 } , being Λ 1 and Λ 2 defined in Lemmas 3.4and 3.5, respectively. Then, there exists u D 0 1 , p ( R N ) solution to ( P ˆ λ ).

Proof

By virtue of Lemmas 3.33.5, the hypotheses of the mountain pass theorem (Theorem 2.5) are fulfilled: hence, there exists u D 0 1 , p ( R N ) solution to ( P ˆ λ ).□

Remark 3.7

Any solution u to either ( P ˆ λ ) or ( P λ ) satisfies u u ̲ λ , being u ̲ λ defined in (3.1). Indeed, if u solves ( P ˆ λ ), then it satisfies (in weak sense)

Δ p u λ a ( , u ) = λ w f ( u ̲ λ , v ) λ c 1 w u ̲ λ γ = Δ p u ̲ λ , on { u < u ̲ λ } ,

because of (3.2) and ( H f ) . Thus, Lemma 2.8 yields u u ̲ λ in R N . A similar argument holds for solutions to ( P λ ), after noting that they are positive by definition.

4 Unfreezing the convection term

Set

(4.1) L 2 S N p .

Let λ ( 0 , Λ ) with Λ = min { Λ 1 , Λ 2 , Λ 3 } , where Λ 1 and Λ 2 stem from Lemmas 3.4 (cf. (3.26)) and 3.5 (cf. (3.29) and (3.32)), while Λ 3 will be determined in such a way that (4.9) holds true.

Consider the D 0 1 , p ( R N ) -ball { u D 0 1 , p ( R N ) : u p < L } . Let S : be defined as

(4.2) S ( v ) { u D 0 1 , p ( R N ) : u solves ( P ˆ λ ) and satisfies  J ( u ) < c } ,

where c ( 0 , c ˆ ) stems from Lemma 3.5. We explicitly note that S depends on λ ; anyway, for the sake of simplicity, we omit this dependence.

Lemma 4.1

The set-valued function S is well defined, i.e., S ( ) .

Proof

Take any v and u S ( v ) . Applying Lemma 3.1 with u n u , v n v , and J n J , after observing that J ( u ) < c < c ˆ and J ( u ) = 0 by definition of S , we obtain

u p p < 2 N C ˆ λ p p 1 + γ ( L p ( r 1 ) + 1 ) + c ˆ .

The conclusion then follows by recalling (3.12).□

Lemma 4.2

For any v , the set S ( v ) is non-empty and admits minimum.

Proof

Fix any v . The fact that S ( v ) is guaranteed by Theorem 3.6.

Now, we prove that S ( v ) is downward directed. Let u 1 , u 2 S ( v ) and set u ¯ min { u 1 , u 2 } . Consider the truncation T : D 0 1 , p ( R N ) D 0 1 , p ( R N ) , T ( u ) ( x ) = τ ( x , u ( x ) ) , being τ : R N × R R defined as

τ ( x , t ) = u ̲ λ ( x ) , if t < u ̲ λ ( x ) , t , if u ̲ λ ( x ) t u ¯ ( x ) , u ¯ ( x ) , if t > u ¯ ( x ) .

We claim that there exists a solution u ˇ D 0 1 , p ( R N ) to

(4.3) Δ p u = λ a ( x , T ( u ) ) + ( T ( u ) ) p * 1 , in R N

satisfying J ( u ˇ ) < c ˆ .

The energy functional associated with (4.3) is

J ˆ ( u ) = 1 p u p p R N B ˆ ( x , u ) d x ,

where

B ˆ ( x , s ) 0 s b ˆ ( x , t ) d t , b ˆ ( x , t ) λ a ( x , τ ( x , t ) ) + τ ( x , t ) p * 1 .

From (3.4), (3.1), and λ ( 0 , 1 ) , we estimate

b ˆ ( x , t ) c 2 λ w ( x ) ( τ ( x , t ) γ + v ( x ) r 1 ) + τ ( x , t ) p * 1 c 2 λ w ( x ) ( u ̲ λ ( x ) γ + v ( x ) r 1 ) + τ ( x , t ) p * 1 c 2 λ p 1 p 1 + γ w ( x ) ( u ̲ ( x ) γ + v ( x ) r 1 ) + u ¯ ( x ) p * 1 h ( x ) ,

so h L ( p * ) ( R N ) . Hence, J ˆ is coercive: indeed,

J ˆ ( u ) 1 p u p p R N h ( x ) u d x 1 p u p p h ( p * ) u p * 1 p u p p S 1 p h ( p * ) u p .

Moreover, it is readily seen that J ˆ is weakly sequentially lower semi-continuous. Thus, applying the direct methods of calculus of variations (see [52, Theorem I.1.2]), there exists u ˇ D 0 1 , p ( R N ) such that J ˆ ( u ˇ ) = min D 0 1 , p ( R N ) J ˆ . In particular, J ˆ ( u ˇ ) J ˆ ( 0 ) = 0 .

