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Periodic solution for ϕ-Laplacian neutral differential equation

  • Shaowen Yao and Zhibo Cheng EMAIL logo
Published/Copyright: March 26, 2019

Abstract

This paper is devoted to the existence of a periodic solution for ϕ-Laplacian neutral differential equation as follows

(ϕ(x(t)cx(tτ)))=f(t,x(t),x(t)).

By applications of an extension of Mawhin’s continuous theorem due to Ge and Ren, we obtain that given equation has at least one periodic solution. Meanwhile, the approaches to estimate a priori bounds of periodic solutions are different from the corresponding ones of the known literature.

MSC 2010: 34C25; 34K14

1 Introduction

In this paper, we consider a kind of second order ϕ-Laplacian neutral differential equation as follows

(ϕ(x(t)cx(tτ)))=f(t,x(t),x(t)), (1.1)

where f : ℝ3 → ℝ is continuous function with f(t + T, ⋅, ⋅) ≡ f(t, ⋅, ⋅); c, τ are constants. ϕ : ℝ → ℝ is a continuous function and ϕ(0) = 0 which satisfies

(A1) (ϕ(x1) − ϕ(x2))(x1x2) > 0 for ∀ x1x2, x1, x2 ∈ ℝ;

(A2) There exists a function α : [0, +∞] → [0, +∞], α(s) → +∞ as s → +∞, such that ϕ(x) ⋅ xα(|x|)|x| for ∀ x ∈ ℝ.

It is easy to see that ϕ represents a large class of nonlinear operator, including ϕp : ℝ → ℝ is a p-Laplacian, i.e., ϕp(x) = |x|p−2x for x ∈ ℝ.

The study of p-Laplacian neutral differential equations began with the paper of Zhu and Lu. In 2007, Zhu and Lu [1] discussed the existence of a periodic solution for a kind of p-Laplacian neutral differential equation as follows

(ϕp(x(t)cx(tτ)))+g(t,x(tδ(t)))=p(t),

where c is a constant and |c| ≠ 1. Since (ϕp(x′(t)))′ is nonlinear (i.e. quasilinear), Mawhin’s continuous theorem [2] can not be apply directly. In order to get around this difficulty, Zhu and Lu translated the p-Laplacian neutral differential equation into a two-dimensional system

(x1(t)cx1(tτ))(t)=ϕq(x2(t))=|x2(t)|q2x2(t)x2(t)=g(t,x1(tδ(t)))+p(t),

where 1p+1q=1, for which Mawhin’s continuation theorem can be applied. Zhu and Lu’s work attracted the attention of many scholars in neutral differential equation and they have contributed to the research of p-Laplacian neutral differential equation (see [3]-[12]). Besides, a good deal of work has been performed on the existence of periodic solutions to ϕ-Laplacian differential equation. Manásevich and Mawhin [13] in 1998 investigated ϕ-Laplacian differential equation

(ϕ(x(t)))=f(t,x(t),x(t)).

Applying Leray-Schauder degree theory, the authors proved that the above equation has at least one periodic solution.

All the aforementioned results are related to p-Laplacian neutral equations [1], [3]-[12] or ϕ-Lpalacian differential equation [13]. Naturally, a new question arises: how neutral differential equation works on ϕ-Laplacian operator? Besides practical interests, the topic has obvious intrinsic theoretical significance. To answer this question, in this paper, we try to fill the gap and establish the existence of periodic solutions of (1.1) by employing the extension of Mawhin’s continuation theorem due to Ge and Ren. The obvious difficulty lies in the following two aspects. The first is that since the leading term contains a ϕ-Laplacian neutral operator, the operator is much more than the corresponding p-Laplacian neutral operator; the second is that a priori bounds of periodic solutions are not easy to estimate. For example, the key step for ϕp to get the priori bounds of periodic solution, 0T(ϕp(x(t)))x(t)dt=0T|x(t)|pdt, is no longer available for general ϕ-Laplacian. So we need to find a new method to solve that problem.

The remaining part of the paper is organized as follows. In section 2, we give some preliminary lemmas. In Section 3, by employing the extension of Mawhin’s continuation theorem, we state and prove the existence of periodic solution for (1.1) in |c| ≠ 1 and |c| = 1 (critical) cases. In Section 4, we investigate the existence of the result for a kind of ϕ-Laplacian neutral Liénard equation in |c| ≠ 1 case by applications of the Theorem 3.1. In Section 5, we consider the existence of periodic solution for a kind of p-Laplacian neutral Liénard equation in |c| ≠ 1 and |c| = 1 cases by applications of the Theorem 3.1. In Section 6, two numerical examples demonstrate the validity of the method.

Throughout this paper, we will denote by Z the set of integers, Z1 the set of odd integers, Z2 the set of even integers, N the set of positive integers, N1 the set of odd positive integers and N2 the set of even positive integers. Let CT := {x|xC(ℝ, ℝ), x(t + T) ’ x(t) ≡ 0, ∀ t ∈ ℝ}, CT1 := {x|xC(ℝ, ℝ), x(t + T) − x(t) ≡ 0, ∀ t ∈ ℝ}. L2π2 := {x : x(t + 2π) − x(t) ≡ 0, t ∈ ℝ and 02π |x(s)|2ds < +∞}, under the norm |φ|2 = 02π|φ(t)|2dt12,L2π2={x:xL2π2,x(t+π)+x(t)0} and L2π2+={x:xL2π2,x(t+π)x(t)0} with the norm |⋅|2. Clearly, L2π2,L2π2 and L2π2+ are all Banach spaces.

2 Preliminaries

In order to use the extension of Mawhin’s continuous theorem [14] due to Ge and Ren, we first recall it.

