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AAPP | Atti della Accademia Peloritana dei Pericolanti

Classe di Scienze Fisiche, Matematiche e Naturali

ISSN 1825-1242 Vol. 98, No. S2, A3 (2020)

SEQUENCES OF WEAK SOLUTIONS TO A FOURTH-ORDER ELLIPTIC PROBLEM

FILIPPOCAMMAROTO∗

ABSTRACT. This paper contains some results of existence of infinitely many solutions to an elliptic equation involving the p(x)-biharmonic operator coupled with Navier boundary conditions where the nonlinearities depend on two real parameters and do not possess any symmetric property. The approach is variational and the main tool is an abstract result of Ricceri.

1. Introduction

The aim of this paper is to establish the existence of infinitely many solutions to the following p(x)-biharmonic elliptic equation with Navier boundary conditions,

⎧ ⎨ ⎩ ∆2p(x)u= λ f (x, u) + µg(x, u) in Ω u= ∆u = 0 on ∂ Ω (Pλ ,µ)

where Ω ⊂ Rn(n ≥ 1) is a bounded domain with smooth boundary ∂ Ω, p ∈ C0(Ω) satisfies max{1, n/2} < infp≤ supp, ∆2p(x)u:= ∆(|∆u|p(x)−2∆u) is the p(x)-biharmonic operator, f, g : Ω × R → R are two Carathéodory functions with suitable behaviors, λ ∈ R and µ > 0. The operator ∆2p(x)is the natural generalization to the variable exponent framework of the standard p-biharmonic (p > 1 constant).

Equations with variable exponent growth conditions model various phenomena, for instance, the image restoration or the motion of the so called electrorheological fluids, characterized by their ability to drastically change their mechanical properties under the influence of an exterior electromagnetic field (see for instance R˚užiˇcka (2000) and Chen et al. (2004) and the survey paper of R˘adulescu (2015)). The most suitable contexts in which this kind of problems can be studied is represented by the Lebesgue and Sobolev spaces with variable exponents; for more informations about this topic, the reader is invited to consult Kováˇcik and Rákosník (1991), Fan et al. (2001), Fan and Zhao (2001), and Diening et al. (2011) together with the further sources of Cammaroto and Vilasi (2013a,b, 2014) and Vilasi (2016) in which several classes of variable exponent problems (and related multiplicity results) are investigated, still from a variational perspective.

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In the last years several authors have showed their interest in fourth-order differential problems involving p-biharmonic and p(x)-biharmonic operators, motivated by the fact that this type of equations arise in many domains like micro electromechanical systems, surface diffusion on solids, thin film theory, flow in Hele-Shaw cells and phase fieldmodels of multiphasic systems and, more generically, in fields such as the elasticity theory, or more in general, in continuous mechanics. Some recent existence results for Navier problems driven by the p-biharmonic and p(x)-biharmonic operators are provided by Furusho and Takaˆsi (1998), Ayoujil and El Amrouss (2009), Wang and Shen (2009), Candito and Livrea (2010), Ayoujil and El Amrouss (2011), Candito et al. (2012), Massar et al. (2012), Yin and Liu (2013), Kong (2014), Kefi and R˘adulescu (2017), and Bueno et al. (2018).

In this paper, the existence of infinitely many solutions to (Pλ ,µ) is obtained by finding

suitable conditions on the nonlinearities; unlike much of the existing literature on the subject this approach does not require any symmetry condition on the nonlinearities, but rather an opportune behaviour of the term µg at infinity, expressed in terms of its primitive. The approach used in this paper is variational; more precisely we will apply the following critical point theorem that Ricceri established in 2000 (Theorem 2.5 of Ricceri (2000)), recalled below for the reader’s convenience.

Theorem 1.1. Let E be a reflexive real Banach space and let Φ, Ψ : E → R be two sequen-tially weakly lower semicontinuous and Gâteaux differentiable functionals. Assume also that Ψ is strongly continuous and coercive.

For each r> infEΨ, define ϕ to be ϕ (r) := inf x∈Ψ−1(]−∞,r[) Φ(x) − inf Ψ−1(]−∞,r[)wΦ r− Ψ(x) , where Ψ−1(] − ∞, r[)

wis the closure of Ψ−1(] − ∞, r[) in the weak topology.

Fixed L∈ R, then

a) if {rk} is a real sequence such that limk→∞rk= +∞ and ϕ(rk) < L for all k ∈ N,

the following alternative holds: either Φ + LΨ has a global minimum or there exists a sequence{xk} ⊂ E of critical points of Φ + LΨ such that limk→∞Ψ(xk) = +∞;

b) if {sk} is a real sequence such that limk→∞sk= (infEΨ)+and ϕ(sk) < L for all

k∈ N, the following alternative holds: either there exists a global minimum of Ψ which is a local minimum of Φ + LΨ or there exists a sequence {xk} ⊂ E of

pairwise distinct critical points of Φ + LΨ with limk→∞Ψ(xk) = infEΨ which

weakly converges to a global minimum of Ψ.

Since its appearance in 2000 until our days, Theorem 1.1 has been a powerful tool to get multiplicity results for different kinds of problems. In particular, it has been applied to obtain the existence of infinitely many solutions for a vast range of differential problems. In each of these applications, in order to guarantee that ϕ(rk) < L (or ϕ(sk) < L), for each

k∈ N, and that the functional Φ + LΨ has no global minimum, it is necessary to construct suitable sequences of functions. Generally, in these constructions, one uses the norm of the variable raised to a suitable power which depends on the nature of the problem and that gives to the functions the requested regularity properties: in some application the norm is used without power (see, for instance, Cammaroto et al. (2005), Kristály (2006), Bonanno et al.(2010), and Dai and Wei (2010)), in some others it is raised to the second (Candito

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and Livrea (2010), Bonanno and Di Bella (2011), Candito et al. (2012), and Massar et al. (2012)) or to the third (Heidarkhani (2014) and Makvand Chaharlanga and Razani (2018)) or to the forth power (Afrouzi and Shokooh (2015)); Hadjian and Ramezani (2017) and Reza Heidari Tavani and Nazari (2019) combined the norm with trigonometric functions. The choice of a particular sequence of functions inside the proof reflects heavily on the assumptions and while there are some cases in which probably the choice is optimal, in some other cases it could happen that a different choice of the sequence would make the result applicable in a greater number of cases. This is the reason why in this paper an abstract class of test functions is introduced; some examples presented in Section 4 will clarify this fact. A similar procedure is used by Cammaroto and Genoese (2018) and Cammaroto and Vilasi (2019) and above all by Song (2014) where he doesn’t choose the test functions arbitrarily during the proof but uses two generic functions whose properties are described in the initial assumptions.

