• Nem Talált Eredményt

The study of higher-order resonant and non-resonant boundary value problems

N/A
N/A
Protected

Academic year: 2022

Ossza meg "The study of higher-order resonant and non-resonant boundary value problems"

Copied!
10
0
0

Teljes szövegt

(1)

The study of higher-order resonant and non-resonant boundary value problems

Aijun Yang

B1

, Johnny Henderson

2

and Dingjiang Wang

1

1College of Science, Zhejiang University of Technology, Hangzhou, 310023, China

2Department of Mathematics, Baylor University, Waco, Texas, 76798-7328, USA

Received 14 October 2015, appeared 2 February 2016 Communicated by Paul Eloe

Abstract. The existence of at least one solution to a nonlinear nth order differential equationx(n)= f(t,x,x0, . . . ,x(n−1)), 0<t<1, under both non-resonant and resonant boundary conditions, is proved. The methods involve the characterization of theRδ-set and an application of a new generalization for a multi-valued version of the Miranda Theorem.

Keywords: nonlinear boundary value problem, decomposable maps,Rδ-set, set-valued map.

2010 Mathematics Subject Classification: 34B15, 34B09.

1 Introduction

Higher order differential equations have been extensively studied in recent years. A variety of results ranging from the theoretical aspects of existence and uniqueness of solutions to analytic and numerical methods for finding solutions have appeared in the literature [1,6,11–13,18].

Such differential equations can be written in the formLx= Nx, whereLis a linear differential operator defined in appropriate Banach spaces and N is a nonlinear operator. When L is a linear Fredholm operator of index 0 under certain boundary conditions, then the kernel of the linear part of the above equation is trivial, and in this case, the corresponding BVP is called non-resonant. This means that there exists an integral operator; then, topological methods can be applied to prove existence theorems. If the kernel ofLis nontrivial, then the problem is said to be at resonance, and then the problem can be managed by using coincidence degree theory.

Such boundary value problems for higher order differential equations have been studied by standard methods in many papers; see, for instance, the papers [2,4,7–10,15–17].

Motivated in this paper by the above research, by applying a generalized Miranda Theorem [14] and a technique completely different from the methods mentioned above, we obtain results devoted to the study of the following higher-order nonlinear differential equation

x(n) = f(t,x,x0, . . . ,x(n1)), 0<t <1, (1.1)

BCorresponding author. Email: yangaij2004@163.com

(2)

under the non-resonant boundary conditions

x(i)(0) =0, x(1) =0, i=1, 2, . . . ,n−1, (1.2) and under the resonant conditions

x(i)(0) =0, x0(1) =0, i=1, 2, . . . ,n−1, (1.3) respectively, where

f: [0, 1]×Rk× · · · ×Rk

| {z }

n

Rk

is a continuous vector function and satisfies appropriate growth conditions; in particular, we assume:

(H1) |f(t,X1,X2, . . . ,Xn)| ≤a1(t)|X1|+a2(t)|X2|+· · ·+an(t)|Xn|+an+1(t), wherea1,a2, . . . , an+1 ∈C([0, 1], R+);

(H2) there exists mi > 0 such that x1i · fi(t,X1,X2, . . . ,Xn) ≥ 0 for t ∈ [0, 1], Xj = (xj1,xj2, . . . ,xjk)∈Rk, and|x1i| ≥mi,i=1, 2, . . . ,k,j=1, 2, . . . ,n.

The rest of this paper is organized as follows. In Section 2, we give some preliminary definitions and theorems on the topological structure of certain sets in metric spaces, which will be employed to obtain the main results. In Section 3, we study the non-resonant BVP (1.1)–(1.2). By introducing an auxiliary initial value problem and characterizing the upper semicontinuous set-valued Rδ-map, we show that this problem has at least one solution. Fi- nally, in Section 4, we deal with the resonant BVP (1.1)–(1.3). By a differential transformation, we get the desired results by adopting the techniques used in Section 3.

2 Preliminaries

First, we present some notations and terminologies.