Let X and Z be Banach spaces with norms ∥ ⋅ ∥X and ∥ ⋅ ∥Y, respectively. A continuous operator M : X⋂dom MZ is said to be quasilinear if

  1. ImM := M(X⋂ domM) is a closed subset of Z;

  2. kerM := {xX⋂ domM : Mx = 0} is a subspace of X with dim ker M < +∞.

    Let X1 = kerM and X2 be the complement space of X1 in X, then X = X1X2. On the other hand, Z1 is a subspace of Z and Z2 is the complement space of Z1 in Z, so that Z = Z1Z2. Suppose that P : XX1 and Q : ZZ1 two projects and ΩX is an open and bounded set with the origin θΩ.

    Let Nλ : ΩZ, λ ∈ [0, 1] be a continuous operator. Denote N1 by N, and let ∑λ = {xΩ : Mx = Nλ x}. Nλ is said to be Mcompact in Ω if

  3. there is a vector subspace Z1 of Z with dimZ1 = dimX1 and an operator R : Ω × [0, 1] → X2 being continuous and compact such that for λ ∈ [0, 1],

    (IQ)Nλ(Ω¯)ImM(IQ)Z, (2.1)

    QNλx=0,λ(0,1)QNx=0, (2.2)

    R(,0)is the zero operator andR(,λ)|λ=(IP)|λ, (2.3)

    and

    M[P+R(,λ)]=(IQ)Nλ. (2.4)

    Let J : Z1X1 be a homeomorphism with J(θ) = θ.

Lemma 2.1

([14]) Let X and Z be Banach spaces with norm ∥⋅∥X and ∥⋅∥Y, respectively, and ΩX be an open and bounded set with origin θΩ. Suppose that M : X ∩ domMZ is a quasi – linear operator and

Nλ:Ω¯Z,λ(0,1)

is an M-compact mapping. In addition, if

  1. MxNλ x, λ ∈ (0, 1), x Ω,

  2. deg{JQN, Ω ∩ kerM, 0} ≠ 0,

where N = N1, then the abstract equation Mx = Nx has at least one solution in Ω.

Lemma 2.2

(see [15]) If |c| ≠ 1, then the operator (Ax)(t) := x(t) − cx(tτ) has a continuous inverse A−1 on the space CT, and satisfying

A11|1|c||.

Lemma 2.3

(see [16, 17]) The follow propositions are true:

  1. Suppose c = −1, |τ| = (m/n)π, where m, n are coprime positive integers with m even, then A : L2π2L2π2 , has a unique inverse A−1 : L2π2L2π2 satisfying

    A11σ1,

    where σ1:=infkN|1ceikτ|=infkN2(1+coskτ)12>0.

  2. Suppose c = −1, |τ| = (m/n)π, where m, n are coprime odd positive integers, then A : L2π2+L2π2+ , has a unique inverse A−1 : L2π2+L2π2+ satisfying

    A11σ2,

    where σ2:=infkN1|1ceikτ|=infkN12(1+coskτ)12>0.

  3. Suppose c = −1, |τ| = (m/n)π, where m, n are coprime positive integers with m odd and n even, then A : L2π2L2π2 , has a unique inverse A−1 : L2π2L2π2 satisfying

    A11σ3,

    where σ3:=infkN2|1ceikτ|=infkN22(1+coskτ)12>0.

  4. Suppose c = 1, |τ| = (m/n)π, where m, n are coprime positive integers with m odd, then A : L2π2L2π2 , has a unique inverse A−1 : L2π2L2π2 satisfying

    A11σ4,

    where σ4:=infkN1|1ceikτ|=infkN12(1+coskτ)12>0.

  5. Suppose c = 1, |τ| = π, then A : L2π2L2π2 , has a unique inverse A−1 : L2π2L2π2 satisfying

    A11σ5,

    where σ5:=infkN1|1ceikτ|=infkN12(1+coskτ)12=2>0.

3 Periodic solution for (1.1)

In this section, we will prove the existence of a periodic solution for ϕ-Laplacian neutral operator with |c| ≠ 1 and |c| = 1 by using Lemma 2.1.

Theorem 3.1

Assume that condition (A1), (A2) and |c| ≠ 1, Ω is an open bounded set in CT1 . Suppose the following conditions hold:

  1. For each λ ∈ (0, 1) the equation

    (ϕ(Ax)(t))=λf(t,x(t),x(t)) (3.1)

    has no solution on ∂Ω;

  2. The equation

    F(a):=1T0Tf(t,x(t),x(t))dt=0,

    has no solution on ∂Ω ∩ℝ;

  3. The Brouwer degree

    deg{F,ΩR,0}0.

Then (1.1) has at least one periodic solution on Ω.

Proof

In order to use Lemma 2.1 studying the existence of a periodic solution to (3.1), we set X := {xC[0, T] : x(0) = x(T)} and Z := C[0, T],

M:XdomMZ,(Mx)(t)=(ϕ(Ax)(t)), (3.2)

where dom M := {uX : ϕ(Au)′ ∈ C1(ℝ, ℝ)}. Then ker M = ℝ. In fact

kerM={xX:(ϕ(Ax)(t))=0}={xX:ϕ(Ax)c}={xX:(Ax)ϕ1(c):=c1}={xX:(Ax)(t)c1t+c2},

where c, c1, c2 are constant in ℝ. Since (Ax)(0) = (Ax)(T), then, we get ker M = {xX : (Ax)(t) ≡ c2}. In addition,

ImM={yZ,forxXdomM,(ϕ(x))(t)=y(t),0Ty(t)dt=0T(ϕ(x))(t)dt=0}.

So M is quasi-linear. Let

X1=kerM,X2={xX:x(0)=x(T)=0}.Z1=R,Z2=ImM.

