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On some classes of generalized Schrödinger equations

  • Amanda S. S. Correa Leão , Joelma Morbach , Andrelino V. Santos and João R. Santos Júnior EMAIL logo
Published/Copyright: August 22, 2020

Abstract

Some classes of generalized Schrödinger stationary problems are studied. Under appropriated conditions is proved the existence of at least 1 + i=2m dim Vλi pairs of nontrivial solutions if a parameter involved in the equation is large enough, where Vλi denotes the eigenspace associated to the i-th eigenvalue λi of laplacian operator with homogeneous Dirichlet boundary condition.

MSC 2010: 35J10; 35J25; 35J60

1 Introduction

Recently, it has been studied in [19] the following class of generalized Schrödinger problems

div(ϑ(u)u)+12ϑ(u)|u|2=λ|u|q2uinΩ,u=0onΩ, (Pλ,q)

where Ω ⊂ RN, N ≥ 3, is a bounded smooth domain, q, λ are real parameters and ϑ : R → [1, ∞) is an even C1-function verifying:

  1. tϑ(t) is decreasing in (− ∞, 0) and increasing in (0, ∞);

  2. tϑ(t)/t2 increasing in (− ∞, 0) and decreasing in (0, ∞);

  3. lim|t|→∞ ϑ(t)/t2 = α2/2, for some α > 0.

By considering the ordinary differential equation

f(s)=1ϑ(f(s))1/2andf(0)=0, (ODE)

whose unique solution is f(s) = Y−1(s), with Y(t):=0tϑ(r)1/2dr, the authors proved that

Proposition 1.1

The following claims hold:

  1. f is an increasing C2-diffeomorphism, with f″(s) = −ϑ′(f(s))/2ϑ(f(s))2;

  2. 0 < f′(s) ≤ 1, for all s ∈ R;

  3. lims→0 f(s)/s = 1/ϑ(0)1/2;

  4. |f(s)| ≤ |s|, for all s ∈ R;

  5. Suppose that (ϑ1) − (ϑ2) hold. Then, |f(s)|/2 ≤ f′(s)|s| ≤ |f(s)|, for all s ∈ R, and the map s ↦ |f(s)|/ |s| is nonincreasing in (− ∞, 0) and nondecreasing in (0, ∞);

  6. Suppose that (ϑ1) − (ϑ3) hold. Then,

    lim|s||f(s)||s|=8α21/4andlim|s|f(s)s=0,

    where α is given in (ϑ3).

Motivated by ideas in [5] and [14], the authors in [19] make use of the following approach: Despite the energy functional associated to (Pλ,q) is not well defined in H01 (Ω), Proposition 1.1 allows them to consider the change of variable v = f(u) in the semilinear problem (Pλ,q) in order to obtain the problem

Δv=λg(v)inΩ,v=0onΩ, ( Pλ,q )

where g(s) := f′(s)|f(s)|q−2 f(s), which has the advantage of possessing a well defined C1-energy functional in H01 (Ω), given by

Iλ,q(v)=12v2λΩG(v)dx, (1.1)

where ∥v2 := ∫Ω|∇ v|2 dr and G(s)=0sg(r)dx=(1/q)|f(s)|q. They also prove that critical points of (1.1) in C1(Ω) are weak solutions of (Pλ,q). In this way, by working with ( Pλ,q ), among other things, they were able to prove that:

  1. If q = 2, λ > ϑ(0)λ1 and (ϑ1) − (ϑ2) holds, then (Pλ,q) has a unique positive solution;

  2. If q = 4, λ > (α2/4)λ1 and (ϑ1) − (ϑ3) holds, then (Pλ,q) has at least one positive solution.

Having in mind the previous results, the present paper has as its main goal to improve the results in [19] when one considers the cases q = 2 or q = 4 in problem (Pλ,q). Indeed, since in these two particular cases we prove in Lemma 2.1 that g is asymptotically linear at zero and at infinity, respectively, by using genus theory combined with arguments involving the Nehari manifold, it is possible to show that the number of solutions increases with λ. To be more precise, if dim Vλi denotes the dimension of the eigenspace Vλi associated to i-th eigenvalue λi of laplacian operator under homogeneous Dirichlet boundary condition, we prove the following multiplicity result:

Theorem 1.2

Suppose that (ϑ1) − (ϑ3) hold.