Definition 2.1. A metric space Xis an absolute neighborhood retract (written ANR) if, given a space Y and a homeomorphic embedding i: X → Y of X onto a closed subset i(X) ⊂ Y, i(X) is a neighborhood retract of Y, i.e. there is an open neighborhood U of i(X) in Y and a retraction r: U → i(X). A map r: U → i(X) is a retraction provided that r(y) = y for y∈i(X).

Definition 2.2. A nonempty space Xis contractible provided there existx0 ∈X and a homo- topyh: X×[0, 1]→ Xsuch thath(x, 0) =x andh(x, 1) =x0 for every x∈X.

Definition 2.3. A compact (nonempty) space X is an Rδ-set (we write X ∈ Rδ), if there is a decreasing sequenceXnof compact contractible spaces such thatX= ∩n1Xn.

Definition 2.4. A set-valued mapΦ: X(Yis upper semicontinuous (writtenUSC) if, given an openV ⊂Y, the set{x ∈X :Φ(x)⊂ V}is open. We sayΦis an Rδ-map if it isUSCand, for eachx ∈X,Φ(x)∈ Rδ.

Definition 2.5. By a decomposable map we mean a pair(D,F)consisting of a set-valued map F: X ( Y and a diagram D: X(Φ Z −→ϕ Y, where Z ∈ ANR, Φ: X ( Z is an Rδ-map, and ϕ: Z→Y a single-valued continuous map, such thatF= ϕΦ.

(3)

Remark 2.6. In our case, Z will be a Banach space, which is ANR. Moreover, notice that a decomposable map (D,F)is an admissible map in the sense of Górniewicz (see [5]).

Remark 2.7. A superposition of a set-valued map with compact values and continuous func- tion is an USCmap, so any decomposable map isUSC.

Definition 2.8. We say the two decomposable maps(D0,F0),(D1,F1)whereDk: X(Φk Zk ϕk

−→Y, k =0, 1, are homotopic (we write (D0,F0) ' (D1,F1)), if there is a decomposable map(D, ˘˘ F) with ˘D: X×[0, 1](Φ˘ Z−→ϕ˘ Yand maps jk: Zk →Z,k=0, 1, such that the diagram

X −→Φ0 Z0

i0j0 &ϕ0 X×[0, 1] −→Φ˘ Z −→ϕ˘ Y

i1j1 %ϕ1

X −→Φ1 Z1

whereik(x) = (x,k)forx∈ X,k=0, 1, is commutative.

Next, we present a result from [3] about the topological structure of the set of solutions for some nonlinear functional equations.

Theorem 2.9. Let X be a space, (B,k · k) a Banach space and h: X → B a proper map, i.e. h is continuous and for every compact E ⊂ B the set h1(E) is compact. Assume further that for each ε>0a proper map hε: X→ B is given and the following two conditions are satisfied:

(a) khε(x)−h(x)k<ε, for every x ∈X;

(b) for anyε>0and u∈ B such thatkuk ≤ε, the equation hε(x) =u has exactly one solution.

Then the set S=h1(0)is Rδ.

Next, we present a generalization of the Miranda Theorem proven in [14], which will be of crucial importance.

Theorem 2.10. Let Mi > 0, i = 1, . . . ,k, and F be an admissible map from∏ki=1[−Mi,Mi] toRk, i.e. there exist a Banach space E,dimE≥k, a linear, bounded and surjective map ϕ: E→Rk and an Rδ-mapΦfrom∏ki=1[−Mi,Mi]to E such that F= ϕ◦Φ. If for any i=1, . . . ,k and every y∈ F(x), where|xi|= Mi, we have

xi·yi ≥0, (2.1)

then there exists x ∈ki=1[−Mi,Mi]such that0∈ F(x).

3 Solutions for BVP (1.1)–(1.2)

In this section, we discuss the BVP (1.1)–(1.2).

First, in setting the stage for the application of Theorem2.10, let the Banach space(B,k · kB) be defined by

B:= {x∈Cn1([0, 1],Rk):x(i)(0) =0, i=1, 2, . . . ,n−1}, kxkB :=max{|x|0, |x(n1)|0},

(4)

where|x|0=max{x(t):t ∈[0, 1]}.