Clearly, dim X1 = dim Z1 = 1, and X = X1X2, P : XX1, Q : ZZ1, are defined by

Px=x(0),Qy=1T0Ty(s)ds.

For ∀ ΩX define Nλ : ΩZ by

(Nλx)(t)=λf(t,x,x).

We claim (IQ)Nλ(Ω) ⊂ ImM = (IQ)Z holds. In fact, for xΩ, we have

0T(IQ)Nλx(t)dt=0T(IQ)λf(t,x(t),x(t))dt=0Tλf(t,x(t),x(t))dtλT0T0Tf(s,x(s),x(s))dsdt=0.

Hence, we have (IQ)Nλ(Ω) ⊂ Im M.

Moreover, for any xZ, we have

0T(IQ)x(t)dt=0Tx(t)1T0T0Tx(t)dtdt=0.

So, we have (IQ)Z ⊂ ImM. On the other hand, x ∈ ImM and 0T x(t)dt = 0, then we have x(t) = x(t) − 0T x(t)dt. Hence, we can get x(t) ∈ (IQ)Z. Therefore, ImM = (IQ)Z.

From QNλ x = 0, we can get λT0T f(t, x(t), x′(t))dt = 0. Since λ ∈ (0, 1), then we have 1T0T f(t, x(t), x′(t))dt = 0. Therefore, we can get QNx = 0, then, (2.4) also holds.

Let J : Z1X1, J(x) = x, then J(0) = 0. Define R : Ω × [0, 1] → X2, by Lemma 2.2, we know that there exists a continuous inverse operator A−1 of neutral operator A such that

R(x,λ)(t)=0tA1ϕ1a+0sλf(u,x(u),x(u))duλsT0Tf(u,x(u),x(u))duds, (3.3)

where aR is a constant such that

R(x,λ)(T)=0TA1ϕ1a+0sλf(u,x(u),x(u))duλsT0Tf(u,x(u),x(u))duds=0. (3.4)

From Lemma 2.3 of [13], we know that a is uniquely defined by

a=a~(x,λ),

where ã(x, λ) is continuous on Ω × [0, 1] and bounded sets of Ω × [0, 1] into bounded sets of ℝ.

From (3), we can find that

R:Ω¯×[0,1]X2.

Now, for any x ∈ ∑λ = {xΩ : Mx = Nλ x} = {xΩ : (ϕ(Ax)′(t))′ = λ f(t, x(t), x′(t))}, we have 0T f(t, x(t), x′(t))dt = 0, together with (3) gives

R(x,λ)(t)=0tA1ϕ1a+0sλf(u,x(u),x(u))duds=0tA1ϕ1a+0s(ϕ(Ax)(u))duds=0tA1ϕ1a+ϕ(Ax)(s)ϕ(Ax)(0)ds.

Take a = ϕ(Ax)’(0), from (Ax)′(t) = (Ax′)(t), then we can get

R(x,λ)(T)=0TA1(ϕ1(ϕ(Ax)(s)))ds=x(T)x(0)=0,

where a is unique, we see that

a=a~(x,λ)=ϕ(Ax)(0),λ[0,1].

So, we have

R(x,λ)(t)|xλ=0tA1ϕ1ϕ(Ax)(0)+0sλf(t,u,x(u),x(u))duds=0tA1ϕ1(ϕ(Ax)(s))ds=x(t)x(0)=(IP)x(t),

which yields the second part of (2.4). Meanwhile, if λ = 0, the

λ={xΩ¯:Mx=Nλx}={xΩ¯:(ϕ(Ax)(t))=λf(t,x(t),x(t))}=c3,

where c3 ∈ ℝ is a constant, so by the continuity of ã(x, λ) with respect to (x, λ), a = ã(x, 0) = ϕ(Ac)′(0) = θ. So,

R(x,0)(t)=0tA1ϕ1(θ)ds=0,xΩ¯,

which yields the first part of (2.4). Furthermore, we consider the following equation

M(P+R)=(IQ)Nλ.

In fact,

ddtϕ(A(P+R))=(IQ)Nλ. (3.5)

Integrating both sides of (3.5) over [0, s], we have

0sddtϕ(A(P+R))ds=0s(IQ)Nλds.

Therefore, we have

ϕ(A(P+R))(s)a=λ0sf(u,x(u),x(u))du0sλT0Tf(u,x(u),x(u))dudt=0sf(u,x(u),x(u))duλsT0Tf(u,x(u),x(u))du,

where a := ϕ(A(P + R))′(0). Then, we can get

(A(P+R))(s)=ϕ1a+λ0sf(u,x(u),x(u))duλsT0Tf(u,x(u),x(u))du.

Then, we have

(P+R)(s)=A1ϕ1a+λ0sf(u,x(u),x(u))duλsT0Tf(u,x(u),x(u))du,

since (A(P + R))′(s) = A(P + R)′(s). Hence, we have

R(x,λ)(t)R(x,λ)(0)=0tA1ϕ1a+λ0sf(u,x(u),x(u))duλsT0Tf(u,x(u),x(u))duds,

since R(x, λ)(0) = 0. So, we can get

R(x,λ)(t)=0tA1ϕ1a+λ0sf(u,x(u),x(u))duλsT0Tf(u,x(u),x(u))duds.

Thus, Nλ is M-compact on Ω. Obviously, the equation

(ϕ(Ax)(t))=λf(t,x(t),x(t))

can be converted to

Mx=Nλx,λ(0,1),

where M and Nλ are defined by (3.2) and (3), respectively. As proved above,

Nλ:Ω¯Z,λ(0,1)

is an M-compact mapping. From assumption (C1), one find

MxNλx,λ(0,1),xΩ,

and assumptions (C2) and (C3) imply that deg{JQN, Ω ∩ kerM, θ} is valid and

deg{JQN,ΩkerM,θ}0.