The paper is then structured as follows. Section 2 includes all the basic results about Lebesgue and Sobolev variable exponent spaces necessary for the variational set-up of Problem (Pλ ,µ). In Section 3 the multiplicity results will be presented and, finally, in Section 4 some concrete examples of nonlinearities will be exhibited.

2. Variational framework

We collect here some preliminary results about Lebesgue and Sobolev variable exponent spaces, which are used in our investigations.

To begin with, we fix some notation for the sequel. Given a measurable function u : Ω → R, we set u−:= essinf Ω u, u+:= esssup Ω u. We denote by ω := πn2/Γ(︁n

2+ 1)︁ the measure of the unit ball in Rn. If X is a Banach space,

the symbol B(x, r) denotes the open ball centered at x ∈ X and of radius r > 0 and B(x, r) its clousure.

Let Ω be a bounded smooth domain of Rn, n ≥ 1, and let p ∈ C0(Ω) satisfy 1 < p−≤ p+.

Define the variable exponent Lebesgue space Lp(x)(Ω) by Lp(x)(Ω) = {︃ u: Ω → R measurable: ∫︂ Ω |u|p(x)dx< +∞ }︃ . It is a reflexive Banach space when endowed with the Luxemburg norm

|u|p(x)= inf {︃ σ > 0 : ∫︂ Ω ⃓ ⃓ ⃓ u σ ⃓ ⃓ ⃓ p(x) dx≤ 1 }︃ . If we denote by ρp(x): Lp(x)(Ω) → R the functional defined by

ρp(x)(u) =

∫︂

|u|p(x)dx

for all u ∈ Lp(x)(Ω), it is the so-called modular of the space Lp(x)(Ω) and the following

proposition clarifies its relations with the Luxemburg norm.

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(1) |u|p(x)< 1 (= 1; > 1) ⇔ ρp(x)(u) < 1 (= 1; > 1); (2) |u|p(x)> 1 ⇒ |u|p − p(x)≤ ρp(x)(u) ≤ |u|p + p(x); (3) |u|p(x)< 1 ⇒ |u|p + p(x)≤ ρp(x)(u) ≤ |u| p− p(x); (4) |uk− u|p(x)→ 0 ⇔ ρp(x)(uk− u) → 0.

For any k ∈ N, define the variable exponent Sobolev space Wk,p(x)(Ω) by Wk,p(x)(Ω) ={︂u∈ Lp(x)(Ω) : Dαu∈ Lp(x)(Ω) for any |α| ≤ k}︂,

where Dαu is the partial derivative of u with respect to the multi-index

α = (α1, α2, . . . , αn) ∈ N0n and |α| = ∑ni=1αi. The space Wk,p(x)(Ω) is a separable and

reflexive Banach space under the norm ∥u∥k,p(x)=

|α|≤k

|Dαu| p(x).

We denote by W0k,p(x)(Ω) the closure of C∞

0(Ω) in Wk,p(x)(Ω) and X := W2,p(x)(Ω) ∩

W01,p(x)(Ω) will be the space naturally associated with (Pλ ,µ). On X the functional

∥u∥ := inf {︄ σ > 0 : ∫︂ Ω ⃓ ⃓ ⃓ ⃓ ∆u σ ⃓ ⃓ ⃓ ⃓ p(x) dx≤ 1 }︄

for any u ∈ X , defines a norm equivalent to ∥·∥2,p(x)(see for instance Zang and Fu (2008)). Clearly the embedding X ↪→ W2,p−(Ω) ∩W1,p−

0 (Ω) is continuous and, by Rellich-

Kon-drachov’s theorem, W2,p−(Ω) ∩ W01,p−(Ω) ↪→ C0(Ω) compactly when Ω is bounded and p−>n

2. This leads immediately to the following important result.

Proposition 2.2. The embedding X ↪→ C0(Ω) is compact provided that p−>n 2. The previous result implies that there exists a constant c∞> 0 such that

∥u∥≤ c∞∥u∥ (1)

for every u ∈ X . In addition, defining the modular ϒ : X → R by ϒ(u) = ρp(x)(∆u) =

∫︂

|∆u|p(x)dx

for all u ∈ X , it is well known that a similar result as Proposition 2.1 holds: Proposition 2.3. Let u ∈ X and let {uk} be a sequence in X. Then

(1) ∥u∥ < 1 (= 1; > 1) ⇔ ϒ(u) < 1 (= 1; > 1); (2) ∥u∥ ≥ 1 ⇒ ∥u∥p−≤ ϒ(u) ≤ ∥u∥p+; (3) ∥u∥ ≤ 1 ⇒ ∥u∥p+≤ ϒ(u) ≤ ∥u∥p−; (4) ∥uk− u∥ → 0 ⇔ ϒ(uk− u) → 0.

Now, for the motivations illustrated in the Introduction, let us introduce the following class of functions.

If {ak}, {bk}, {σk} are three real sequences with 0 < ak< bkand σk> 0 for all k ∈ N,

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(i) χk∈ W2,p

+

(ak, bk), for each k ∈ N;

(ii) 0 ≤ χk(x) ≤ σkfor a.e. x ∈ (ak, bk) and for each k ∈ N;

(iii) lim x→a+ k χk(x) = σk, lim x→b− k χk(x) = 0; (iv) lim x→a+k χk′(x) = lim x→b−k χk′(x) = 0;

(v) for all j ∈ {1, 2} there exists cj> 0, independent of k, such that

k( j)(x)| ≤ cj

σk

(bk− ak)j

(2) for a.e. x ∈ (ak, bk) and for each k ∈ N.