  1. If q = 2 and λ > ϑ(0)λm, then problem (Pλ,q) possesses at least 1 + i=2m dim Vλi pairs of nontrivial solutions ui with Iλ,2(f−1(ui)) > 0;

  2. If q = 4 and λ > (α2/4)λm, then problem (Pλ,q) has at least 1 + i=2m dim Vλi pairs of nontrivial solutions ui with Iλ,4(f−1(ui)) > 0.

By comparing Theorem 1.2 in [19] with Theorem 1.2(i) previously aimed, we can immediately conclude that at least i=2m dim Vλi of solutions provided in Theorem 1.2(i) are sign-changing.

To better understand the relevance of Schrödinger equations in different fields of applied science, we refer to [1, 2, 3, 10, 11, 12, 13, 15, 17]. For a brief history about stationary Schrödinger equations (generalized or not), see [5, 6, 7, 8, 9, 14, 16, 20, 21, 22, 25].

The paper is organized in a unique section where we study both cases, q = 2 and q = 4.

2 Multiplicity of solutions

Since, by [19], it does not exist any nontrivial solution when λ ≤ 0, along of this section we are just considering positive values of λ. Moreover, before proving the main results of this section we need to study the properties of function g. Such properties play an important role throughout the paper.

Lemma 2.1

Suppose that (ϑ1) − (ϑ3) hold. Then:

  1. Map s ↦ |g(s)| is decreasing in (− ∞, 0), increasing in (0, ∞), lims→0g(s)/s = 1/ϑ(0) and lim|s|→∞|g(s)| = 2 /α, if q = 2;

  2. Map sg(s)/s is decreasing in (− ∞, 0), increasing in (0, ∞), lims→0g(s)/s = 0 and lim|s|→∞g(s)/s = 4/α2, if q = 4;

  3. Map s ↦ (1/2)g(s)sG(s) is decreasing in (− ∞, 0), increasing in (0, ∞) and lim|s|→∞ [(1/2)g(s)sG(s)] = +∞, if q = 4.

Proof

  1. The monotonicity is a straightforward consequence of Proposition 1.1(ii) and (ϑ2). On the other hand, by Proposition 1.1(iii)

    lims0g(s)s=lims01ϑ(f(s))1/2×f(s)s=1ϑ(0).

    Moreover, by (ϑ3)

    lim|s||g(s)|=lim|s|1(ϑ(f(s))/f(s)2)1/2=2α.
  2. Since f is odd (because ϑ is even), it is sufficient to prove this item for s > 0. Observe that

    g(s)s=f(s)3sϑ(f(s))1/2=t2Y(t)×tϑ(t)1/2,

    where t := f(s) and Y(t):=0tϑ(r)1/2dr. It follows from (ϑ2) that t/ϑ(t)1/2 (and consequently t2/Y(t)) is increasing in (0, ∞). This proves that g(s)/s is increasing in (0, ∞). Moreover, by item (iii) and (vi) of Proposition 1.1, we have

    lims0g(s)s=lims0f(s)2ϑ(f(s))1/2×f(s)s=0

    and

    limsg(s)s=limsf(s)s1/22×f(s)ϑ(f(s))1/2=8α21/2×2α=4α2.
  3. The monotonicity follows immediately from (ii). To prove the second part, note that

    12g(s)sG(s)=t34ϑ(t)1/22Y(t)tϑ(t)1/2.

    By (ϑ3) we know that t3/4ϑ(t)1/2 goes to infinity as t goes to infinity. On the other hand, by (ϑ2), 2Y(t) − (t)1/2 is nonnegative and increasing in (0, ∞). Indeed, by defining h(t) := 2Y(t) − (t)1/2, we have h(0) = 0 and

    h(t)=2ϑ(t)tϑ(t)2ϑ(t)1/2>0,t>0.

The result follows. □

From now on {ej} stands for a Hilbertian basis of H01 (Ω) composed by eigenfunctions of the laplacian operator with homogeneous Dirichlet boundary condition, Vλj is the eigenspace associated to λj, 𝓢 and 𝓢d(m) are, respectively, the unit sphere of H01 (Ω) and the unit sphere of Wm:=j=1mVλj.

2.1 Case q = 2

Proof of Theorem 1.2

(i):

By Lemma 2.1(i) and Sobolev embedding

Iλ,2(v)12v22λαΩ|v|dx12v22Cλαv.