So by applications of Lemma 2.1, we see that (3.1) has a T-periodic solution. □

In the following, applying Lemma 2.3 and Theorem 3.1, we consider the existence of a periodic solution to (1.1) in the case that |c| = 1.

Theorem 3.2

Assume that conditions (A1), (A2) (C1), (C2) and (C3) hold, Ω is an open bounded set in C2π1. Furthermore, suppose one of the following conditions holds:

  1. c = −1 and |τ| = (m/n)π, with m, n are coprime positive integers with m even;

  2. c = −1 and |τ| = (m/n)π, with m, n are coprime odd positive integers;

  3. c = −1 and |τ| = (m/n)π, with m, n are coprime positive integers with m odd and n even;

  4. c = 1 and |τ| = (m/n)π, with m, n are coprime positive integers with m odd;

  5. c = 1 and |τ| = π.

Then (1.1) has at least one periodic solution on Ω.

Proof

We follow the same strategy and notation as in the proof of Theorem 3.1. Next, we consider R(x, λ)(t).

Case (i) c = −1 and |τ| = (m/n)π, with m, n are coprime positive integers with m even. Take T = 2π, from (3.3) and (3.4), applying Lemma 2.3, we know that there exist a continuous inverse operator A−1 of neutral operator A in the case that c = −1 such that

R(x,λ)(t)=0tA1ϕ1a+0sλf(u,x(u),x(u))duλs2π02πf(u,x(u),x(u))duds,

where aR is a constant such that

R(x,λ)(2π)=02πA1ϕ1a+0sλf(u,x(u),x(u))duλs2π02πf(u,x(u),x(u))duds=0.

Similarly, we can get Case (ii)-Case (v). This proves the claim and the rest of the proof of the theorem is identical to that of Theorem 3.1. □

4 Application of Theorem 3.1: ϕ-Laplacian operator

As an application, we consider the following ϕ-Laplacian neutral Liénard equation

(ϕ(Ax)(t))+f(x(t))x(t)+g(t,x(t))=e(t), (4.1)

where g is a continuous function defined on ℝ2 and periodic in t with g(t, ⋅) = g(t + T, ⋅), fC(ℝ, ℝ), e is a continuous periodic function defined on ℝ with period T and 0T e(t) dt = 0. Next, by applications of Theorem 3.1, we investigate the existence of a periodic solution for (4.1) in the case that |c| ≠ 1.

Theorem 4.1

Suppose |c| ≠1, (A1) and (A2) hold. Assume that the following conditions hold:

  1. There exists a constant D > 0 such that

    xg(t,x)>0,(t,x)[0,T]×R,with|x|>D.
  2. There exist two positive constants σ*, σ* such that σ* ≤ |f(x(t))| ≤ σ*, ∀ t ∈ ℝ.

  3. There exist positive constants a, b, B such that

    |g(t,x(t))|a|x(t)|+b,for|x(t)|>BandtR.

Then (4.1) has at least one solution with period T if σσ|c|+22(1+|c|)aT>0.

Proof

Consider the homotopic equation

(ϕ(Ax)(t))+λf(x(t))x(t)+λg(t,x(t))=λe(t). (4.2)

Firstly, we will claim that the set of all T-periodic solutions of (4.2) is bounded. Let x(t) ∈ CT1 be an arbitrary T-periodic solution of (4.2). As (Ax)(0) = (Ax)(T), there exists a point t0 ∈ (0, T) such that (Ax)′(t0) = 0, while ϕ(0) = 0, and we see

|ϕ(Ax)(t)|=t0t(ϕ(Ax)(s))ds=λ0T|f(x(t))||x(t)|dt+λ0T|g(t,x(t))|dt+λ0T|e(t)|dt. (4.3)

Integrating both sides of (4.2) over [0, T], we have

0Tg(t,x(t))dt=0. (4.4)

From the mean value theorem, there is a constant ξ ∈ (0, T) such that

g(ξ,x(ξ))=0.

In view of (H1), we obtain

|x(ξ)|D.

Then, we have

x=maxt[0,T]|x(t)|=maxt[ξ,ξ+T]|x(t)|=12maxt[ξ,ξ+T]|x(t)|+|x(tT)|=12maxt[ξ,ξ+T]x(ξ)+ξTx(s)ds+x(ξ)tTξx(s)dsD+12ξt|x(s)|ds+tTξ|x(s)|dsD+120T|x(s)|ds. (4.5)

Multiplying both sides of (4.2) by (Ax)′(t) and integrating over the interval [0, T], we get

0T(ϕ(Ax)(t))(Ax)(t)dt+λ0Tf(x(t))x(t)(Ax)(t)dt+λ0Tg(t,x(t))(Ax)(t)dt=λ0Te(t)(Ax)(t)dt. (4.6)

Substituting 0T (ϕ(Ax)′(t))′(Ax)′(t)dt = 0, 0T f(x(t))x′(t)(Ax)′(t)dt = 0T f(x(t))(x′(t))2dtc 0T f(x(t))x′(t)x′(tτ))dt

0Tf(x(t))|x(t)|2dt=c0Tf(x(t))x(t)x(tτ)dt0Tg(t,x(t))(Ax)(t)dt+0Te(t)(Ax)(t)dt.

Therefore, we have

0Tf(x(t))|x(t)|2dt=c0Tf(x(t))x(t)x(tτ)dt0Tg(t,x(t))(Ax)(t)dt+0Te(t)(Ax)(t)dt.

From (H2), we have

0Tf(x(t))|x(t)|2d=0T|f(x(t))||x(t)|2dtσ0T|x(t)|2dt.