If x0∈ Ω, {bk} ⊂]0, +∞[ such that B(x0, bk) ⊂ Ω, for each k ∈ N, and {χk} ∈H ({ak}, {bk}, {σk}),

consider the function uk: Ω → R defined as follows:

uk(x) := ⎧ ⎨ ⎩ 0 in Ω \ B(x0, bk) σk in B(x0, ak) χk(|x − x0|) in B(x0, bk) \ B(x0, ak). (3)

Owing to the embedding W2,p+(Ω) ↪→ W2,p(x)(Ω), it is clear that {u

k} ⊂ X. Moreover, a

simple computation shows that, fixed k ∈ N, for any i = 1, 2, . . . , n one has

∂2uk ∂ x2i (x) = ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩ 0 in Ω \ B(x0, bk) 0 in B(x0, ak) χk′′(|x − x0|) (xi− x0 i)2 |x − x0|2 + +χk′(|x − x0|) |x − x0|2− (xi− x0i)2 |x − x0|3 in B(x0, bk) \ B(x0, ak) (4)

From (2) (4) we obtain the following inequality

|∆uk(x)| = χk′′(|x − x0|) + χk′(|x − x0|) n− 1 |x − x0| ≤ σk (bk− ak)2c2+ σk bk− ak n− 1 ak c1, (5)

thanks to which we are able to get the following estimation of the modular ϒ at uk

ϒ(uk) ≤ (︃ σk (bk− ak)2 c2+ σk bk− ak n− 1 ak c1 )︃p+ ω (bnk− ank) ≤ ω σ p+ k (bnk− ank) akp+(bk− ak)2p+(akc2+ (n − 1)(bk− ak)c1) p+ (6)

that is valid for those k ∈ N such that σk (bk− ak)2 c2+ σk bk− ak n− 1 ak c1≥ 1.

In the sequel, without further mentioning, we always assume that p ∈ C0(Ω) satisfies max{︂1,n

2 }︂

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Let us denote by C the class of all Carathéodory functions ζ : Ω × R → R satisfying sup

|t|≤ξ

|ζ (·,t)| ∈ L1(Ω) for all ξ > 0 and let f , g ∈C . A weak solution to (Pλ ,µ) is any function u ∈ X such that

∫︂ Ω |∆u|p(x)−2∆u∆vdx = λ ∫︂ Ω f(x, u)vdx + µ ∫︂ Ω g(x, u)vdx

for all v ∈ X . Obviously the weak solutions of problem (Pλ ,µ) are nothing but the critical points of the functionalE : X → R defined by

E (u) := Ψ(u) + λJF(u) + µJG(u),

for any u ∈ X , where

Ψ(u) := ∫︂ Ω |∆u|p(x) p(x) dx, JF(u) := − ∫︂ Ω F(x, u)dx, JG(u) := − ∫︂ Ω G(x, u)dx, (7)

for all u ∈ X , where

F(x,t) := ∫︂ t 0 f(x, s)ds, G(x,t) := ∫︂ t 0 g(x, s)ds for all (x,t) ∈ Ω × R. 3. Multiplicity results

The main result of this paper reads as follows: Theorem 3.1. Let f , g ∈C satisfy:

( f1) there exist a measurable function m : Ω → R, with 1 ≤ m ≤ p in Ω and m+< p−

and a function h∈ L1(Ω), such that

| f (x,t)| ≤ h(x)(︂1 + |t|m(x)−1)︂ for a.e. x∈ Ω, for all t ∈ R;

(g1) G(x,t) ≥ 0 for a.e. x ∈ Ω, for all t ≥ 0;

(g2) there exist x0∈ Ω, ρ, s1, s2> 0, such that B(x0, ρ) ⊂ Ω and

a:= lim inf t→+∞ ∫︂ Ω max |ξ |≤tG(x, ξ )dx ts1 < +∞, b:= lim supt→+∞ ∫︂ B(x0,ρ) G(x,t)dx ts2 > 0.

Then the following facts hold:

(i) if s1< p−and s2> p+, for all λ ∈ R and for all µ > 0, (Pλ ,µ) admits a sequence

of non-zero weak solutions;

(ii) if s1< p−and s2= p+, there exists µ1> 0 such that, for all λ ∈ R and for all

µ > µ1,(Pλ ,µ) admits a sequence of non-zero weak solutions;

(iii) if s1= p−and s2> p+, there exists µ2> 0 such that, for all λ ∈ R and for all

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(iv) if s1= p−and s2= p+, there exist γ > 1 and Cγ ,ρ> 0 such that, if Cγ ,ρ< bp− ap+ω cp− ∞ , (8)

(the previous inequality always being satisfied whether a= 0 or b = +∞) then µ1< µ2and for all λ ∈ R and every µ ∈ (µ1, µ2), (Pλ ,µ) admits a sequence of

non-zero weak solutions.

Proof. To prove (i), fixed λ ∈ R and µ > 0, we use Theorem 1.1, item a), with E = X, Ψ as in (7), Φ = λ JF+ µJG and L = 1. It is clear that Ψ is C1, sequentially weakly lower

semicontinuous and, being

Ψ(u) ≥ 1 p+∥u∥

p−,

coercive as well. The sequential weak lower semicontinuity of Φ follows, by standard arguments, from ( f1), (g2) and Proposition 2.2. Now, we define

ϕ (r) = inf

Ψ(u)<r

supΨ(w)≤rΦ − Φ(u) r− Ψ(u)

for all r > 0, and we will find a sequence {rk} ⊂ R, diverging to +∞, such that ϕ(rk) < 1

for all k ∈ N. To this aim, thanks to the definition of ϕ, it sufficies to build a sequence {uk} ⊂ X, with Ψ(uk) < rk, for all k ∈ N, and satisfying

sup Ψ(w)≤rk (︃ −λ ∫︂ Ω F(x, w)dx − µ ∫︂ Ω G(x, w)dx )︃ + λ ∫︂ Ω F(x, uk)dx+ + µ ∫︂ Ω G(x, uk)dx < rk− Ψ(uk). (9)

We choose uk= 0, for any k ∈ N. Thanks to (g2), fixed a˜ > a, for any k ∈ N there exists

αk≥ k such that ∫︂ Ω max |ξ |≤αk G(x, ξ )dx ≤ a˜αs1 k .

For any k ∈ N define

rk:= 1 p+cp− ∞ αp − k .