Therefore Iλ,2 is coercive. Since Iλ,2 is weakly lower semicontinuous, we conclude that Iλ,2 is bounded from below. On the other hand, since

Iλ,2(sv)s2=12λ[v0]G(sv)(sv)2v2dx,

for all vd(m). We conclude from Lemma 2.1(i), L’Hospital and Lebesgue Dominated Convergence Theorem that

lims0Iλ,2(sv)s2=12λ2ϑ(0)Ωv2dx,

for all vd(m). Since v=j=1d(m)vλjej, where d(m) := 1 + i=2m dim Vλi, we get

lims0Iλ,2(sv)s2=12λ2ϑ(0)j=1d(m)vj2Ωej2dx+jivjviΩejeidx=12λ2ϑ(0)j=1d(m)vj2λj.

Since v ∈ 𝓢d(m),

lims0Iλ,2(sv)s2=12j=1d(m)1λϑ(0)λjvj2121λϑ(0)λm<0,

for all v ∈ 𝓢d(m), because λ > ϑ(0)λm. Therefore, there exist ε, δ > 0 such that

Iλ,2(sv)=(Iλ,2(sv)/s2)s2εs2,

for all 0 < s < δ and v ∈ 𝓢d(m). Fixing 0 < s < δ, we have

supwsSd(m)Iλ,2(w)<0.

Since Iλ,2 is coercive, it is standard to prove that it satisfies the (PS)c condition. Finally, as Iλ,2 is an even C1-functional, it follows from Theorem 9.1 in [18] (see also [4]) that Iλ,2 has at least d(m) pairs of critical points. □

2.2 Case q = 4

Before we are ready to prove Theorem 1.2(ii), we will make a careful study about some topological and geometrical aspects involving the Nehari Manifold. Let

N=vH01(Ω){0}:v2=λΩg(v)vdx

be the Nehari manifold associated to Iλ,4, 𝓢 the unit sphere in H01 (Ω) and

F:=vH01(Ω):v2<4λα2Ωv2dx.

Lemma 2.2

If ϑ satisfies (ϑ1) − (ϑ3) and λ > (α2/4)λ1, the following claims hold:

  1. The set 𝓕 is open and nonempty;

  2. 𝓕 = {v H01 (Ω) : ∥v2 = (4λ/α2)∫Ω v2 dx};

  3. 𝓕c = {v H01 (Ω) : ∥v2 ≥ (4λ/α2)∫Ωv2 dx};

  4. 𝓝 ⊂ 𝓕;

  5. 𝓢 ∩ 𝓕 ≠ ∅.

Proof

(i) Since λ > (α2/4)λ1, any eigenfunction associated to λ1 belongs to 𝓕. Moreover, 𝓕 = Φ−1(− ∞, 0) where Φ: H01 (Ω) → ℝ is the continuous functional defined by Φ(v) = ∥v2 − (4λ/α2)∫Ωv2 dx. Items (ii) and (iii) are immediate.

(iv) If v ∈ 𝓝 then, by Lemma 2.1(ii), we obtain

v2=λ[v0]g(v)vv2dx<4λα2Ωv2dx.

(v) It is sufficient to choose a normalized (in H01 (Ω)) eigenfunction associated to λ1. □

By previous Lemma, the set 𝓢𝓕 := 𝓢 ∩ 𝓕 is open in 𝓢. Moreover, 𝓢𝓕 = {v ∈ 𝓢: 1 = (4λ/α2)∫Ωv2dx} and SFc = {v ∈ 𝓢: 1 ≥ (4λ/α2)∫Ωv2dx} are nonempty because any normalized eigenfunction associated to λj such that λ ≤ (α2/4)λj, belongs to SFc . Thus, 𝓢𝓕 is a noncomplete C1-submanifold of H01 (Ω).

Lemma 2.3

Suppose that ϑ verifies (ϑ1) − (ϑ3) and let hv : [0, ∞) → R be defined by hv(s) = Iλ,4(sv).

  1. For each v ∈ 𝓕, there exists a unique sv > 0 such that hv (s) > 0 in (0, sv), hv (sv) = 0 and hv (s) < 0 in (sv, ∞). Moreover, sv ∈ 𝓝 if, and only if, s = sv;

  2. For each v ∈ 𝓕c ∖ {0}, hv (s) > 0 for all s ∈ (0, ∞).

Proof

  1. Observe that hv(0) = 0. Moreover, for each v ∈ 𝓕, we have

    hv(s)s2=12v2λ[v0]G(sv)(sv)2v2dx. (2.1)

    Thus, in view of Lemma 2.1(ii), L’Hôspital rule and Lebesgue’s dominated convergence theorem, it follows that

    limshv(s)s2=12v2(4λ/α2)Ωv2dx<0.