So, we have

σ0T|x(t)|2dt|c|0T|f(x(t))||x(t)||x(tτ)|dt+0T|g(t,x(t))||x(t)|dt+|c|0T|g(t,x(t))||x(tτ)|dt+0T|e(t)||x(t)|dt+|c|0T|e(t)||x(tτ)|dt.

Define

E1:={t[0,T]||x(t)|B},E2:={t[0,T]||x(t)|>B}.

From (H2) and the Hölder inequality, we have

σ0T|x(t)|2dt|c|σ0T|x(t)||x(tτ)|dt+E1+E2|g(t,x(t))||x(t)|dt+|c|E1+E2|g(t,x(t))||x(tτ)|dt+e0T|x(t)|dt+|c|e0T|x(tτ)|dt|c|σ0T|x(t)|2dt120T|x(tτ)|2dt12+E1|g(t,x(t))||x(t)|dt+E2|g(t,x(t))||x(t)|dt+|c|E1|g(t,x(t))||x(tτ)|dt+|c|E2|g(t,x(t))||x(tτ)|dt+e0T|x(t)|dt+|c|e0T|x(tτ)|dt (4.7)

where e:=maxt[0,T]|e(t)|. Substituting 0T |x′(tτ)|dt = 0T |x′(t)|dt into (4.7), and by applications of condition (H3), we have

σ0T|x(t)|2dt|c|σ0T|x(t)|2dt+(1+|c|)gB0T|x(t)|dt+E2|g(t,x(t))||x(t)|dt+|c|E2|g(t,x(t))||x(tτ)|dt+(1+|c|)e0T|x(t)|dt|c|σ0T|x(t)|2dt+(1+|c|)gBT120T|x(t)|dt12+a0T|x(t)||x(t)|dt+b0T|x(t)|dt+a|c|0T|x(t)||x(tτ)|dt+b|c|0T|x(tτ)|dt+(1+|c|)eT120T|x(t)|dt12|c|σ0T|x(t)|2dt+a0T|x(t)|dt120T|x(t)|dt12+a|c|0T|x(t)|dt120T|x(tτ)|dt12+(1+|c|)gBT120T|x(t)|dt12+(1+|c|)bT120T|x(t)|dt12+(1+|c|)eT120T|x(t)|dt12=|c|σ0T|x(t)|2dt+(1+|c|)a0T|x(t)|dt120T|x(t)|dt12+N10T|x(t)|dt12|c|σ0T|x(t)|2dt+(1+|c|)aT12x120T|x(t)|dt12+N10T|x(t)|dt12 (4.8)

where ∥gB∥ := max|x(t)|B |g(t, x(t))| and N1:=(1+|c|)(|gB|+b+e)T12. Substituting (4.5) into (4.8), we have

σ0T|x(t)|2dt|c|σ0T|x(t)|2dt+(1+|c|)aT12D+120T|x(t)|dt120T|x(t)|dt12+N10T|x(t)|dt12|c|σ0T|x(t)|2dt+22(1+|c|)aT0T|x(t)|2dt+(1+|c|)a(TD)12+N10T|x(t)|dt12 (4.9)

since (a + b)kak + bk, 0 < k < 1. From (4.9), we can get

σ0T|x(t)|2dt|c|σ+22(1+|c|)aT0T|x(t)|2dt+(1+|c|)a(TD)12+N10T|x(t)|dt12.

Since σσ|c|+22(1+|c|)aT>0, it is easy to see that there exists a constant M1 > 0 (independent of λ) such that

0T|x(t)|2dtM1. (4.10)

From (4.5) and the Hölder inequality, we have

xD+120T|x(s)|dsD+12T120T|x(s)|2ds12D+12T12M112:=M1. (4.11)

From (4.3), (4.10) and (4.11), we see that

|ϕ(Ax)(t)|=t0t(ϕ(Ax)(s))dsλ0T|f(x(t))||x(t)|dt+λ0Tg(t,x(t))|dt+λ0T|e(t)|dtfM1T120T|x(t)|2dt12+TgM1+TefM1T12M112+TgM1+Te:=M2,

where fM1:=max|x(t)|M1|f(x(t))|.

We claim that there exists a positive constant M2>M2+1 such that, for all t ∈ ℝ, we have

(Ax)M2. (4.12)

In fact, if (Ax)′(t) is not bounded, then from the definition of α, there exists a positive constant M2 such that α(|(Ax)′|) > M2 for all (Ax)′ ∈ ℝ. However, from (A2), we have

α(|(Ax)|)|(Ax)|ϕ((Ax))(Ax)|ϕ(Ax)||(Ax)|M2|(Ax)|.

Then, we can get

α(|(Ax)|)M2,for all(Ax)R,

which is a contradiction. So, (4.12) holds.

By Lemma 2.2 and (4.12), we have

x=A1Ax=A1(Ax)(Ax)|1|c||M2|1|c||:=M2. (4.13)

Set M=M12+M22+1, we have

Ω={xCT1(R,R)|xM+1,xM+1},

and we know that (4.1) has no solution on ∂Ω as λ ∈ (0, 1) and when x(t) ∈ ∂Ω ∩ ℝ, x(t) = M + 1 or x(t) = –M – 1, from (4.5) we know that M + 1 > D. So, from (H1), we see that

1T0Tg(t,M+1)dt<0,1T0Tg(t,M1)dt>0,

since 0T e(t)dt = 0. So condition (C2) of Theorem 3.1 is also satisfied. Set

H(x,μ)=μx+(1μ)1T0Tg(t,x))dt,xΩR,μ[0,1]

Obviously, from (H1), we can get xH(x, μ) > 0 and thus H(x, μ) is a homotopic transformation and

deg{F,ΩR,0}=deg{1T0Tg(t,x)dt,ΩR,0}=deg{x,ΩR,0}0.