Reasoning as in the proof of [31, Lemma 2.5.4] (see also [36, Lemma 3.4]), the minimum of two super-solutions to ( P ˆ λ ) is a super-solution to ( P ˆ λ ); in particular, u ¯ is a super-solution to ( P ˆ λ ). Since u ̲ λ and u ¯ are, respectively, sub- and super-solution to ( P ˆ λ ), Lemma 2.8 ensures u ̲ λ u ˇ u ¯ in R N . Accordingly, u ˇ solves ( P ˆ λ ) and J ˆ ( u ˇ ) = J ( u ˇ ) , so that J ( u ˇ ) 0 < c . The claim is proved. In addition, we obtained u ˇ S ( v ) .

By arbitrariness of u 1 and u 2 , the set S ( v ) is downward directed. Arguing as in [31, Theorem 2.5.7] (see also [36, Lemma 3.14]), we conclude that S ( v ) admits minimum.□

Lemma 4.3

The set-valued function S is compact.

Proof

Let ( v n ) be a (bounded) sequence in . For any n N , pick u n S ( v n ) . Our aim is to prove that u n u in D 0 1 , p ( R N ) for some u D 0 1 , p ( R N ) .

Remark 3.7 ensures u n 0 in R N for all n N , so Lemma 3.2 produces u D 0 1 , p ( R N ) such that u n u in D 0 1 , p ( R N ) and u n u in L p * ( R N ) . Note that, for all n N ,

(4.4) 0 = J n ( u n ) , u n u = R N u n p 2 u n ( u n u ) d x λ R N a n ( x , u n ) ( u n u ) d x R N u n p * 1 ( u n u ) d x .

Computations similar to the ones of (3.18) show that ( a n ( , u n ) ) is bounded in L ( p * ) ( R N ) , and ( u n p * 1 ) enjoys the same property; hence,

lim n R N a n ( x , u n ) ( u n u ) d x = lim n R N u n p * 1 ( u n u ) d x = 0 .

Letting n in (4.4) entails

lim n Δ p u n , u n u = lim n R N u n p 2 u n ( u n u ) d x = 0 ,

so that the ( S + ) property of ( Δ p , D 0 1 , p ( R N ) ) (see [42, Proposition 2.2]) yields u n u in D 0 1 , p ( R N ) .□

Lemma 4.4

If Λ 3 > 0 is sufficiently small, then S is lower semi-continuous.

Proof

Let v n v in D 0 1 , p ( R N ) and u S ( v ) . We have to construct a sequence ( u n ) D 0 1 , p ( R N ) such that u n S ( v n ) for every n N and u n u in D 0 1 , p ( R N ) . To this aim, we consider the following family of problems, parameterized by indexes n , m N and defined by recursion on m :

(4.5) Δ p u n m = λ a n ( x , u n m 1 ) + ( u n m 1 ) p * 1 , in R N , u n 0 = u , for all n N .

By induction on m N , problem (4.5) admits a unique solution u n m D 0 1 , p ( R N ) for all n , m N , according to Minty-Browder’s theorem [9, Theorem 5.16].

Fixed R > 0 , for every g : R N R , we define g R : R N R as g R ( x ) = g ( R x ) for all x R N . By a change of variables, g R q = R N q g q for all q 1 .

We want to determine R , Λ 3 > 0 such that the set { z n m : n , m N } is bounded in D 0 1 , p ( R N ) , being z n m ( u n m ) R for all n , m N . We observe that z n m solves

(4.6) Δ p z n m = R p [ λ a n ( R x , z n m 1 ) + ( z n m 1 ) p * 1 ] .

Testing (4.6) with z n m , besides using (3.4), ( H w ), (3.1), λ ( 0 , Λ ) , Hölder’s inequality, and the boundedness of ( v n ) in D 0 1 , p ( R N ) , produces

z n m p p R p c 2 λ R N w R ( ( u ̲ λ ) R γ + ( v n ) R r 1 ) z n m d x + R N ( z n m 1 ) p * 1 z n m d x R p c 2 λ p 1 p 1 + γ R N w R ( u ̲ R γ + ( v n ) R r 1 ) z n m d x + z n m 1 p * p * 1 z n m p * R p c 2 Λ p 1 p 1 + γ ( w R u ̲ R γ ( p * ) + w R θ ( v n ) R p r 1 ) z n m p * + z n m 1 p * p * 1 z n m p * R p S 1 p z n m p c 2 Λ p 1 p 1 + γ R N ( p * ) ( w u ̲ γ ( p * ) + w θ v n p r 1 ) + S p * 1 p z n m 1 p p * 1 .