It is clear that rk→ +∞ as k → ∞ and Ψ(uk) < rk. To verify (9), observe that one has

∥w∥≤ c∞∥w∥ ≤ c∞max {︃ (p+Ψ(w)) 1 p+, (p+Ψ(w)) 1 p− }︃

for any w ∈ X . Taking this fact into account, if w ∈ X and Ψ(w) ≤ rk, one has, for k large

enough ∥w∥∞≤ c∞(p +r k)1/p − = αk

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and by ( f1), (g1), (g2) we obtain, for k large enough, − λ ∫︂ Ω F(x, w)dx − µ ∫︂ Ω G(x, w)dx ≤ |λ | ∫︂ Ω |h(x)| (︄ w+|w| m(x) m(x) )︄ dx+ + µ ∫︂ Ω max |ξ |≤αk G(x, ξ )dx ≤ |λ | ∥h∥L1(Ω) (︄ αk+ αkm+ m− )︄ + µa˜αs1 k ≤ ≤ |λ | ∥h∥L1(Ω)c∞(p +)p−1 r 1 p− k + |λ | ∥h∥L1(Ω) m− c m+ ∞ (p +)m+p−r m+ p− k + + µa˜cs1 ∞(p +)p−s1r s1 p− k < rk. (10)

According to part a) of Theorem 1.1, either the functional Φ + Ψ has a global minimum or there exists a sequence of weak solutions {vk} ⊂ X such that ∥vk∥ → +∞ as k → ∞. Let us

show that Φ + Ψ is unbounded from below. Thanks to (g2), fixed 0 < b˜ < b, for any k ∈ N

there exists βk≥ k such that

∫︂

B(x0,ρ)

G(x, βk)dx ≥ b˜βks2.

Let γ > 1 such that B(x0, γρ) ⊂ Ω and {χk} ∈H (ρ,γρ,βk). Similarly to (3), consider the

function ukdefined by uk(x) := ⎧ ⎨ ⎩ 0 in Ω \ B(x0, γρ) βk in B(x0, ρ) χk(|x − x0|) in B(x0, γρ) \ B(x0, ρ). (11)

Since βk→ +∞ as k → ∞, we can use (6) and we get

ϒ(uk) ≤ ω βp + k (γn− 1) ρ2p+−n(γ − 1)2p+ (c2+ (n − 1)(γ − 1)c1)p + and hence Ψ(uk) ≤ 1 p−ϒ(uk) ≤ 1 p−ωCγ ,ρβ p+ k , (12) where Cγ ,ρ= Cγ ,ρ({ηk}) := γn− 1 ρ2p+−n(γ − 1)2p+ (c2+ (n − 1)(γ − 1)c1)p + . (13)

So, one has

Φ(uk) + Ψ(uk) ≤ |λ | ∫︂ Ω |h(x)| (︄ uk+ |uk|m(x) m(x) )︄ dx− µb˜βs2 k + 1 p−ωCγ ,ρβ p+ k ≤ ≤ |λ | ∥h∥L1(B(x 0,ρ))βk+ |λ | ∥h∥L1(B(x 0,ρ)) m− β m+ k − µb˜β s2 k + 1 p−ωCγ ,ρβ p+ k (14)

and, since m+< p+< s2 and βk→ +∞ as k → ∞, Φ(uk) + Ψ(uk) → −∞, namely the

functional Ψ + Φ does not possess any global minimum, as desired. This concludes the proof of (i).

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µ1:=

ωCγ ,ρ

bp− (if b = +∞, we agree to read, as usual, µ1= 0). Then, if λ ∈ R and µ > µ1,

choosing ωCγ ,ρ

µ p− < b˜ < b, in the wake of the proof of (i), we obtain Φ(uk) + Ψ(uk) ≤ |λ | ∥h∥L1(B(x 0,ρ))βk+ |λ | ∥h∥L1(B(x 0,ρ)) m− β m+ k − µb˜β p+ k + 1 p−ωCγ ,ρβ p+ k

and also in this case Φ(uk) + Ψ(uk) → −∞ thanks to the choice of b˜. On the other hand, in

the case s1= p−and s2> p+, it suffices to pick µ2:=

1 ap+cp∞−

(as before, if a = 0, we set µ2= +∞). Then, fixing λ ∈ R, µ < µ2and choosing a < a˜ <

1 µ p+cp

, similarly to (i), using (g2) with such an a˜ we get

− λ ∫︂ Ω F(x, w)dx − µ ∫︂ Ω G(x, w)dx ≤ |λ | ∥h∥L1(Ω)c∞(p +)p−1 r 1 p− k + +|λ | ∥h∥L1(Ω) m− c m+ ∞ (p +)m+p−r m+ p− k + µa˜c p− ∞ p +r k< rk

for k large enough, due to the choice of a˜.

Finally, in the last case (iv), assumption (8) ensures that µ1< µ2. So, in the light of (ii) and

(iii), the conclusion is achieved for any λ ∈ R and µ ∈ (µ1, µ2). □

The next result is a direct consequence of Theorem 3.1 and deals with the case that the nonlinearities f and g have a particular form.

Theorem 3.2. Let h ∈ L1(Ω), h1∈ L1(Ω) \ {0} with h1≥ 0 in Ω, m : Ω → R

measur-able with1 ≤ m ≤ p in Ω and m+< p−. Let g˜ : R → R be a continuous function with ∫︂ t

0

g˜(ξ )dξ ≥ 0 for all t ≥ 0. Finally assume that there exist two real sequences {αk}, {βk},

withlimk→∞αk= limk→∞βk= +∞, and s1, s2, α, β > 0, such that

max |ξ |≤αk ∫︂ ξ 0 g˜(t)dt ≤ ααs1 k , ∫︂ βk 0 g˜(t)dt ≥ β βs2 k .

Then, considering the problem ⎧ ⎨ ⎩ ∆2p(x)u= λ h(x)|u|m(x)−2u+ µh1(x)g˜(u) in Ω u= ∆u = 0 on ∂ Ω (P˜λ ,µ)

the following facts hold:

(i) if s1< p−and s2> p+, for all λ ∈ R and for all µ > 0, (P˜λ ,µ) admits a sequence

of non-zero weak solutions;

(ii) if s1< p−and s2= p+, there exists µ1> 0 such that, for all λ ∈ R and for all

µ > µ1,(P˜λ ,µ) admits a sequence of non-zero weak solutions;

(iii) if s1= p−and s2> p+, there exists µ2> 0 such that, for all λ ∈ R and for all

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(iv) if s1= p−and s2= p+, there exist x0∈ Ω, ρ > 0, γ > 1 and Cγ ,ρ> 0 such that, if Cγ ,ρ< β p−∥h1∥L1(B(x 0,ρ)) α p+∥h1∥L1(Ω)ω cp − ∞ , (15)

then µ1< µ2and for all λ ∈ R and every µ ∈ (µ1, µ2), (P˜λ ,µ) admits a sequence

of non-zero weak solutions.