    Showing that lims→∞hv(s) = − ∞. Moreover, hv(s) is positive for s small enough. Indeed, reasoning as in the previous limit, we get

    lims0+hv(s)s2=12v2λ[v0]G(sv)(sv)2v2dx=12v2>0.

    Hence, there exists a global maximum point sv > 0 of hv which, by Lemma 2.1(ii), is the unique critical point of hv.

  2. If v ∈ 𝓕c ∖ {0}, then ∥v2 ≥ (4λ/α2)∫Ωv2dx. Thus, by Lemma 2.1(ii), it follows that

    hv(s)s=v2λ[v0]g(sv)svv2dxλ[v0]4α2g(sv)svv2dx>0,s>0.

    Consequently, hv (s) > 0 for all s ∈ (0, ∞). □

Lemma 2.4

If ϑ verifies (ϑ1) − (ϑ3), the following claims hold:

  1. There exists τ > 0 such that svτ, for all v ∈ 𝓢𝓕;

  2. For each compact set 𝓦 ⊂ 𝓢𝓕 there exists C𝓦 > 0 such that svC𝓦, for all v ∈ 𝓦;

  3. The map m̂ : 𝓕 → 𝓝 given by m̂(v) = svv is continuous and m := |𝓢𝓕 is a homeomorphism between 𝓢𝓕 and 𝓝. Moreover, m−1(v) = v/∥v∥.

Proof

  1. Suppose that there exists {vn} ⊂ 𝓢𝓕 with sn := svn → 0. In this case, we get v H01 (Ω) with vnv in H01 (Ω). It follows from Lemma 2.1(ii) that

    1=λΩg(snvn)vndx(4/α2)λsnΩvn2dx. (2.2)

    By passing to the limit as n → ∞ in the last inequality, we get a contradiction.

  2. Let {vn} ⊂ 𝓦 be a sequence such that sn := svn → ∞. Since 𝓦 is compact, up to a subsequence, we get v ∈ 𝓦 such that vnv in H01 (Ω). Hence, passing to the lower limit as n → ∞ in

    1=vn2λ[v0]g(snvn)snvnvn2χ[vn0]dx,

    it follows from Lemma 2.1(ii) that

    v2=1(4λ/α2)Ωv2dx,

    showing that v ∈ 𝓕c. Since v ∈ 𝓦 ⊂ 𝓕, we have a contradiction.

  3. We are going to prove that is continuous. Let {vn} ⊂ 𝓕 and v ∈ 𝓕 be such that vnv in H01 (Ω). Since (sw) = (w) for all w ∈ 𝓕 and s > 0, we can assume that {vn} ⊂ S𝓕. Hence,

    sn=snvn2=λΩg(snvn)vndx, (2.3)

    where sn := svn. By (A1) and (A2), it follows that, passing to a subsequence, sns > 0. Thence, passing to the limit as n → ∞ in (2.3), we have

    s=sv2=λΩg(sv)vdx,

    showing that (vn) = snvnsv = (v). The second part of (A3) is immediate. □

Lemma 2.5

Suppose that ϑ satisfies (ϑ1) − (ϑ3). Then Iλ,4 is bounded from below in 𝓝.

Proof

By Lemma 2.1(iii), we get

Iλ,4(v)=λΩ12g(v)vG(v)dx0,vN. (2.4)

Therefore Iλ,4 is bounded from below in 𝓝. □

Now we are going to set the maps Ψ̂λ,4 : 𝓕 → ℝ and Ψλ,4 : 𝓢𝓕 → ℝ, by

Ψ^λ,4(u)=Iλ,4(m^(u))andΨλ,4:=(Ψ^λ,4)|SF.

Previous functions have important properties which will be stated in the next lemma. The proof is a direct consequence of Lemmas 2.3 and 2.4, see [24].

Lemma 2.6

Suppose that ϑ verifies (ϑ1) − (ϑ3). Then,

  1. Ψ̂λ,4C1(𝓕, ℝ) and

    Ψ^λ,4(u)v=m^(u)uIλ,4(m^(u))v,uFandvH01(Ω).
  2. Ψλ,4C1(𝓢𝓕, ℝ) and

    Ψλ,4(u)v=m(u)Iλ,4(m(u))v,vTuSF.
  3. If {un} is a (PS)c sequence for Ψλ,4 then {m(un)} is a (PS)c sequence for Iλ,4. If {un} ⊂ 𝓝 is a bounded (PS)c sequence for Iλ,4 then {m−1(un)} is a (PS)c sequence for Ψλ,4.