Setting H = c 2 S 1 p ( w u ̲ γ ( p * ) + w θ L r 1 ) 1 p 1 , we obtain

(4.7) z n m p H Λ 1 p 1 + γ R 1 N p + R p S p * p ( p 1 ) z n m 1 p p * 1 p 1 .

Now, we want to apply Lemma 2.7 to (4.7). First, we estimate, via Lemma 4.1,

z n 0 p = ( u ) R p = R N p u p R N p L .

Hence, the first condition in (2.3) is met, provided

(4.8) 1 2 R p S p * p ( p 1 ) R N p L p * p p 1 = S p * p ( p 1 ) L R p * p p 1 .

On the other hand, the second condition in (2.3) fulfilled whenever

(4.9) 2 1 p * p 1 > R p S p * p ( p 1 ) H Λ 1 p 1 + γ R 1 N p p * p p 1 = H p * p p 1 Λ p * p ( p 1 ) ( p 1 + γ ) S p * p ( p 1 ) .

Choosing R = R ( p , N ) > 0 sufficiently large and Λ 3 = Λ 3 ( p , N , w , γ , r , c 1 , c 2 ) > 0 small enough, both conditions (4.8)–(4.9) are fulfilled. By virtue of Lemma 2.7, after noting that all the quantities appearing in (4.8)–(4.9) do not depend on n , we conclude that there exists L ˆ = L ˆ ( p , N , R , Λ ) > 0 such that z n m p L ˆ for all n , m N , which implies u n m p R N p L ˆ for all n , m N .

Now, we pass to the weak limit the double sequence ( u n m ) n , m with respect to each index separately: up to sub-sequences, there exists ( u n ) , ( u m ) D 0 1 , p ( R N ) such that

(4.10) u n m u m in D 0 1 , p ( R N ) , as n , m N , u n m u n in D 0 1 , p ( R N ) , as m , n N .

Letting n in the weak formulation of (4.5), it turns out that both u 1 and u solve the problem

(4.11) Δ p U = λ a ( x , u ( x ) ) + u ( x ) p * 1 , in R N , U D 0 1 , p ( R N ) .

Since (4.11) admits a unique solution by Minty-Browder’s theorem, we deduce u 1 = u . Reasoning inductively on m N , it follows that u m = u for all m N . Pick an arbitrary ρ > 0 . Since D 0 1 , p ( R N ) c L p ( B ρ ) , the convergences mentioned in (4.10) are strong in L p ( B ρ ) . Accordingly, the double limit lemma [24, Proposition A.2.35] guarantees, up to sub-sequences,

lim n u n = lim n lim m u n m = lim m lim n u n m = lim m u m = u , in L p ( B ρ ) .

In particular, since ρ was arbitrary, a diagonal argument ensures u n u in R N .

Now, we prove that u n S ( v n ) for all n N . Letting m in the weak formulation of (4.5) reveals that u n solves ( P ˆ λ ) with v = v n , for all n N . Reasoning as in Lemma 3.2, boundedness of ( u n ) in D 0 1 , p ( R N ) allows us to assume u n p μ and u n p * ν for some bounded measures μ and ν . According to Lemmas 2.22.3, there exist some at most countable set A , a family of points ( x j ) j A R N , and two families of numbers ( μ j ) j A , ( ν j ) j A ( 0 , + ) such that

ν = u p * + j A ν j δ x j , μ u p + j A μ j δ x j , limsup n R N u n p * d x = R N d ν + ν , limsup n R N u n p d x = R N d μ + μ ,

and

(4.12) S ν j p p * μ j for all j A , S ν p p * μ ,

being μ , ν as in Lemma 2.3. Suppose, by contradiction, that A , so that μ j = ν j S N p for some j A , according to (4.12). A computation analogous to (3.22), jointly with u S ( v ) , ensures that

c > J ( u ) = J ( u ) 1 p * J ( u ) , u c ˆ ,

being c ˆ defined by (3.12), which contradicts c < c ˆ . Hence, concentration at points cannot occur; as in Lemma 3.2, a similar argument excludes concentration at infinity. We deduce u n u in L p * ( R N ) , which is the starting point of the proof of Lemma 4.3; thus, we infer u n u in D 0 1 , p ( R N ) . In particular, J n ( u n ) J ( u ) as n , so J n ( u n ) < c for all n sufficiently large, ensuring u n S ( v n ) .□

Theorem 4.5

For any λ ( 0 , Λ ) the problem

(4.13) Δ p u = λ w ( x ) f ( u , u ) + u p * 1 , i n R N , u > 0 , i n R N ,

admits a solution u D 0 1 , p ( R N ) .