Proof. The proof follows immediately by applying Theorem 3.1 to the nonlinearities f(x,t) = h(x)|t|m(x)−2t, g(x,t) = h1(x)g˜(t)

for all (x,t) ∈ Ω × R. Assumptions ( f1) and (g1) are immediate to verify. Since h1̸≡ 0, let

us choose x0∈ Ω and ρ > 0 such that B(x0, ρ) ⊂ Ω and h1> 0 in B(x0, ρ). One has

∫︂ Ω max |ξ |≤αk G(x, ξ )dx = ∫︂ Ω max |ξ |≤αk (︃∫︂ ξ 0 h1(x)g˜(t)dt )︃ dx= = ∥h1∥L1(Ω) max |ξ |≤αk ∫︂ ξ 0 g˜(t)dt ≤ α ∥h1∥L1(Ω)αks1 and thus lim inf t→+∞ ∫︂ Ω max |ξ |≤tG(x, ξ )dx ts1 ≤ α ∥h1∥L1(Ω)< +∞. (16) In a similar way, ∫︂ B(x0,ρ) G(x, βk)dx = ∥h1∥L1(B(x 0,ρ)) ∫︂ βk 0 g˜(t)dt ≥ β ∥h1∥L1(B(x 0,ρ))β s2 k and therefore lim sup t→+∞ ∫︂ B(x0,ρ) G(x,t)dx ts2 ≥ β ∥h1∥L1(B(x0,ρ))> 0. (17)

So, the conclusions (i) − (iii) follow directly from Theorem 3.1 with a = α ∥h1∥L1(Ω)and

b= β ∥h1∥L1(B(x

0,ρ)). As for (iv), inequality (8) is verified by the joint use of (15), (16) and

(17).

Obviously, Theorem 3.1 can be applied even in the case of a constant exponent p. Anyway, in this case, the assumption m+< p−doesn’t allow to cover the case m = p. For this reason, the last theorem of this section concerns the case m = p. In this situation the existence of infinite weak solutions will be obtained not for each λ ∈ R but for λ running in an appropriate interval.

Theorem 3.3. Let p > max{1, n/2}, f , g ∈C such that (g1) and (g2) are verified. Moreover,

suppose that:

( f˜1) there exist h ∈ L1(Ω) such that | f (x,t)| = h(x)(︁1 + |t|p−1)︁ for a.e. in Ω and for

(11)

Then, considering the problem ⎧ ⎨ ⎩ ∆2pu= λ h(x)|u|p−2u+ µg(x, u) in Ω u= ∆u = 0 on ∂ Ω (P∗ λ ,µ)

the following facts hold:

(i) if s1< p < s2, for all λ such that |λ | < ∥h∥ 1

L1(Ω)c p

∞ (for all λ if h = 0) and for all

µ > 0, the problem (Pλ ,µ∗ ) admits a sequence of non-zero weak solutions;

(ii) if s1< p = s2, there exists µ1> 0 such that, for all µ > µ1, there exists λµ> 0

such that, for all|λ | < λµ, the problem (Pλ ,µ∗ ) admits a sequence of non-zero weak

solutions;

(iii) if s1= p < s2, there exists µ2> 0 such that, for all µ ∈ (0, µ2), there exists λµ> 0

such that, for all|λ | < λµ, the problem (Pλ ,µ∗ ) admits a sequence of non-zero weak

solutions;

(iv) if s1= s2= p, there exists γ > 1 and Cγ ,ρ> 0 such that, if

Cγ ,ρ<

b aωc∞p

(18) then µ1< µ2and for all µ ∈ (µ1, µ2), there exists λµ> 0 such that, for all |λ | < λµ

the problem (P∗

λ ,µ) admits a sequence of non-zero weak solutions.

Proof. The proof is similar to that of Theorem 3.1; the two main evaluations (10) and (14), when m = p, read as follows

− λ ∫︂ Ω F(x, w)dx − µ ∫︂ Ω G(x, w)dx ≤ |λ | ∥h∥L1(Ω)c∞p 1 pr 1 p k+ + |λ | ∥h∥L1(Ω)cprk+ µa˜cs∞1p s1 pr s1 p k (19) and Φ(uk) + Ψ(uk) ≤ |λ | ∥h∥L1(B(x 0,ρ))βk+ +|λ | ∥h∥L1(B(x0,ρ)) p β p k − µb˜β s2 k + 1 pωCγ ,ρβ p k (20)

with the same meaning of symbols as before. To prove (i), fix λ such that |λ | ≤∥h∥ 1

L1(Ω)c p

∞ and µ > 0. Thanks to the choice of λ and to

the fact that s1< p then, from (19) we get

λ ∫︂ Ω F(x, w)dx + µ ∫︂ Ω G(x, w)dx < rk (21)

for k large enough (remember that lim

k→∞rk= +∞); moreover, from (20) we obtain

lim

(12)

because p < s2.

To prove (ii), it is sufficient to choose µ1=

ωCγ ,ρ

bp . Fixed µ > µ1and b˜ in a similar way as done in Theorem 3.1, we define λµ= min

{︄ 1 ∥h∥L1(Ω)c∞p ,µ b˜ p − ωCγ ,ρ ∥h∥L1(B(x 0,ρ)) }︄ . Fixed λ such that |λ | < λµ, obviously, from (19), we get (21) (for k large enough) because s1< p and

thanks to the choice of λ . Moreover, using (20), the choice of λ and µ guarantees that (22) holds.

To prove (iii), it is sufficient to choose µ2=

1 ac∞pp

. Fixed µ ∈ (0, µ2) and a˜ in a similar

way as done in Theorem 3.1, we choose λµ =

1 − µa˜c∞pp

∥h∥L1(Ω)c∞p

. Fixed λ such that |λ | < λµ,

obviously, from (20), we get (22) because p < s2. Moreover, using (19), the choice of λ

and µ guarantees that (21) holds.

In the last case, to prove (iv), we observe that, thanks to (18), we have µ1< µ2. So, fixed

µ ∈ (µ1, µ2), and choosing a˜ and b˜ in a similar way as done in Theorem 3.1, we define

λµ= min {︄ 1 − µa˜c∞pp ∥h∥L1(Ω)cp∞ ,µ b˜ p − ωCγ ,ρ ∥h∥L1(B(x 0,ρ)) }︄

. Fixed λ such that |λ | < λµ, obviously, from (19),

we get (21) (for k large enough) because of the choice of λ and µ. Moreover, using (20), the choice of λ and µ guarantees that (22) holds.