So condition (C3) of Theorem 3.1 is satisfied. In view of the Theorem 3.1, there exists a solution with period T.□

Remark 4.1

When |c| = 1, from Theorem 4.1, we know that σ* – (σ* + 2 aT) > 0 does not hold. Therefore, by applications of the above method, we do not obtain the existence of periodic solution for (4.1) in critical case (|c| = 1).

5 Application of Theorem 3.1: p-Laplacian operator

When (ϕ(Ax)′(t))′ ≡ (ϕp(Ax)′(t))′, then (4.1) is rewritten

(ϕp(Ax)(t))+f(x(t))x(t)+g(t,x(t))=e(t). (5.1)

Firstly, we consider the existence of a periodic solution for (5.1) in the case that |c| ≠ 1 by applications of Theorem 3.1.

Theorem 5.1

Suppose |c| ≠ 1 and condition (H1) hold. Assume that the following conditions hold:

  1. There exist positive constants α, β such that |f(x(t))| ≤ α |x(t)|p−2 + β, ∀ t ∈ ℝ.

  2. There exist positive constants γ, η, B* such that

    |g(t,x(t))|γ|x(t)|p1+η,for|x(t)|>BandtR.

Then (5.1) has at least one solution with period T if 12p1|c|α+12p(1+|c|)γT<|1|c||pTpq .

Proof

Consider the homotopic equation

(ϕp(Ax)(t))+λf(x(t)x(t)+λg(t,x(t))=λe(t). (5.2)

We follow the same strategy and notation as in the proof of Theorem 4.1. From (H1), we know that there exists a constant D > 0 such that

|x(t)|D+120T|x(t)|dt. (5.3)

Multiplying both sides of (5.2) by (Ax)(t) and integrating over the interval [0, T], we get

0T(ϕp(Ax)(t))(Ax)(t)dt+λ0Tf(x(t))x(t)(Ax)(t)dt+λ0Tg(t,x(t))(Ax)(t)dt=λ0Te(t)dt. (5.4)

Substituting 0T(ϕp(Ax)(t))(Ax)(t)dt=0T|(Ax)(t)|pdtand0Tf(x(t))x(t)x(t)dt=0 into (5.4), we have

0T|(Ax)(t)|pdt=λc0Tf(x(t))x(t)x(tτ)dt+λ0Tg(t,x(t))(x(t)cx(tτ))dtλ0Te(t)(x(t)x(tτ))dt.

Then, we can get

0T|(Ax)(t)|pdt|c|x0T|f(x(t))||x(t)|dt+(1+|c|)x0T|g(t,x(t))|dt+(1+|c|)0T|e(t)|dt.

Define

E3:={t[0,T]||x(t)|B},E4:={t[0,T]||x(t)|>B}.

From (H3) and (H4), we have

0T|(Ax)(t)|pdt|c|αx0T|x(t)|p2|x(t)|dt+|c|βx0T|x(t)|dt+(1+|c|)xE3+E4|g(t,x(t))|dt+(1+|c|)xeT|c|αx0T|x(t)|p2|x(t)|dt+|c|βx0T|x(t)|dt+(1+|c|)xgE3T+(1+|c|)γx0T|x(t)|p1dt+(1+|c|)ηTx+(1+|c|)xeT|c|αxp10T|x(t)|dt+|c|βx0T|x(t)|dt+(1+|c|)γTxp+(1+|c|)T(gE3+η+e)x, (5.5)

where gE3:=max|x(t)|B|g(t,x(t))| . Substituting (5.3) into (5.4), we have

0T|(Ax)(t)|pdt|c|αD+120T|x(t)|dtp10T|x(t)|dt+|c|βD+120T|x(t)|dt0T|x(t)|dt+(1+|c|)γTD+120T|x(t)|dtp+(1+|c|)T(gE3+η+e)D+120T|x(t)|dt=|c|α2D0T|x(t)|dt+1p112p10T|x(t)|dtp+|c|βD+120T|x(t)|dt0T|x(t)|dt+(1+|c|)γT2D0T|x(t)|dt+1p12p0T|x(t)|dtp+(1+|c|)T(gE3+η+e)D+120T|x(t)|dt|c|α1+2Dp0T|x(t)|dt12p10T|x(t)|dtp+|c|βD+120T|x(t)|dt0T|x(t)|dt+(1+|c|)γT1+2D(p+1)0T|x(t)|dt12p0T|x(t)|dtp+(1+|c|)T(gE3+η+e)D+120T|x(t)|dt,

since (1 + x)p ≤ 1 + (1 + p)x for x ∈ [0, δ], here δ is a given positive constant, which is only dependent on k > 0. Therefore, we have

0T|(Ax)(t)|pdt12p1|c|α0T|x(t)|dtp+12p2|c|αDp0T|x(t)|dtp1+12p(1+|c|)γT0T|x(t)|dtp+12p1(1+|c|)γTD(p+1)0T|x(t)|dtp1+12|c|β0T|x(t)|dt2+N30T|x(t)|dt+N4=12p1|c|α+12p(1+|c|)γT0T|x(t)|dtp+12p2|c|αDp+12p1(1+|c|)mTD(p+1)0T|x(t)|dtp1+12|c|β0T|x(t)|dt2+N30T|x(t)|dt+N4. (5.6)

where N3 = |c|β D + 12 (1 + |c|)T(η + |gM3| + |e|), N4 = (1 + |c|)TD(η + |gM3| + |e|). By application of Lemma 2.2, we have

0T|x(t)|dt=0T|(A1Ax)(t)|dt0T|(Ax)(t)|dt|1|c||T1q0T|(Ax)(t)|pdt1p|1|c||, (5.7)

since (Ax′)(t) = (Ax)′(t) and 1p+1q = 1. Applying the inequality

(a+b)kak+bk,fora,b>0,0<k<1.