Proof

Let us consider the following selection of the multi-function S defined in (4.2):

(4.14) T : , T ( v ) = min S ( v ) .

The function T is well defined, according to Lemma 4.2; moreover, it is continuous and compact, since S is lower semi-continuous and compact by Lemmas 4.34.4 (see [36, Lemma 3.16] for details). According to Schauder’s theorem (Theorem 2.6), T admits a fixed point u D 0 1 , p ( R N ) . Remark 3.7 guarantees u u ̲ λ , so that u solves (4.13).□

Remark 4.6

We observe that the choice (4.1) was made for the sake of simplicity: actually, any choice of a smaller L > S N p allows us to prove Theorem 4.5, provided Λ is small enough. To see that, it suffices to perform the energy estimate and the estimate of c ˆ retaining ε in Lemmas 3.13.2 instead of setting ε = 1 2 N . More precisely, for any v and u S ( v ) , the following estimates hold true:

u p p < 1 N ε 1 C ˆ ε λ p p 1 + γ ( L p ( r 1 ) + 1 ) + c ˆ , c ˆ = S N p N C ˆ ε λ p p 1 + γ ( L p ( r 1 ) + 1 ) .

Thus,

u p p < 1 N ε 1 S N p N S N p , as ε 0 ,

ensuring the validity of Lemma 4.1. Anyway, according to (3.32), one has Λ 2 0 as ε 0 , since C ˆ ε + : for this reason, the choice L = S N p is not feasible. On the contrary, L = S N p is admissible in the model case λ = 0 , even if concentration of compactness occurs.

5 Regularity of solutions

In this section, we prove that any solution u to (4.13) lying in an energy level under the critical Palais-Smale level c ˆ (3.12) belongs to L ( R N ) C loc 1 , α ( R N ) , and the estimates are uniform with respect to u within the energy level chosen. In addition, u decays pointwise as x + . We conclude the section with the proof of Theorem 1.1 and a remark concerning a problem related to ( P λ ).

Theorem 5.1

Let λ ( 0 , 1 ) and u D 0 1 , p ( R N ) be a solution to (4.13) satisfying

J ( u ) < c ˆ ,

where J and c ˆ are defined, respectively, in (3.3) and (3.12), with v = u and L u p . Then,

u M ,

for an opportune M = M ( p , N , w , r , c 2 ) > 0 , and

u C 1 , α ( B ¯ R ) C R ,

for some C R = C R ( R , p , N , w , γ , r , c 1 , c 2 ) > 0 and α ( 0 , 1 ] . Moreover,

(5.1) u ( x ) 0 , a s x + .

Proof

Given any k > 1 , we test (4.13) with ( u k ) + . Recalling that λ ( 0 , 1 ) and u > k > 1 in Ω k { x R N : u ( x ) > k } , besides using ( H f ) –( H w ) and Peter-Paul’s inequality, we obtain

( u k ) L p ( Ω k ) p λ Ω k w f ( u , u ) u d x + u L p * ( Ω k ) p * c 2 w Ω k u 1 γ d x + Ω k w u r 1 u d x + u L p * ( Ω k ) p * c 2 w u L p * ( Ω k ) p * + ε c 2 w u L p ( Ω k ) p + C ε u L p * ( Ω k ) p * + w θ Ω k + u L p * ( Ω k ) p * ε ( u k ) L p ( Ω k ) p + C ε ( u L p * ( Ω k ) p * + Ω k ) ε ( u k ) L p ( Ω k ) p + C ε ( u k L p * ( Ω k ) p * + k p * Ω k + Ω k ) .

Choosing ε = 1 2 and re-absorbing the term ( u k ) L p ( Ω k ) p on the left-hand side, we obtain

( u k ) L p ( Ω k ) p C ( u k L p * ( Ω k ) p * + k p * Ω k ) ,

for some C > 0 depending only on p , N , w , r , and c 2 . By Sobolev’s inequality, we obtain

u k L p * ( Ω k ) p C ( u k L p * ( Ω k ) p * + k p * Ω k ) ,

enlarging C if necessary. Let M > 2 and set k n M ( 1 2 n ) for all n N . Repeating verbatim the proof of [11, Lemma 3.2], we infer that u k n L p * ( Ω k n ) 0 as n , provided u M 2 L p * ( Ω M 2 ) is small enough. According to Remark 3.7, u solves ( P ˆ λ ) with v = u ; hence, Lemma 3.2 provides L p * ( R N ) -integrability of u , which is uniform in the sub-level set { u ˜ D 0 1 , p ( R N ) : J ( u ˜ ) J ( u ) < c ˆ } . As a consequence (see [8, p. 267]),

Ω M 2 u M 2 p * d x Ω M 2 u p * d x 0 , as M + ,

and the limit is uniform in u . Hence, u L ( R N ) with uniform L estimates.