□ 4. Examples

In this section we supply some examples related to the previous results. The first one concerns Theorem 3.2 (case (i)) and works as a prototype for this kind of nonlinearities.

Example 4.1. Let h1∈ L1(Ω) \ {0}, h1≥ 0 in Ω. Choose α, β , s1, s2> 0 with s1< p−and

s2> p+, and let {βr} be a non-decreasing real sequence such that limr→∞βr= +∞.

Define a subsequence {βrk} of {βr} and a new sequence {αk} recursively as follows:

βr1> (︃ α β )︃s2−s11 , βrk> (︃ β α )︃s11 β s2 s1 rk−1:= αk−1, for all k ≥ 2. (23) Now, define gˆ : R → R by gˆ(t) := ⎧ ⎪ ⎪ ⎨ ⎪ ⎪ ⎩ 0 for t ∈ (−∞, 0] At3+ Bt2 for t ∈ (0, β r1] β βrsk2 for t ∈ (βrk, αk], k≥ 1 Ckt3+ Dkt2+ Ekt+ Fk for t ∈ (αk, βrk+1], k≥ 1 (24)

(13)

where A:= −2ηβs2−3 r1 , B:= 3β βs2−2 r1 , Ck:= − 2(β βs2 rk − ααk−1) (βrk− αk−1)3 , Dk:= 3(βrk+ αk−1)(β β 2 rk− αα s1 k−1) (βrk− αk−1)3 , Ek:= − 6αk−1βrk(β β s2 rk − αα s1 k−1) (βrk− αk−1) 3 , Fk:= α βr2 kα s1 k−1(βrk− 3αk−1) + β β s2 rkα 2 k−1(3βrk− αk−1) (βrk− αk−1) 3 .

It is straightforward to verify that the sequences {αk}, {βrk} defined by (23) and the function

∫︂ t

0

g˜(ξ )dξ := gˆ(t) satisfy all the requirements of Theorem 3.2. Indeed, by construction, one has max |ξ |≤αk gˆ(ξ ) = β βs2 rk = αα s1 k , gˆ(βrk) = β β s2 rk, for all k ∈ N.

The second example is related to Theorem 3.2 (case (iv)). In this circumstance, for the sake of concreteness we limit ourselves to the one-dimensional setting, providing an explicit estimate of the constant c∞in (15).

Example 4.2. Let n = 1, Ω = (−1, 1), p(x) = −2x2+ 4 for all x ∈ (−1, 1), s1= p−= 2,

s2= p+= 4, h1∈ L1((−1, 1)) \ {0}, h1≥ 0 in (−1, 1) and

∫︂ 1/2

−1/2

h1(x)dx > 0.

Assume {αk}, {βrk}, g˜ as in Example 4.1. It is well-known that, for all u ∈ W

2,2((−1, 1)) ∩ W01,2((−1, 1)), one has max x∈(−1,1)|u(x)| ≤ √ 2 2 ⃦ ⃦u′⃦⃦ L2((−1,1)) and ⃦ ⃦u′⃦⃦ L2((−1,1))≤ 2 π ⃦ ⃦u′′⃦⃦ L2((−1,1)), so max x∈(−1,1)|u(x)| ≤ √ 2 π ⃦ ⃦u′′⃦⃦ L2((−1,1)).

Now, since Lp(x)((−1, 1)) ↪→ L2((−1, 1)) and

∥u∥L2((−1,1))≤ 2 max ⎧ ⎨ ⎩ 2 (︃ x2−1 2(x2−2) )︃+ , 2 (︃ x2−1 2(x2−2) )︃−⎫ ⎬ ⎭ |u|p(x)= 2√42|u|p(x)

(14)

(cf. Corollary 3.3.4 in Diening et al. 2011), collecting the previous estimates we finally get max

x∈(−1,1)|u(x)| ≤

2√48 π ∥u∥ . Now choose ρ =12, γ =32and for any k ∈ N let χk∈H

(︃ 1 2, 3 4, βrk )︃ be the function χk(x) := 64βrk (︃ 2x3−15 4 x 2+9 4x− 27 64 )︃ , for any x ∈(︃ 1 2, 3 4 )︃

. The computations of the first two derivatives of ηkyield

|χ′(x)| ≤ 6βrk, |χ ′′ (x)| ≤ 96βrk, so (2) is satisfied by c1= 3 2 and c2= 6, respectively.

As a next step, consider the sequence {uk} ⊂ W2,p(x)((−1, 1)) ∩W01,p(x)((−1, 1)) defined

by uk(x) := ⎧ ⎨ ⎩ 0 in (−1, 1) \ (−34,34) βrk in (− 1 2, 1 2) χk(|x|) in (−34,34) \ (−12,12). (25)

It turns out that Cγ ,ρ= 21834. Hence, inequality (8) is fulfilled provided that

β α > 22234√2 π2 ∥h1∥L1((−1,1)) ∥h1∥L1((−1/2,1/2)) .

The third example is again related to Theorem 3.2 and it concerns a similar type of nonlin-earity as in Example 4.1.

Example 4.3. Let p > 1, δ > 1 and let g˜ : R → R be the function such that

∫︂ t 0 g˜(ξ )dξ = ⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩ 0, in (−∞, 0], −2δt3+ 3δ t2, in (0, 1], 2p(k−1)δk in (︂ 2k−1δ k−1 p , 2k−1δkp ]︂ k≥ 1, Akt3+ Bkt2+Ckt+ Dk in (︂ 2k−1δ k p, 2kδ k p ]︂ k≥ 1 where Ak:= −2(p−3)k+4δ (p−3)k p (︁δ − 2−p)︁ , Bk:= 9 · 2(p−2)k+2δ (p−2)k p (︁δ − 2−p)︁ , Ck:= −3 · 2(p−1)k+3δ (p−1)k p (︁δ − 2−p)︁ , Dk:= 2pkδk(︁5δ − 22−p)︁ .

(15)

The function s satisfies all the assumption of Theorem 3.2 with α = 1, β = δ , αk= 2k−1δ

k p

and βk= 2kδ

k

p, for each k ∈ N. In particular

max |ξ |≤αk ∫︂ ξ 0 g˜(t)dt = ∫︂ 2k−1δ k p 0 g˜(t)dt = 2p(k−1)δk= αkp and ∫︂ βk 0 g˜(t)dt = 2pkδk+1= δ βkp for all k ∈ N.