  4. u is a critical point of Ψλ,4 if, and only if, m(u) is a nontrivial critical point of Iλ,4. Moreover, the corresponding critical values coincide and

    infSFΨλ,4=infNIλ,4.

Proposition 2.7

Suppose that (ϑ1) − (ϑ3) hold. If {vn} ⊂ 𝓢𝓕 is such that dist(vn, 𝓢𝓕) → 0, then there exists v H01 (Ω) ∖ {0} such that vnv in H01 (Ω), svn → ∞ and

Ψλ,4(vn). (2.5)

Proof

Since {vn} ⊂ 𝓢𝓕 is bounded, up to a subsequence, there exists v H01 (Ω) with vnv in H01 (Ω). Since dist(vn, 𝓢𝓕) → 0, there exists {wn} ⊂ 𝓢𝓕 such that ∥vnwn∥ → 0 as n → ∞. Thus,

(4λ/α2)Ωvn2dx1=(4λ/α2)Ω(vn2wn2)dx(4λ/α2)|vn+wn|2|vnwn|2(8λ/α2λ1)vnwn.

Therefore,

(4λ/α2)Ωvn2dx1.

By using compact embedding from H01 (Ω) into L2(Ω), it follows that

1=(4λ/α2)Ωv2dx. (2.6)

Thus v ≠ 0. Suppose by contradiction that, for some subsequence, {svn} is bounded. In this case, passing again to a subsequence, there exists s0 > 0 (see Lemma 2.4(A1)) such that

svns0. (2.7)

It follows from (2.7) and

svn=λΩg(svnvn)vndx,

that

s0=λΩg(s0v)vdx.

Combining last equality and Lemma 2.1(ii), we obtain

1<(4λ/α2)Ωv2dx.

But this contradicts (2.6). Showing that svn → ∞. Finally, from svn → ∞, Lemma 2.1(iii) and Fatou Lemma, we get

lim infnΨλ,4(vn)=λlim infnΩ12g(svnvn)svnvnG(svnvn)dx.

Proposition 2.8

Suppose that (ϑ1) − (ϑ3) hold and λ > (α2/4)λ1. Then Ψλ,4 satisfies the (PS)c condition.

Proof

By Lemmas 2.4(A3) and 2.6(iii), it is sufficient to show that Iλ,4 satisfies the (PS)c condition. For this, let {wn} ⊂ 𝓝 be a (PS)c sequence for Iλ,4. We are going to prove that {wn} is bounded in H01 (Ω). Indeed, otherwise, up to a subsequence, we have ∥wn∥ → ∞. Define vn := wn/∥wn∥ = m−1(wn) ∈ 𝓢𝓕. Thus {vn} is bounded in H01 (Ω) and

Ψλ,4(vn)c. (2.8)

Consequently, there exists v H01 (Ω) such that

vnvinH01(Ω). (2.9)

Suppose by contradiction that v = 0. Since {Ψλ,4(vn)} is bounded, it follows that there exists C > 0 such that

C>Ψλ,4(vn)=Iλ,4(svnvn)Iλ,4(svn)=12λ[vn0]G(svn)(svn)2vn2dxs2,s>0. (2.10)

By Lemma 2.1(ii), L’Hôspital rule and compact embedding, passing to the limit as n → ∞ in (2.10), we get

C(1/2)s2,s>0,

a clear contradiction. Thereby, we conclude that v ≠ 0.

Since {wn} ⊂ 𝓝 is a (PS)c sequence for functional Iλ,4, we get

on(1)+Ωwnwdx=λΩg(wn)wdx,wH01(Ω).

Dividing last equality by ∥wn∥, we have

on(1)+Ωvnwdx=λ[vn0]g(wnvn)wnvnvnwdx.

Passing to the limit as n → ∞, it follows from Lemma 2.1(ii) that

Ωvwdx=(4λ/α2)Ωvwdx,wH01(Ω). (2.11)

Now we are going to consider two cases:

  1. If (4λ/α2) ≠ λj, whatever j > 1, it follows from (2.11) that v = 0. But this is a contradiction. Therefore {wn} is bounded in H01 (Ω).

  2. If (4λ/α2) = λj, for some j > 1, then (2.11) implies that v is an eigenfunction associated to λj. From (2.11), it follows also that ∥v2 = (4λ/α2)∫Ωv2dx, i.e., v𝓕. On the other hand,

    (4λ/α2)Ωv2dx=v2lim infnvn2=1.