Now, we prove uniform C 1 , α local estimates for u . By ( H f ) –( H w ), (3.1), Lemma 2.9, and the uniform L estimate of u , we obtain

(5.2) 0 λ f ( u , u ) + u p * 1 c 2 λ ( w u ̲ λ γ + w u r 1 ) + u p * 1 c 2 λ p 1 p 1 + γ w u ̲ γ + c 2 λ w u r 1 + u p * 1 = C ( 1 + u r 1 ) ,

for a suitable C = C ( p , N , w , γ , r , c 1 , c 2 ) > 0 . Applying [16, Theorem 1.5] (with b ( x , u , u ) = 1 + u r 1 , V ( x ) C , and q = r 1 ) yields u L loc ( R N ) with uniform L local estimates: more precisely,

(5.3) u L ( B ρ ) C L + ρ 1 p r + 2 , for all ρ > 0 ,

enlarging C if necessary. Thus, by (5.2), the right-hand side of ( P λ ) is locally bounded in R N , which entails, by nonlinear regularity theory (see [15, Corollary p. 830]), u C loc 1 , α ( R N ) with uniform C 1 , α local estimates.

In order to prove (5.1), we observe that (5.3) and (1.1) imply

w ( x ) u ( x ) r 1 C x r 1 p r + 2 l , in B R e ,

being R as in (1.1). Since

l > N + γ N p p 1 > N > N + 1 2 > p + 1 2 > p + 1 p r + 2 = r 1 p r + 2 + 1 ,

we deduce r 1 p r + 2 l < 1 , whence w u r 1 L q ( R N ) for some q > N . Consequently, reasoning as for (5.2) leads to

sup y R N λ f ( u , u ) + u p * 1 L q ( B 2 ( y ) ) c 2 λ p 1 p 1 + γ w u ̲ γ q + λ w u r 1 q + u p * 1 B 2 1 q .

An application of [35, Lemma 2.4] (adapting its proof to locally summable reaction terms) ensures that u L ( R N ) uniformly in u . Hence, a computation similar to (5.2) yields

λ f ( u , u ) C w u ̲ λ γ C x γ N p p 1 l , in B ρ e ,

for some C = C ( p , N , w , γ , r , c 1 , c 2 ) > 0 and for all ρ > 0 sufficiently large. The conclusion then follows by repeating the argument used in the proof of [53, Lemma 3.1].□

Proof of Theorem 1.1

Theorem 1.1 is a direct consequence of Theorems 4.5 and 5.1.□

Remark 5.2

At the end of this article, we would like to obtain a glimpse of another problem, which is a critical perturbation of a singular problem:

(Pλ′) Δ p u = w ( x ) f ( u , u ) + λ u p * 1 , in R N , u > 0 , in R N ,

being λ ( 0 , 1 ) and p , N , w , f as in ( P λ ).

Performing the change of variable z = λ 1 p * p u , one has

Δ p z = λ p 1 p * p w ( x ) f ˜ ( z , z ) + z p * 1 ,

where

f ˜ ( s , ξ ) = f λ 1 p p * s , λ 1 p p * ξ .

According to ( H f ) , one has

c 1 λ p 1 + γ p * p z γ λ p 1 p * p f ˜ ( z , z ) c 2 λ p 1 + γ p * p z γ + λ p r p * p z r 1 .

Since p 1 + γ p * p > p r p * p , problem ( P λ ) cannot be directly reduced to problem ( P λ ). Anyway, we note that p 1 + γ p * p , p r p * p > 0 , and this is mainly due to the p-sub-linearity of the convection terms; thus, the smallness conditions on λ for problem ( P λ ) are mapped into smallness conditions on λ p 1 + γ p * p and λ p r p * p for problem ( P λ ). Accordingly, the techniques used in this article may be effectively employed to study problem ( P λ ).

Acknowledgements

We warmly thank Prof. Sunra Mosconi for his valuable comments about the mountain pass theorem and the L estimates. This work has been partially carried out during a stay at the Department of Mathematics and Computer Sciences of the University of Catania: the authors would like to express their deep gratitude to this prestigious institution for its support and warm hospitality.