The last example shows a case in which the choice of a sequence of functions with the norm raised to a second power makes Theorem 3.2 inapplicable, while the use of a different sequence solves the problem.

Example 4.4. Let p > max{1, n/2}, Ω = B(0, 1) in Rn, x0= 0, h1∈ L1(Ω) \ 0, with h1≥ 0,

ρ =1

2, γ = 2 and {σk} ⊂]0, +∞[ with limk→∞σk= +∞. Let {︁

χk1}︁ , {︁χk2}︁ ∈H (12, 1, {σk})

the sequences defined by

χk1(x) = 4σk(4x3− 9x2+ 6x − 1) and χk2(x) = σk 2 cos(π(2x − 1) + 1) for all x ∈(︃ 1 2, 1 )︃

and for each k ∈ N. We observe that, for each x ∈(︃ 1 2, 1 )︃ , |χk1 ′ (x)| ≤ 3σk, |χk1 ′′ (x)| ≤ 24σk

and then the constants cj(

{︁

χk1}︁), defined in (2), are respectively c1({︁χk1}︁) = 3 2 and c2(

{︁

χk1}︁) = 6. In a similar way, for each x ∈(︃ 1 2, 1 )︃ , we have |χ2 k ′ (x)| ≤ πσk, |χk2 ′′ (x)| ≤ 2π2σk

and, in this case, the constants cj(

{︁ χk2}︁) are respectively c1( {︁ χk2}︁) = π 2 and c2( {︁ χk1}︁) = π2 2 .

The last sequence of test function that we take in consideration has been used by Candito et al.2012 for the same kind of problem; in this case the norm is raised to the second power; namely χk3(x) = {︄ σk(︁−8x2+ 8x − 1 )︁ in (12,34) σk(8x2− 16x + 8) in (34, 1) (26) for each k ∈ N. In this case

|χ3 k ′ (x)| ≤ 4σk, |χk3 ′′ (x)| ≤ 16σk

(16)

and then c1({︁χk3}︁) = 2 and c2({︁χk1}︁) = 4. With respect to these three sequences of test functions the best Cγ ,ρdepends on the values of n and p. For instance, for n = 3 and p = 2

the best Cγ ,ρis the one in correspondance with the sequence {χk3}; in fact

Cγ ,ρ({χk1}) = 1134, Cγ ,ρ({χk2}) ≈ 913, Cγ ,ρ({χk3}) = 896.

But, for instance, for n = 4 and p = 3, the best Cγ ,ρis the one in correspondance with the

sequence {χk2} being Cγ ,ρ({χ 1 k}) = 69457, 5 Cγ ,ρ({χ 2 k}) ≈ 53871, Cγ ,ρ({χ 3 k}) = 60000.

Now, in any case, if we consider the function g˜ of Example 4.3, taking δ >

ω c∞p∥h1∥L1(Ω)Cγ ,ρ

∥h1∥L1(B(0,1 2)

the corresponding problem admits a sequence of non-zero weak solutions.

Acknowledgments

The author is member of the Gruppo Nazionale per l’Analisi Matematica, la Probabilità e le loro Applicazioni (GNAMPA) of the Istituto Nazionale di Alta Matematica (INdAM). References

Afrouzi, G. A. and Shokooh, S. (2015). “Existence of infinitely many solutions for quasilinear prob-lems with a p(x)-biharmonic operator”. Electronic Journal of Differential Equations 2015(317), 1–14.

Ayoujil, A. and El Amrouss, A. R. (2009). “On the spectrum of a fourth order elliptic equation with variable exponent”. Nonlinear Analysis, Theory, Methods and Applications 71(10), 4916–4926.

DOI:10.1016/j.na.2009.03.074.

Ayoujil, A. and El Amrouss, A. R. (2011). “Continuous spectrum of a fourth-order nonhomogeneous elliptic equation with variable exponent”. Electronic Journal of Differential Equations 24, 1–12. Bonanno, G. and Di Bella, B. (2011). “Infinitely many solutions for a fourth-order elastic beam

equation”. Nonlinear Differential Equations and Applications 18(3), 357–368.DOI:10.1007/ s00030-011-0099-0.

Bonanno, G., Molica Bisci, G., and O’Regan, D. (2010). “Infinitely many weak solutions for a class of quasilinear elliptic systems”. Mathematical and Computer Modelling 52(1-2), 152–160.DOI: 10.1016/j.mcm.2010.02.004.

Bueno, H., Paes-Leme, L., and Rodrigues, H. (2018). “Multiplicity of solutions for p-biharmonic problems with critical growth”. Rocky Mountain Journal of Mathematics 48(2), 425–442.DOI: 10.1216/RMJ-2018-48-2-425.

Cammaroto, F., Chinnì, A., and Di Bella, B. (2005). “Infinitely many solutions for the Dirichlet problem involving the p-Laplacian”. Nonlinear Analysis, Theory, Methods and Applications 61(1-2), 41–49.DOI:10.1016/j.na.2004.11.009.

Cammaroto, F. and Genoese, F. (2018). “Infinitely many solutions for a nonlinear Navier problem involving the p-biharmonic operator”.

Cammaroto, F. and Vilasi, L. (2013a). “On a perturbed p(x)–Laplacian problem in bounded and unbounded domains”. Journal of Mathematical Analysis and Applications 402(1), 71–83.DOI: 10.1016/j.jmaa.2013.01.013.

(17)

Cammaroto, F. and Vilasi, L. (2013b). “On a Schrödinger-Kirchhoff-type equation involving the p(x)-Laplacian”. Nonlinear Analysis, Theory, Methods and Applications 81, 42–53.DOI:10.1016/ j.na.2012.12.011.

Cammaroto, F. and Vilasi, L. (2014). “Existence of three solutions for a degenerate Kirchhoff-type transmission problem”. Numerical Functional Analysis and Optimization 35(7-9), 911–931.DOI: 10.1080/01630563.2014.895752.

Cammaroto, F. and Vilasi, L. (2019). “Sequences of weak solutions for a Navier problem driven by the p(x)-biharmonic operator”. Minimax Theory and its Applications 4(1), 71–85.

Candito, P., Li, L., and Livrea, R. (2012). “Infinitely many solutions for a perturbed nonlinear Navier boundary value problem involving the p-biharmonic”. Nonlinear Analysis, Theory, Methods and Applications75(17), 6360–6369.DOI:10.1016/j.na.2012.07.015.