Suppose that

v2=(4λ/α2)Ωv2dx<1. (2.12)

In this case, since

wn=svnvn=svn, (2.13)

passing to the limit as n → ∞ in

Ψλ,4(vn)=wn212λΩG(wnvn)(wnvn)2vn2dx

and using Lemma 2.1(ii), L’Hôspital rule and (2.12), we conclude that Ψλ,4(vn) → ∞, a contradiction with (2.8). Consequently,

v2=(4λ/α2)Ωv2dx=1, (2.14)

showing that v = ej and

vnv. (2.15)

By using (2.9) and (2.15), we derive vnv in H01 (Ω) with v𝓢𝓕 (see (2.14)). Invoking Proposition 2.7, we conclude that

Ψλ,4(vn). (2.16)

Since (2.16) cannot occurs, we conclude that {vn} is bounded.

Hence, there exists v H01 (Ω) such that vnv in H01 (Ω) up to a subsequence. Since vnv, to finish the proof we just have to prove that ∥vn∥ → ∥v∥. To this end, it is sufficient to note that since {vn} is a (PS)c sequence, we have

on(1)+Ωvnvdx=λΩg(vn)vdx.

Passing to the limit as n → ∞ in the previous equality, we get

v2=λΩg(v)vdx. (2.17)

Then (2.17) and Lebesgue’s convergence theorem imply that

vn2=λΩg(vn)vndx=λΩg(v)vdx+on(1)=v2+on(1).

The main result of this section will be proved through Krasnoselski’s genus theory. For this, we start defining some preliminaries notations:

yj:=BE:BSFandy(B)j,

where

E={BH01(Ω){0}:Bis closed andB=B}

and y : 𝓔 → ℤ ∪ {∞} is the Krasnoselski’s genus function, which is defined by

y(B)=n:=min{mN:there exists an odd mapφC(B,Rm{0})},,if there exists no mapφC(B,Rm{0}),0,ifB=. (2.18)

It is important to note that, since 𝓢𝓕 = −𝓢𝓕, yj is well defined.

Below we state some standard properties of the genus which can be found, for instance, in [18].

Lemma 2.9

Let B and C be sets in 𝓔.

  1. If x ≠ 0, then y({x} ∪ {− x}) = 1;

  2. If there exists an odd map φC(B, C), then y(B) ≤ y(C). In particular, if BC then y(B) ≤ y(C).

  3. If there exists an odd homeomorphism φ : BC, then y(B) = y(C). In particular, if B is homeomorphic to the unit sphere in Rn, then y(B) = n.

  4. If B is a compact set, then there exists a neighborhood K ∈ 𝓔 of B such that y(B) = y(K).

  5. If y(C) < ∞, then y(BC) ≥ y(B) − y(C).

  6. If y(A) ≥ 2, then A has infinitely many points.

Remember that, we have denoted by d(m) the sum of the dimensions of all eigenspaces Vλj associated to eigenvalues λj, where 1 ≤ jm.

Lemma 2.10

Suppose that (ϑ1) − (ϑ3) hold and λ > (α2/4)λm. Then,

  1. yd(m) ≠ ∅;

  2. y1y2 ⊃ … ⊃ yd(m);

  3. If φC(𝓢𝓕, 𝓢𝓕) and is odd, then φ(yj) ⊂ yj, for all 1 ≤ jd(m);

  4. If Byj and C ∈ 𝓔 with y(C) ≤ s < jd(m), then BCyjs.

Proof

(i) Let Sd(m) be the unit sphere of V1V2 ⊕ … ⊕ Vm. Since λ > (α2/4)λm, it is clear that Sd(m) ⊂ 𝓢𝓕. Moreover, by Lemma 2.9(iii), we have y(Sd(m)) = d(m). Showing that Sd(m)yd(m). (ii) It is immediate. (iii) It follows directly from Lemma 2.9(ii). (iv) It is a consequence of Lemma 2.9(v). □

Now, for each 1 ≤ jd(m), we define the following minimax levels

cj=infByjsupuBΨλ,4(u). (2.19)

Lemma 2.11

Suppose (ϑ1) − (ϑ3) hold. Then,

0c1c2cd(m)<.

Proof

First inequality follows from Lemma 2.5. On the other hand, the monotonicity of the levels cj is a consequence of Lemma 2.10(ii). □

Next proposition is crucial to ensure the existence of multiple solutions.