  1. Funding information: The authors are member of the Gruppo Nazionale per l’Analisi Matematica, la Probabilità e le loro Applicazioni (GNAMPA) of the Istituto Nazionale di Alta Matematica (INdAM); they were partially supported by the INdAM-GNAMPA Project 2023 titled Problemi ellittici e parabolici con termini di reazione singolari e convettivi (E53C22001930001). Laura Baldelli was partially supported by National Science Centre, Poland (Grant No. 2020/37/B/ST1/02742) and by the “Maria de Maeztu” Excellence Unit IMAG, reference CEX2020-001105-M, funded by MCIN/AEI/10.13039/501100011033/. Umberto Guarnotta was supported by the following research projects: 1) PRIN 2017 “Nonlinear Differential Problems via Variational, Topological and Set-valued Methods” (Grant no. 2017AYM8XW) of MIUR; and 2) PRA 2020–2022 “PIACERI” Linea 3 of the University of Catania. This study was carried out within the RETURN Extended Partnership and received funding from the European Union Next-GenerationEU (National Recovery and Resilience Plan - NRRP, Mission 4, Component 2, Investment 1.3 – D.D. 1243 2/8/2022, PE0000005).

  2. Author contributions: All authors have accepted responsibility for the entire content of this manuscript and consented to its submission to the journal, reviewed all the results, and approved the final version of the manuscript. All authors contributed equally to this work.

  3. Conflict of interest: The authors state no conflict of interest.

  4. Data availability statement: Data sharing is not applicable to this article as no datasets were generated or analysed during the current study.

References

[1] G. Astarita and G. Marrucci, Principles of Non-Newtonian Fluid Mechanics, McGraw-Hill, New York, 1974. Search in Google Scholar

[2] L. Baldelli and R. Filippucci, Existence results for elliptic problems with gradient terms via a priori estimates, Nonlinear Anal. 198 (2020), Paper No. 111894, 22pp. 10.1016/j.na.2020.111894Search in Google Scholar

[3] L. Baldelli, Y. Brizi, and R. Filippucci, Multiplicity results for (p,q)-Laplacian equations with critical exponent in RN and negative energy, Calc. Var. Partial Differential Equations 60 (2021), Paper No. 8, 30pp. 10.1007/s00526-020-01867-6Search in Google Scholar

[4] L. Baldelli, Y. Brizi, and R. Filippucci, On symmetric solutions for (p,q)-Laplacian equations in RN with critical terms, J. Geom. Anal. 32 (2022), Paper No. 120, 25pp. 10.1007/s12220-021-00846-3Search in Google Scholar

[5] L. Baldelli and R. Filippucci, Existence of solutions for critical (p,q)-Laplacian equations in RN, Commun. Contemp. Math. 25 (2022), Paper No. 2150109, 26pp. 10.1142/S0219199721501091Search in Google Scholar

[6] L. Baldelli and R. Filippucci, Multiplicity results for generalized quasilinear critical Schrödinger equations in RN, NoDEA Nonlinear Differential Equations Appl. 31 (2024), 8. 10.1007/s00030-023-00897-1Search in Google Scholar

[7] A. K. Ben-Naoum, C. Troestler, and M. Willem, Extrema problems with critical Sobolev exponents on unbounded domains, Nonlinear Anal. 26 (1996), 823–833. 10.1016/0362-546X(94)00324-BSearch in Google Scholar

[8] V. I. Bogachev, Measure Theory. Volume I, Springer-Verlag, Berlin, 2007. 10.1007/978-3-540-34514-5Search in Google Scholar

[9] H. Brezis, Functional analysis, Sobolev spaces and partial differential equations, Universitext, Springer, New York, 2011. 10.1007/978-0-387-70914-7Search in Google Scholar

[10] H. Brezis and L. Nirenberg, Positive solutions of nonlinear elliptic equations involving critical Sobolev exponents, Comm. Pure Appl. Math. 36 (1983), 437–477. 10.1002/cpa.3160360405Search in Google Scholar

[11] P. Candito, U. Guarnotta, and R. Livrea, Existence of two solutions for singular Φ-Laplacian problems, Adv. Nonlinear Stud. 22 (2022), 659–683. 10.1515/ans-2022-0037Search in Google Scholar

[12] A. Canino, B. Sciunzi, and A. Trombetta, Existence and uniqueness for p-Laplace equations involving singular nonlinearities, NoDEA Nonlinear Differential Equations Appl. 23 (2016), Paper No. 8, 18pp. 10.1007/s00030-016-0361-6Search in Google Scholar

[13] Y. S. Choi, A. C. Lazer, and P. J. McKenna, Some remarks on a singular elliptic boundary value problem, Nonlinear Anal. 32 (1998), 305–314. 10.1016/S0362-546X(97)00492-6Search in Google Scholar

[14] L. Damascelli, Comparison theorems for some quasilinear degenerate elliptic operators and applications to symmetry and monotonicity results, Ann. Inst. H Poincaré C Anal. Non Linéaire 15 (1998), 493–516. 10.1016/s0294-1449(98)80032-2Search in Google Scholar

[15] E. Di Benedetto, C1+α local regularity of weak solutions of degenerate elliptic equations, Nonlinear Anal. 7 (1983), 827–850. 10.1016/0362-546X(83)90061-5Search in Google Scholar