Candito, P. and Livrea, R. (2010). “Infinitely many solution for a nonlinear Navier boundary value problem involving the p-biharmonic”. Studia Universitatis Babes-Bolyai Mathematica LV(4), 41–51.

Chen, Y., Levine, S., and Rao, R. (2004). “Functionals with p(x)-growth in image processing”. Duquesne University, Department of Mathematics and Computer Science, Technical Report. Dai, G. and Wei, J. (2010). “Infinitely many non-negative solutions for a p(x)-Kirchhoff-type problem

with Dirichlet boundary condition”. Nonlinear Analysis 73, 3420–3430.DOI:10.1016/j.na.2010. 07.029.

Diening, L., Harjulehto, P., Hästö, and R˚užiˇcka, M. (2011). Lebesgue and Sobolev spaces with variable exponents. (Lecture Notes in Mathematics). Springer-Verlag Berlin Heidelberg.

Fan, X. L., Shen, J., and Zhao, D. (2001). “Sobolev embedding theorems for spaces Wk,p(x)(Ω)”. Journal of Mathematical Analysis and Applications262, 749–760.DOI:10.1006/jmaa.2001.7618. Fan, X. L. and Zhao, D. (2001). “On the spaces Lp(x)(Ω) and Wm,p(x)(Ω)”. Journal of Mathematical

Analysis and Applications263, 424–446.DOI:10.1006/jmaa.2000.7617.

Furusho, Y. and Takaˆsi, K. (1998). “Positive entire solutions to nonlinear biharmonic equations in the plane”. Journal of Computational and Applied Mathematics 88(1), 161–173.DOI: 10.1016/S0377-0427(97)00214-8.

Hadjian, A. and Ramezani, M. (2017). “Existence of infinitely many solutions for fourth-order equations depending on two parameters”. Electronic Journal of Differential Equations 2017(117), 1–10.

Heidarkhani, S. (2014). “Infinitely many solutions for systems of n fourth order partial differential equations coupled with Navier boundary conditions”. Arab Journal of Mathematical Sciences 20(1), 77–100.DOI:10.1016/j.ajmsc.2013.04.003.

Kefi, K. and R˘adulescu, V. D. (2017). “On a p(x)-biharmonic problem with singular weights”. Zeitschrift für angewandte Mathematik und Physik68(4).DOI:10.1007/s00033-017-0827-3. Kong, L. (2014). “On a fourth order elliptic problem with a p(x)-biharmonic operator”. Applied

Mathematics Letters27, 21–25.DOI:10.1016/j.aml.2013.08.007.

Kováˇcik, O. and Rákosník, J. (1991). “On spaces Lp(x)and Wk,p(x)”. Czechoslovak Mathematical Journal41(4), 592–618.DOI:10.21136/CMJ.1991.102493.

Kristály, A. (2006). “Infinitely many solutions for a differential inclusion problem in Rn”. Journal of Differential Equations220(2), 511–530.DOI:10.1016/j.jde.2005.02.007.

Makvand Chaharlanga, M. and Razani, A. (2018). “Infinitely Many Solutions for a Fourth Order Singular Elliptic Problem”. Filomat 32(14), 5003–5010.DOI:10.2298/FIL1814003M.

Massar, M., Hssini, E. L., and Tsouli, N. (2012). “Infinitely many solutions for class of Navier boundary (p, q)-biharmonic systems”. Electronic Journal of Differential Equations 2012(163), 1–9.

(18)

R˘adulescu, V. D. (2015). “Nonlinear elliptic equations with variable exponent: Old and new to Professor Enzo L. Mitidieri, with cordial wishes for his 60th birthday”. Nonlinear Analysis, Theory, Methods and Applications121, 336–369.DOI:10.1016/j.na.2014.11.007.

Reza Heidari Tavani, M. and Nazari, A. (2019). “Infinitely many weak solutions for a fourth-order equation with nonlinear boundary conditions”. Miskolc Mathematical Notes 20(1), 525–538.DOI: 10.18514/MMN.2019.2648.

Ricceri, B. (2000). “A general variational principle and some of its applications”. Journal of Compu-tational and Applied Mathematics113(1), 401–410.DOI:10.1016/S0377-0427(99)00269-1. R˚užiˇcka, M. (2000). Electrorheological Fluids: Modeling and Mathematical Theory. Springer-Verlag

Berlin Heidelberg.

Song, Y. (2014). “A nonlinear boundary value problem for fourth-order elastic beam equations”. Boundary Value Problems2014(191), 1–11.DOI:10.1186/s13661-014-0191-6.

Vilasi, L. (2016). “Eigenvalue estimate for stationary p(x)-Kirchhoff problems”. Electronic Journal of Differential Equations186, 1–9.

Wang, L. and Shen, Y. (2009). “Infinitely many sign-changing solutions for a class of biharmonic equation without symmetry”. Nonlinear Analysis: Theory, Methods and Applications 71(3-4), 967–977.DOI:10.1016/j.na.2008.11.052.

Yin, H. and Liu, Y. (2013). “Existence of three solutions for a Navier boundary value problem involving the p(x)-biharmonic”. Bulletin of the Korean Mathematical Society 50(6), 1817–1826.

DOI:10.4134/BKMS.2013.50.6.1817.

Zang, A. and Fu, Y. (2008). “Interpolation inequalities for derivatives in variable exponent Lebesgue-Sobolev spaces”. Nonlinear Analysis: Theory, Methods and Applications 69(10), 3629–3636.DOI: 10.1016/j.na.2007.10.001.

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Università degli Studi di Messina

Dipartimento di Scienze Matematiche e Informatiche, Scienze Fisiche e Scienze della Terra Viale F. Stagno d’Alcontres, 31

98166 Messina, Italy Email: fdcammaroto@unime.it

Paper contributed to the meeting on “Variational Analysis, PDEs and Mathematical Economics“, held in Messina, Italy (19–20 September 2019), on the occasion of Prof. Antonino Maugeri’s 75th birthday,

under the patronage of the Accademia Peloritana dei Pericolanti Manuscript received 8 March 2020; published online 13 December 2020

© 2020 by the author(s); licensee Accademia Peloritana dei Pericolanti (Messina, Italy). This article is an open access article distributed under the terms and conditions of theCreative Commons Attribution 4.0 International License (https://creativecommons.org/licenses/by/4.0/).

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