Next, we consider the equation (1.1) under the following initial conditions:

x(0) =c, x(i)(0) =0, i=1, 2, . . . ,n−1, (3.1) wherec∈ Rk is fixed. Notice that the IVP (1.1)–(3.1) is equivalent to

x(t) =c+ 1 (n−1)!

Z t

0

(t−s)n1f s,x(s),x0(s), . . . ,x(n1)(s)ds, t ∈[0, 1]. (3.2) Moreover, we have

x(n1)(t) =

Z t

0

f s,x(s),x0(s), . . . ,x(n1)(s)ds, t∈ [0, 1]. (3.3) Note that

x(t) =c+ 1 (n−2)!

Z t

0

(t−s)n2x(n1)(s)ds, x(i)(t) = 1

(n−2−i)! Z t

0

(t−s)n2ix(n1)(s)ds, i=1, 2, . . . ,n−2.

Then, by applying (3.3) and (H1), fort∈[0, 1], we get

|x(n1)(t)| ≤

Z t

0

a1(s)|x(s)|+a2(s)|x0(s)|+· · ·+an(s)|x(n1)(s)|+an+1(s)ds

Z t

0

a1(s)

|c|+ 1 (n−2)!

Z s

0

(s−τ)n2|x(n1)(τ)|dτ

+a2(s) 1 (n−3)!

Z s

0

(s−τ)n3|x(n1)(τ)|dτ +· · ·

+an1(s)

Z s

0

|x(n1)(τ)|dτ+an(s)|x(n1)(s)|+an+1(s)

ds

Z t

0

a1(s)|c|+an+1(s) +

a1(s)sn1

(n−1)! + a2(s)sn2

(n−2)! +· · ·+an1(s)s+an(s)

· max

τ∈[0,s]

|x(n1)(τ)|

ds

Setw(t) =maxs∈[0,t]|x(n1)(s)|. We obtain

|w(t)| ≤

Z t

0

(a1(s)|c|+an+1(s))ds +

Z t

0

a1(s)sn1

(n−1)! + a2(s)sn2

(n−2)! +· · ·+an1(s)s+an(s)

w(s)ds

≤Kc+

Z t

0

a1(s)sn1

(n−1)! + a2(s)sn2

(n−2)! +· · ·+an1(s)s+an(s)

w(s)ds, where

Kc=

Z 1

0

(a1(s)|c|+an+1(s))ds.

(5)

Now, in view of Gronwall’s Lemma, we have w(t)≤Kcexp

Z t

0

a1(s)sn1

(n−1)! + a2(s)sn2

(n−2)! +· · ·+an1(s)s+an(s)

ds.

Hence

|x(n1)(t)| ≤Kc·eK, t∈[0, 1], (3.4) where

K=

Z 1

0

a1(s)sn1

(n−1)! + a2(s)sn2

(n−2)! +· · ·+an1(s)s+an(s)

ds.

By (3.4), we get the following estimate

|x(t)|=

c+ 1

(n−2)! Z t

0

(t−s)n2x(n1)(s)ds

≤ |c|+ Kc·eK

(n−1)! <∞. (3.5) From above, the Leray–Schauder Alternative implies that the IVP (1.1)–(3.1) has a bounded global solution for everyt∈ [0, 1]and fixedc∈Rk.

Now, givenc∈Rk, consider the nonlinear operatorT: Rk×B→B,(c,x)7→ Tc(x), defined as

Tc(x)(t) =c+ 1 (n−1)!

Z t

0

(t−s)n1f s,x(s),x0(s), . . . ,x(n1)(s)ds, t∈[0, 1]. (3.6) It is clear that Tc(x): [0, 1] → Rk is continuous. Moreover, by applying (H1), (3.4) and (3.5) one can easily show that the image of

{(c,x)∈Rk×B:k(c,x)kRk×B ≤L} underT is relatively compact. we obtain the following results.

Lemma 3.1. Let assumption(H1)hold. Then the operator T is completely continuous.