Substituting (5.5) into (5.6), we have

0T|x(t)|dtT1q12p1|c|α+12p(1+|c|)γT1p0T|x(t)|dt|1|c||+T1q12p2|c|αDp+12p1(1+|c|)γTD(p+1)1p0T|x(t)|dtp1p|1|c||+T1q12|c|β1p0T|x(t)|dt2p+N31p0T|x(t)|dt1p+N41p|1|c||.

Since 12p1|c|α+12p(1+|c|)γT<|1|c||pTpq , it is easy to see that there exists a positive constant M1 such that

0T|x(t)|dtM1. (5.8)

From (5.3) and (5.7), we have

xD+120ω|x(t)|dtD+12M1:=M1. (5.9)

As (Ax)(0) = (Ax)(T), there exists t1 ∈ [0, T] such that (Ax)′(t1) = 0, while ϕp(0) = 0, we have

|ϕp((Ax)(t))|=t1t(ϕp((Ax)(s)))dsλ0T|f(x(t))||x(t)|dt+λ0T|g(t,x(t))|dt+λ0T|e(t)|dt, (5.10)

where t ∈ [t1, t1 + T]. In view of (H5), (5.7), (5.8) and (5.9), we have

ϕp(Ax)=maxt[0,T]{ϕp((Ax)(t))}=maxt[t1,t1+T]t1t(ϕp((Ax)(s)))dsλ0T|f(x(t)||x(t)|dt+0T|g(t,x(t))|dt+0T|e(t)|dtfM1M1+γM1p1+ηT+Te:=λM2, (5.11)

where fM1:=max|x|M1|f(x(t)| .

We claim that there exists a positive constant M2 > M2 + 1 such that, for all t ∈ ℝ

xM2. (5.12)

In fact, if x′ is not bounded, there exists a positive constant M2 such that |x′| > M2 for some x′ ∈ ℝ. Therefore, we have

ϕp(Ax)=ϕp(Ax)=Axp1=(1+|c|)p1xp1(1+|c|)p1M2p1:=M2.

Then, it is a contradiction. So, (5.12) holds.

This proves the claim and the rest of the proof of the theorem is identical to that of Theorem 4.1.□

Remark 5.1

Obviously, the conditions (H4) and (H5) are weaken than the conditions (H2) and (H3). Moreover, by using the method of Theorem 5.1, we can investigate (5.1) in critical case |c| = 1.

Next, we discuss the existence of periodic solution for (5.1) in critical case |c| = 1 by using Theorem 3.1.

Theorem 5.2

Suppose conditions (H1), (H4), (H5) and |c| = 1 hold. Then (5.1) has at least one solution with period T, if one of the following conditions holds:

  1. c = -1 and |τ| = (m/n)π, with m, n are coprime positive integers with m even, and 12p1(α+γT)<σ1pTpq;

  2. c = −1 and |τ| = (m/n)π, with m, n are coprime odd positive integers, and 12p1(α+γT)<σ2pTpq;

  3. c = −1 and |τ| = (m/n)π, with m, n are coprime positive integers with m odd and n even, and 12p1(α+γT)<σ3pTpq;

  4. c = 1 and |τ| = (m/n)π, with m, n are coprime positive integers with m odd, and 12p1(α+γT)<σ4pTpq;

  5. c = 1 and |τ| = π, and 12p1(α+γT)<σ5pTpq.

Proof

We follow the same strategy and notation as in the proof of Theorem 5.1. Next, we consider that there exists a positive constant M1 such that

0T|x(t)|dtM1.

Case (i). If c = −1 and |τ| = (m/n)π, with m, n are coprime positive integers with m even. From (5.7) and Lemma 2.3, we have

0T|x(t)|dt=0T|(A1Ax)(t)|dt0T|(Ax)(t)|dtσ1T1q0T|(Ax)(t)|pdt1pσ1. (5.13)

Substituting (5.6) into (5.13), we have

0T|x(t)|dtT1q12p1α+12p1γT1p0T|x(t)|dtσ1+T1q12p2αDp+12p2γTD(p+1)1p0T|x(t)|dtp1pσ1+T1q12β1p0T|x(t)|dt2p+N51p0T|x(t)|dt1p+N61pσ1,

where N5 = β D + T(η + ∥gM3∥ + ∥e∥), N6 = 2TD(η + ∥gM3∥ + ∥e∥). Since α+γT<2p1σ1pTpq, it is easy to see that there exists a positive constant M1 such that

0T|x(t)|dtM1.

Similarly, we can get Case (ii)-Case (v). This proves the claim and the rest of the proof of the theorem is identical to that of Theorem 5.1. □

6 Examples

Example 6.1

Consider the following ϕ-Laplacian Liénard equation:

(ϕ(x(t)110x(tτ)))+(cosx+3)x(t)+110(cos2t+1)x(tσ)=sin2t, (6.1)

where relativistic operator ϕ(u)=u1|u|c2, here c* is the speed of light in the vacuum and c* > 0, τ, σ are constants and 0 ≤ τ, σ < T.

Comparing (6.1) to (4.1), it is easy to see that f(x) = cos x + 3, g(t, x) = 110 (cos2t + 2)x, e(t) = sin 2t, T = π, c = 110 . Obviously, we get

u1|u|c2v1|v|c2(uv)0,

and

ϕ(u)u=|u|21|u|c2.

So, the conditions (A1) and (A2) hold. Moreover, it is easy to see that there exists a constant D = 1 such that (H1) holds. 2 ≤|f(x)| = |cos x + 3| ≤ 4, here σ* = 2, σ* = 4, condition (H2) holds. Consider |g(t, x)| = | 110 (cos 2t + 2)x| ≤ 310 |x| + 1, here a = 310 , b = 1. So, condition (H3) is satisfied. Next, we consider the condition

σ(|c|σ+22(1+|c|)aT)=2110×4+221+110×310×π=225+332π200>0.