Proposition 2.12

Suppose that ϑ satisfies (ϑ1) − (ϑ3) and λ > (α2/4)λm. If cj = … = cj+pc, j + pd(m), then y(Kc) ≥ p + 1, where Kc := {v ∈ 𝓢𝓕 : Ψλ,4(v) = c and Ψλ,4 (v) = 0}.

Proof

Suppose that y(Kc) ≤ p. By Proposition 2.8 and Lemma 2.11, Kc is a compact set. Thus, by Lemma 2.9(iv), there exists a compact neighborhood K (in H01 (Ω)) of Kc such that y(K) ≤ p. Defining M := K ∩ 𝓢𝓕, we derive from Lemma 2.9(ii) that y(M) ≤ p. Despite the noncompleteness of 𝓢𝓕 we can still use Theorem 3.11 in [23] (see also Remark 3.12 in [23]) to ensure the existence of an odd homeomorphisms family η(., t) of 𝓢𝓕 such that, for each u ∈ 𝓢𝓕, the map

tΨλ,4(η(u,t))is non-increasing. (2.20)

Observe that, although 𝓢𝓕 is non-complete, from Proposition 2.7 and (2.20), for all u ∈ 𝓢𝓕, maps tη(u, t) are well defined in t ∈ [0, ∞). Consequently, it makes sense the third claim of Theorem 3.11 in [23], namely,

η((Ψλ,4)c+εM,1)(Ψλ,4)cε. (2.21)

Let us choose Byj+p such that supB Ψλ,4c + ε. From Lemma 2.10(iv), BMyj. It follows again from Lemma 2.10(iii) that η(BM, 1) ∈ yj. Therefore, from (2.21) and the definition of c, we have

csupη(BM¯,1)Ψλ,4cε,

that is a contradiction. Then y(Kc) ≥ p + 1. □

We are now ready to prove the following multiplicity result:

Proof of Theorem 1.2

(ii):

Note that 0 ≤ cj < ∞ are critical levels of Ψλ,4. In fact, suppose by contradiction that cj is regular for some j. Invoking Theorem 3.11 in [23], with β = cj, ε = 1, N = ∅, there exist ε > 0 and a family of odd homeomorphisms η(., t) satisfying the properties of referred theorem. Choosing Byj such that supB ψ < cj + ε and arguing as in the proof of Proposition 2.12 we get a contradiction.

Finally, if the levels cj, 1 ≤ jd(m), are different from each other, by Proposition 2.6(iv) the result is proved. On the other hand, if cj = cj+1c for some 1 ≤ jd(m), it follows from Proposition 2.12 that y(Kc) ≥ 2. Combining last inequality with Lemma 2.9(vi) and Proposition 2.6(iv), we conclude that (Pλ,q) has infinitely many pairs of nontrivial solutions. □

Acknowledgement

João R. Santos Júnior was partially supported by CNPq-Proc. 302698/2015-9 and CAPES-Proc. 88881.120045/2016-01, Brazil.

References

[1] A. V. Borovskii, and A. L. Galkin, Dynamical modulation of an ultrashort high-intensity laser pulse in matter, JETP, 77, (1993), 562-573.Search in Google Scholar

[2] H. S. Brandi, C. Manus, G. Mainfray, T. Lehner, and G. Bonnaud, Relativistic and ponderomotive self-focusing of a laser beam in a radially inhomogeneous plasma, Phys. Fluids B, 5, (1993), 3539-3550.10.1063/1.860828Search in Google Scholar

[3] X. L. Chen, and R. N. Sudan, Necessary and sufficient conditions for self-focusing of short ultraintense laser pulse, Phys. Rev. Lett., 70, (1993), 2082-2085.10.1103/PhysRevLett.70.2082Search in Google Scholar PubMed

[4] D. C. Clark, A variant of the Lusternik-Schnirelman theory, Indiana Univ. Math. J., 22, (1972), 65-74.10.1512/iumj.1973.22.22008Search in Google Scholar

[5] M. Colin and L. Jeanjean, Solutions for a quasilinear Schrödinger equations: A dual approach, Nonlinear Anal., 56, 213-226, (2004).10.1016/j.na.2003.09.008Search in Google Scholar

[6] A. De Bouard, N. Hayashi, and J. C. Saut, Global existence of small solutions to a relativistic nonlinear Schrödinger equation, Comm. Math. Phys., 189, (1997), 73-105.10.1007/s002200050191Search in Google Scholar

[7] Y. Deng, S. Peng, and S. Yan, Positive soliton solutions for generalized quasilinear Schrödinger equations with critical growth, J. Differential Equations, 258, (2015), 115-147.10.1016/j.jde.2014.09.006Search in Google Scholar