Notice that the solutions of the IVP (1.1)–(3.1) are fixed points of the operator T defined by (3.6). Let FixTc(·)denote the set of fixed points of operatorTc, wherec∈Rk is given.

Lemma 3.2. Let assumption (H1)hold and Φ: Rk 3 c ( FixTc(·) ⊆ Cn1([0, 1],Rk). Then the set-valued mapΦis USC with compact values.

Proof. The set-valued map Φ is USC with compact values, if given a sequence {cn} in Rk, cn→c0and{xn} ⊆Φ(cn),{xn}has a converging subsequence to somex0Φ(c0).

Taking any sequence{cn},cn→c0 and{xn} ⊆Φ(cn), we have

xn= Tcn(xn). (3.7)

Since {cn}is bounded, by (3.4) and (3.5), we see that {xn(t)} ⊂ B, t ∈ [0, 1] is equibounded.

So {xn} is bounded in B. Lemma 3.1 yields that the operator T is completely continuous.

Then, by (3.7),{xn}is relatively compact inB. Passing to a subsequence if necessary, we may assume that xn →x0 inB. The continuity ofTimplies that

x0= Tc0(x0). Thus, x0Φ(c0)and the proof is complete.

(6)

Lemma 3.3. Let assumption(H1)hold. ThenΦis an Rδ-map.

Proof. By Lemma3.2, the mapΦisUSC. It remains to be shown that for anyc∈Rk,Φ(c)∈Rδ, i.e. the set FixTc(·)is anRδ-set.

Let E = {x ∈ B : kxk ≤ R}, where R := maxKc·eK, |c|+ (Kc·eK

n1)! . Define an operator h: E → B as h(x) = x−Tc(x). Since Tc: E → B is a compact map from Lemma 3.1, h is a compact vector field associated with Tc(·). Then we shall show that there exists a sequence hn: E → B of continuous proper mappings satisfying conditions (a) and (b) of Theorem 2.9 with respect toh.

For the proof it is sufficient to define a sequenceTcn(·): E→Bof compact maps such that Tc(x) = lim

nTcn(x)uniformly inE and show thathn(x) = x−Tcn(x)is a one-to-one map. To do this, we define auxiliary mappingsrn: R+R+by

rn(t):=

(0, t∈[0,n1], t− 1n, t∈(n1, 1]. Now, we can define the sequence{Tcn(·)}as follows:

Tcn(x)(t) =Tc(x)(rn(t)), x∈ E, n∈N+. (3.8) We see that Tcn(·) are continuous and compact. Since |rn(t)−t| ≤ 1n, we deduce from the compactness ofTcn(·)and (3.8) thatTcn(x)→Tc(x)uniformly inE.

Next, we shall prove thathnis a one-to-one map. Assume that for someu,v∈ E, we have hn(u) =hn(v). This implies that

u−v= Tcn(u)−Tcn(v). Ift∈[0,1n], then we have

u(t)−v(t) =Tc(u)(rn(t))−Tc(v)(rn(t)) =Tc(u)(0)−Tc(v)(0) =0.

Thus, we obtainu(t) =v(t)fort ∈[0,1n].

If t ∈ [n1,2n], then rn(t) ∈ [0,1n], rn(rn(t)) = 0. Hence, by the property of operator Tc(·) mentioned above, we have

Tcn(u)(rn(t)) =Tc(u)(rn(rn(t))) =0 and Tc(u)(t) = lim

nTcn(u)(rn(t)) =0

fort∈[n1,2n]. So, we can getTc(v)(t) =0 fort∈[n1,2n]. Thus, we haveu(t) =v(t)fort∈[0,2n]. By repeating this procedure n times we infer that u(t) = v(t)for t ∈ [0, 1]. Therefore, hn is a one-to-one map. Hence the assumptions of Theorem2.9 hold and h1(0) = FixTc(·)is an Rδ-set.

Consider a multifunctionF: Rk(Rk given by

F(c):= {x(1): x∈FixTc}. (3.9) Now, letϕ: B→Rk be such that

ϕ(x) =x(1).