[16] F. Duzaar and G. Mingione, Local Lipschitz regularity for degenerate elliptic systems, Ann. Inst. H Poincaré Anal. Non Linéaire 27 (2010), 1361–1396. 10.1016/j.anihpc.2010.07.002Search in Google Scholar

[17] L. C. Evans and R. F. Gariepy, Measure theory and fine properties of functions, Textbook of Mathematics, CRC Press, Boca Raton, 2015. 10.1201/b18333Search in Google Scholar

[18] L. F. O. Faria, O. H. Miyagaki, and M. Tanaka, Existence of a positive solution for problems with (p,q)-Laplacian and convection term in RN, Bound. Value Probl. 158 (2016), Paper No. 158, 20pp. 10.1186/s13661-016-0665-9Search in Google Scholar

[19] I. Fonseca and G. Leoni, Modern Methods in the Calculus of Variations: Lp Spaces, Springer Monographs in Mathematics, Springer, New York, 2007. Search in Google Scholar

[20] W. Fulks and J. S. Maybee, A singular non-linear equation, Osaka Math. J. 12 (1960), 1–19. 10.2969/jmsj/01240401Search in Google Scholar

[21] L. Gambera and U. Guarnotta, Strongly singular convective elliptic equations in RN driven by a non-homogeneous operator, Commun. Pure Appl. Anal. 21 (2022), 3031–3054. 10.3934/cpaa.2022088Search in Google Scholar

[22] L. Gambera and U. Guarnotta, Existence, uniqueness, and decay results for singular Φ-Laplacian systems in RN. NoDEA Nonlinear Differential Equations Appl. 31 (2024), 111.10.1007/s00030-024-01001-xSearch in Google Scholar

[23] J. García Azorero and I. Peral Alonso, Multiplicity of solutions for elliptic problems with critical exponent or with a nonsymmetric term, Trans. Amer. Math. Soc. 323 (1991), 877–895. 10.1090/S0002-9947-1991-1083144-2Search in Google Scholar

[24] L. Gasiński and N. S. Papageorgiou, Nonlinear Analysis, Chapman & Hall/CRC, Boca Raton, 2006. Search in Google Scholar

[25] A. Ghanmi, M. Kratou, K. Saoudi, D. D. Repovš, Nonlocal p-Kirchhoff equations with singular and critical nonlinearity terms, Asymptot. Anal. 131 (2023), 125–143. 10.3233/ASY-221769Search in Google Scholar

[26] M. Ghergu and V. D. Rădulescu, Singular elliptic problems: bifurcation and asymptotic analysis, Oxford Lecture Series in Mathematical Applications, vol. 37, The Clarendon Press, Oxford University Press, Oxford, 2008. 10.1093/oso/9780195334722.003.0002Search in Google Scholar

[27] J. Giacomoni, I. Schindler, and P. Takáč, Sobolev versus Hölder local minimizers and existence of multiple solutions for a singular quasilinear equation, Ann. Sc. Norm. Super. Pisa Cl. Sci. 6 (2007), 117–158. 10.2422/2036-2145.2007.1.07Search in Google Scholar

[28] B. Gidas and J. Spruck, A priori bounds for positive solutions of nonlinear elliptic equations, Comm. Partial Differential Equations 6 (1981), 883–901. 10.1080/03605308108820196Search in Google Scholar

[29] J. V. Gonçalves and C. A. Santos, Positive solutions for a class of quasilinear singular equations, Electron. J. Differ. Equ. 2004 (2004), Paper no. 56, 15 pp. Search in Google Scholar

[30] A. Granas and J. Dugundji, Fixed Point Theory, Springer Monographs in Mathematics, Springer-Verlag, New York, 2003. 10.1007/978-0-387-21593-8Search in Google Scholar

[31] U. Guarnotta, Existence Results for Singular Convective Elliptic Problems, Ph.D. Thesis, University of Palermo, 2020/21. Search in Google Scholar

[32] U. Guarnotta, R. Livrea, and S. A. Marano, Some recent results on singular p-Laplacian equations, Demonstr. Math. 55 (2022), 416–428. 10.1515/dema-2022-0031Search in Google Scholar

[33] U. Guarnotta, R. Livrea, and S. A. Marano, Some recent results on singular p-Laplacian systems, Discrete Contin. Dyn. Syst. Ser. S 16 (2023), 1435–1451. 10.3934/dcdss.2022170Search in Google Scholar

[34] U. Guarnotta and S. A. Marano, Infinitely many solutions to singular convective Neumann systems with arbitrarily growing reactions, J. Differential Equations 271 (2021), 849–863. 10.1016/j.jde.2020.09.024Search in Google Scholar