Therefore, by Theorem 4.1, we know that (6.1) has at least one positive π-periodic solution.

Example 6.2

Consider the p-Laplacian neutral Liénard equation:

(ϕp(x(t)11x(tτ)))+(x4+3)x(t)+(5+sint)x5(tσ)=cost, (6.2)

where p = 6, τ, σ are constants and 0 ≤ τ, σ < T.

It is clear that T = 2π, g(t, x) = (5 + sin t)x5(tσ), f(x) = x4 + 3, e(t) = cos t. It is obvious that there exists a constant D = 1 such that (H1) holds. |f(x)| = |x4 + 3| ≤|x|4 + 5, here α = 1, β = 5, condition (H4) holds. Consider |g(t, x)| = |(5 + sin t)x5| ≤ 6|x|5 + 1, here γ = 6, η = 1. So, condition (H3) is satisfied. Next, we consider the condition

Tpq12p1|c|α+12p(1+|c|)γT|1|c||p=(2π)5125×11+126×(1+11)×6×2π106723431000000<1.

Therefore, by applications of Theorem 5.1, we know that (6.2) has at least one positive periodic solution.

  1. Competing interests: The authors declare that they have no competing interests concerning the publication of this manuscript.

  2. Author’s contributions: The authors contributed equally and significantly in writing this article. Both authors read and approved the final manuscript.

Acknowledgement

This work was supported by National Natural Science Foundation of China (11501170), China Postdoctoral Science Foundation funded project (2016M590886), Fundamental Research Funds for the Universities of Henan Provience (NSFRF170302) and Education Department of Henan Province project (16B110006).

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Received: 2018-09-05
Accepted: 2019-01-29
Published Online: 2019-03-26

© 2019 Yao and Cheng, published by De Gruyter

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

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  92. Non-trivial solutions for Schrödinger-Poisson systems involving critical nonlocal term and potential vanishing at infinity
  93. Characterizations of Benson proper efficiency of set-valued optimization in real linear spaces
  94. A quantitative obstruction to collapsing surfaces
  95. Dynamic behaviors of a Lotka-Volterra type predator-prey system with Allee effect on the predator species and density dependent birth rate on the prey species
  96. Coexistence for a kind of stochastic three-species competitive models
  97. Algebraic and qualitative remarks about the family yy′ = (αxm+k–1 + βxmk–1)y + γx2m–2k–1
  98. On the two-term exponential sums and character sums of polynomials
  99. F-biharmonic maps into general Riemannian manifolds
  100. Embeddings of harmonic mixed norm spaces on smoothly bounded domains in ℝn
  101. Asymptotic behavior for non-autonomous stochastic plate equation on unbounded domains
  102. Power graphs and exchange property for resolving sets
  103. On nearly Hurewicz spaces
  104. Least eigenvalue of the connected graphs whose complements are cacti
  105. Determinants of two kinds of matrices whose elements involve sine functions
  106. A characterization of translational hulls of a strongly right type B semigroup
  107. Common fixed point results for two families of multivalued A–dominated contractive mappings on closed ball with applications
  108. Lp estimates for maximal functions along surfaces of revolution on product spaces
  109. Path-induced closure operators on graphs for defining digital Jordan surfaces
  110. Irreducible modules with highest weight vectors over modular Witt and special Lie superalgebras
  111. Existence of periodic solutions with prescribed minimal period of a 2nth-order discrete system
  112. Injective hulls of many-sorted ordered algebras
  113. Random uniform exponential attractor for stochastic non-autonomous reaction-diffusion equation with multiplicative noise in ℝ3
  114. Global properties of virus dynamics with B-cell impairment
  115. The monotonicity of ratios involving arc tangent function with applications
  116. A family of Cantorvals
  117. An asymptotic property of branching-type overloaded polling networks
  118. Almost periodic solutions of a commensalism system with Michaelis-Menten type harvesting on time scales
  119. Explicit order 3/2 Runge-Kutta method for numerical solutions of stochastic differential equations by using Itô-Taylor expansion
  120. L-fuzzy ideals and L-fuzzy subalgebras of Novikov algebras
  121. L-topological-convex spaces generated by L-convex bases
  122. An optimal fourth-order family of modified Cauchy methods for finding solutions of nonlinear equations and their dynamical behavior
  123. New error bounds for linear complementarity problems of Σ-SDD matrices and SB-matrices
  124. Hankel determinant of order three for familiar subsets of analytic functions related with sine function
  125. On some automorphic properties of Galois traces of class invariants from generalized Weber functions of level 5
  126. Results on existence for generalized nD Navier-Stokes equations
  127. Regular Banach space net and abstract-valued Orlicz space of range-varying type
  128. Some properties of pre-quasi operator ideal of type generalized Cesáro sequence space defined by weighted means
  129. On a new convergence in topological spaces
  130. On a fixed point theorem with application to functional equations
  131. Coupled system of a fractional order differential equations with weighted initial conditions
  132. Rough quotient in topological rough sets
  133. Split Hausdorff internal topologies on posets
  134. A preconditioned AOR iterative scheme for systems of linear equations with L-matrics
  135. New handy and accurate approximation for the Gaussian integrals with applications to science and engineering
  136. Special Issue on Graph Theory (GWGT 2019)
  137. The general position problem and strong resolving graphs
  138. Connected domination game played on Cartesian products
  139. On minimum algebraic connectivity of graphs whose complements are bicyclic
  140. A novel method to construct NSSD molecular graphs
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