It is easy to see that ϕ is continuous, linear and surjective. Hence the map F = ϕΦ is decomposable with a decomposition

Rk(Φ B−→ϕ Rk.

(7)

Theorem 3.4. If assumptions(H1)and(H2) are satisfied, then the BVP(1.1)–(1.2) has at least one solution.

Proof. Let x∈ FixTc(·)be a bounded global solution of the IVP (1.1)–(3.1). Observe thatx(t) is a solution of the BVP (1.1)–(1.2) if there exists ac∈Rk such that 0∈ F(c). So we will show that all the assumptions in Theorem2.10are satisfied.

By Lemma3.2and3.3,ϕ,ΦandFsatisfy the assumptions of Theorem2.10. Now, we shall show that the condition (2.1) holds.

Letci = mi+1, wheremi is as in (H2) fori=1, 2, . . . ,k. First, we shall prove thatx0i(t)≥0 fort∈[0, 1]. From (3.1), we have x0i(0) =0. Assume that for somet∈ [0, 1], we havex0i(t)<0.

Then there exists t :=inf{t ∈ [0, 1]: xi0(t)< 0}such thatx0i(t) =0 and xi0(t)≥ 0 fort < t. Since xi0(t) is continuous, there exists t1 > t such that Rt1

t |xi0(t)|dt ≤ 1. Hence, in view of xi(0) =ci, we get

xi(t)≥ci+

Z t

t

x0i(s)ds≥mi+1−

Z t1

t

|x0i(t)|dt≥ mi >0, t∈[t,t1]. Now, by condition (H2), we obtain

xi(t)·fi(t,x(t),x0(t), . . . ,x(n1)(t)) =xi(t)·x(in)(t)≥0, t ∈[t,t1].

So, x(in)(t) ≥ 0 for t ∈ [t,t1]. This means that x(in1)(t) is nondecreasing on [t,t1]. Since x(in1)(0) =0, we havex(in1)(t)≥0 fort ∈[t,t1], which means thatxi(n2)(t)is nondecreas- ing on [t,t1]. By repeating this procedure, we can see that x00i(t) ≥ 0 for t ∈ [t,t1], which means that x0i(t)is nondecreasing on[t,t1], and x0i(t)≥ x0i(t) =0 for t ∈ [t,t1], which is a contradiction. Hence xi0(t)≥0 fort ∈[0, 1].

Since xi(0) = ci, we have xi(t) ≥ ci for t ∈ [0, 1]. Then xi(1) ≥ ci. Therefore, by the definition of F,ci·xi(1)≥0. Hence, the condition (2.1) in Theorem2.10is satisfied for Mi := mi+1,i=1, 2, . . . ,k. We can proceed analogously to prove (2.1) in the caseci = −(mi+1).

By Theorem2.10, there existsc∈Rk such that 0∈ F(c). This completes the proof.

Remark 3.5. In view of (3.4) and (3.5), one can see that the solutions of the BVP (1.1)–(1.2) are globally bounded.

4 Solutions for BVP (1.1)–(1.3)

In this section, based on the technique and results in the previous section, we search for solutions for the resonant BVP (1.1)–(1.3).

First, we define the Banach space(B,ˆ k · kBˆ)as

Bˆ :={y∈ Cn2([0, 1],Rk):y(i)(0) =0, i=0, 1, 2, . . . ,n−2}

with the normkykBˆ := |y(n2)|0. Lety(t) =x0(t), then the equation (1.1) can be written as y(n1)= f

t,c+

Z t

0 y(s)ds,y,y0, . . . ,y(n2)

, 0<t <1, (4.1) wherec∈Rk. Now, we consider the equation (4.1) under the following initial conditions:

y(i)(0) =0, i=0, 1, 2, . . . ,n−2. (4.2)

(8)

We can see that the IVP (1.1)–(3.1) is equivalent to the IVP (4.1)–(4.2). Also, we can write the IVP (4.1)–(4.2) in the following form

y(t) = 1 (n−2)!