[35] U. Guarnotta and S. A. Marano, A note on gradient estimates for p-Laplacian equations, Boll. Unione Mat. Ital. 17 (2024), 391–399, https://doi.org/10.1007/s40574-023-00371-x. Search in Google Scholar

[36] U. Guarnotta, S. A. Marano, and D. Motreanu, On a singular Robin problem with convection terms, Adv. Nonlinear Stud. 20 (2020), 895–909. 10.1515/ans-2020-2093Search in Google Scholar

[37] U. Guarnotta, S. A. Marano, and A. Moussaoui, Singular quasilinear convective elliptic systems in RN, Adv. Nonlinear Anal. 11 (2022), 741–756. 10.1515/anona-2021-0208Search in Google Scholar

[38] Y. Huang, On multiple solutions of quasilinear equations involving the critical Sobolev exponent, J. Math. Anal. Appl. 231 (1999), 142–160. 10.1006/jmaa.1998.6230Search in Google Scholar

[39] A. C. Lazer and P. J. McKenna, On a singular nonlinear elliptic boundary-value problem, Proc. Amer. Math. Soc. 111 (1991), 721–730. 10.2307/2048410Search in Google Scholar

[40] P.-L. Lions, The concentration-compactness principle in the calculus of variations. The limit case. I, Rev. Mat. Iberoamericana 1 (1985), 145–201. 10.4171/rmi/6Search in Google Scholar

[41] Z. Liu, D. Motreanu, and S. Zeng, Positive solutions for nonlinear singular elliptic equations of p-Laplacian type withdependence on the gradient, Calc. Var. Partial Differ. Equ. 58 (2019), Paper no. 28, 22 pp. 10.1007/s00526-018-1472-1Search in Google Scholar

[42] S. A. Marano, G. Marino, and A. Moussaoui, Singular quasilinear elliptic systems in RN, Ann. Mat. Pura Appl. 198 (2019), 1581–1594. 10.1007/s10231-019-00832-1Search in Google Scholar

[43] S. Mosconi and M. Squassina, Nonlocal problems at nearly critical growth, Nonlinear Anal. 136 (2016), 84–101. 10.1016/j.na.2016.02.012Search in Google Scholar

[44] D. Motreanu, V. V. Motreanu, and N. S. Papageorgiou, Topological and Variational Methods with Applications to Nonlinear Boundary Value Problems, Springer, New York, 2014. 10.1007/978-1-4614-9323-5Search in Google Scholar

[45] T. Mukherjee, P. Pucci, and L. Sharma, Nonlocal critical exponent singular problems under mixed Dirichlet-Neumann boundary conditions, J. Math. Appl. 531 (2024), Paper no. 127843, 28 pp. 10.1016/j.jmaa.2023.127843Search in Google Scholar

[46] N. S. Papageorgiou, V. D. Rădulescu, and D. D. Repovš, Nonlinear analysis - theory and methods, Springer Monographs in Mathematics, Springer, Cham, 2019. 10.1007/978-3-030-03430-6Search in Google Scholar

[47] K. Perera and E. A. B. Silva, Existence and multiplicity of positive solutions for singular quasilinear problems, J. Math. Anal.Appl. 323 (2006), 1238–1252. 10.1016/j.jmaa.2005.11.014Search in Google Scholar

[48] W. L. Perry, A monotone iterative technique for solution of p-th order (p<0) reaction-diffusion problems in permeable catalysis, J. Comput. Chemistry 5 (1984), 353–357. 10.1002/jcc.540050412Search in Google Scholar

[49] P. Pucci and J. Serrin, The maximum principle, Progress in Nonlinear Differential Equations and Their Applications, vol. 73, Birkhäuser Verlag, Basel, 2007. 10.1007/978-3-7643-8145-5Search in Google Scholar

[50] P. Pucci and L. Wang, The Brézis-Nirenberg equation for the Laplacian in the whole space, Discrete Contin. Dyn. Syst. Ser. S 13 (2023), 3270–3289. 10.3934/dcdss.2023068Search in Google Scholar

[51] D. Ruiz, A priori estimates and existence of positive solutions for strongly nonlinear problems, J. Differential Equations 199 (2004), 96–114. 10.1016/j.jde.2003.10.021Search in Google Scholar

[52] M. Struwe, Variational Methods, Springer-Verlag, Berlin, 1990. 10.1007/978-3-662-02624-3Search in Google Scholar

[53] J. Vétois, A priori estimates and application to the symmetry of solutions for critical p-Laplace equations, J. Differential Equations 260 (2016), 149–161.10.1016/j.jde.2015.08.041Search in Google Scholar

Received: 2024-01-29
Revised: 2024-03-23
Accepted: 2024-07-29
Published Online: 2024-11-26

© 2024 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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