[8] J. M. do Ó, O. H. Miyagaki, and S. Soares, Soliton solutions for quasilinear Schrödinger equations: The critical exponential case, Nonlinear Anal., 67, (2007), 3357-3372.10.1016/j.na.2006.10.018Search in Google Scholar

[9] J. M. do Ó, O. H. Miyagaki, and S. Soares, Soliton solutions for quasilinear Schrödinger equations with critical growth, J. Differential Equations, 249, (2010), 722-744.10.1016/j.jde.2009.11.030Search in Google Scholar

[10] R. W. Hasse, A general method for the solution of nonlinear soliton and kink Schrödinger equations, Z. Phys., 37, (1980), 83-87.10.1007/BF01325508Search in Google Scholar

[11] S. Kurihura, Large-amplitude quasi-solitons in superfluid films, J. Phys. Soc. Jpn, 50, (1981) 3262-3267.10.1143/JPSJ.50.3262Search in Google Scholar

[12] E. W. Laedke, K. H. Spatschek, and L. Stenflo, Evolution theorem for a class of perturbed envelope soliton solutions, J. Math. Phys., 24, (1983), 2764-2769.10.1063/1.525675Search in Google Scholar

[13] A. G. Litvak, and A. M. Sergeev, One dimensional collapse of plasma waves, JETP Lett., 27, (1978), 517-520.Search in Google Scholar

[14] J. Q. Liu, Y. Q. Wang, and Z. Q. Wang, Soliton solutions for quasilinear Schrödinger equations II, J. Differential Equations, 187, (2003), 473-493.10.1016/S0022-0396(02)00064-5Search in Google Scholar

[15] V. G. Makhankov and V. K. Fedyanin, Non-linear effects in quasi-one-dimensional models of condensed matter theory, Phys. Rep., 104, (1984), 1-86.10.1016/0370-1573(84)90106-6Search in Google Scholar

[16] M. Poppenberg, K. Schmitt, and Z. Q. Wang, On the existence of soliton solutions to quasilinear Schrödinger equations, Calc. Var. Partial Differential Equations, 14, (3), (2002), 329-344.10.1007/s005260100105Search in Google Scholar

[17] G. R. W. Quispel, and H. W. Capel, Equation of motion for the Heisenberg spin chain, Physica A, 110, (1982), 41-80.10.1016/0378-4371(82)90104-2Search in Google Scholar

[18] P. H. Rabinowitz, Minimax Methods in Critical Point Theory with Applications to Differential Equations, CBMS Regional Conference Series in Mathematics 65, American Mathematical Society, Providence, RI, 1986.10.1090/cbms/065Search in Google Scholar

[19] A. V. Santos, J. R. Santos Júnior and A. Suárez, Study of a class of generalized Schrödinger equations, arXiv:1807.10529, accepted for publication in Journal Topological Methods in Nonlinear Analysis10.12775/TMNA.2020.008Search in Google Scholar

[20] Y. Shen, and Y. Wang, Soliton solutions for generalized quasilinear Schrödinger equations, Nonlinear Anal., 80, (2013)194-201.10.1016/j.na.2012.10.005Search in Google Scholar

[21] Y. Shen, and Y. Wang, A class of generalized quasilinear Schrödinger equations, Commun. Pure Appl. Anal., 15, (2016), 853-870.10.3934/cpaa.2016.15.853Search in Google Scholar

[22] E. A. B. Silva, G. F. Vieira, Quasilinear asymptotically periodic Schrödinger equations with critical growth, Calc. Var. Partial Differential Equations, 39, (2010), 1-33.10.1007/s00526-009-0299-1Search in Google Scholar

[23] M. Struwe, Variational Methods: Applications to Nonlinear Partial Differential Equations and Hamiltonian Systems. Springer, 2008.Search in Google Scholar

[24] A. Szulkin and T. Weth, The method of Nehari manifold, Handbook of Nonconvex Analysis and Applications. D.Y. Gao and D. Montreanu eds., International Press, Boston, 2010, 597-632.Search in Google Scholar

[25] J. Yang, Y. Wang, A. A. Abdelgadir, Soliton solutions for quasilinear Schrödinger equations, Journal of Mathematical Physics, 54, (2013), 071502.10.1063/1.4811394Search in Google Scholar

Received: 2019-04-14
Accepted: 2020-03-20
Published Online: 2020-08-22

© 2021 Amanda S. S. Correa Leão et al., published by De Gruyter

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

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