Z t

0

(t−s)n2f s,c+

Z s

0 y(τ)dτ,y(s),y0(s), . . . ,yn2(s)ds (4.3) fort ∈[0, 1]. Moreover, we have

y(n2)(t) =

Z t

0 f s,c+

Z s

0 y(τ)dτ,y(s),y0(s), . . . ,yn2(s)ds, t∈ [0, 1]. (4.4) Then, by (H1) and (4.4) and applying Gronwall’s Lemma as in Section 3, we can show that

|y(n2)(t)| ≤Kˆc·eKˆ <∞, t ∈[0, 1], (4.5) where

c=

Z 1

0

(a1(s)|c|+an+1(s))ds, Kˆ =

Z 1

0

1

(n−1)!a1(s)sn1+ 1

(n−2)!a2(s)sn2+· · ·+an1(s)s+an(s)

ds.

So, the IVP (4.1) has a bounded global solution for every fixedc∈Rk andt ∈[0, 1]. Now, we also consider a nonlinear operator ˆT:Rk×Bˆ →B,ˆ (c,y)7→ Tˆc(y), given by

c(y)(t) = 1 (n−2)!

Z t

0

(t−s)n2f s,c+

Z s

0 y(τ)dτ,y(s),y0(s), . . . ,yn2(s)ds, (4.6) which is completely continuous.

Notice that the solutions of the IVP (4.1) are fixed points of the operator ˆTdefined by (4.6).

Let Fix ˆTc(·)denote the set of fixed points of operator ˆTc, where c∈Rk is given. We consider the map:

F: Rk (Rk, F(c):= {y(1):y∈Fix ˆTc}. (4.7) If ˆϕ: ˆB→Rk is a map such that

ˆ

ϕ(y) =y(1),

then ˆϕis continuous, linear and surjective. Next, we define a map ˆΦby Φˆ : Rk 3 c(Fix ˆTc(·)⊂Bˆ

and notice thatF= ϕˆ◦Φ.ˆ

The proof of the lemma below is similar to the proof of Lemma3.2, so we omit it here.

Lemma 4.1. Let assumption(H1)hold. Then the set-valued mapΦˆ is USC with compact values.

Lemma 4.2. Let assumption(H1)hold. ThenΦˆ is an Rδ-map.

Proof. By Lemma4.1, the map ˆΦisUSC. We shall show that for anyc∈Rk, the set ˆΦ(c)∈Rδ, i.e. the set Fix ˆTc(·)isRδ-set.

Let ˆE = {x ∈ B : kxk ≤ Rˆ}, where ˆR := Kˆc·eKˆ is taken from (4.5). It is sufficient to observe for the operator ˆTc: ˆE → B, analogous to the proof of Lemmaˆ 3.3, the conditions of Theorem2.9 are satisfied. Hence, ˆΦis anRδ-map.

The following theorem holds true.

(9)

Theorem 4.3. Under assumptions(H1)and(H2), the BVP(1.1)–(1.3)has at least one solution.

Proof. Let y ∈ Fix ˆTc(·) be a bounded global solution of the IVP (4.1). Observe that x(t) = c+Rt

0y(s)ds is a solution of the BVP (1.1)–(1.3) if there exists a c ∈ Rk such that 0 ∈ Fˆ(c). Notice that functions ˆϕ, ˆΦ and ˆF satisfy the assumptions of Theorem 2.10. Now, we shall show that the condition (2.1) holds.

Letci =mi+1, wheremi is as in (H2). First, we shall prove thaty0i(t)≥0 fort∈ [0, 1]. To prove this fact we proceed similarly as in the proof of Theorem 3.4. Now, by the definition of F,ˆ ci·yi(1) ≥ 0. Hence the condition (2.1) in Theorem2.10is satisfied for Mi := mi+1. We can proceed analogously to prove (2.1) in the case thatci =−(mi+1).

Hence, by Theorem2.10, there existsc∈ Rk such that 0∈ Fˆ(c)and the proof is complete.

Remark 4.4. Consider the following boundary conditions

x(i)(0) =0, x(j)(1) =0, i=1, 2, . . . ,n−1, (4.8) where j is a fixed integer such that 1 ≤ j ≤ n−1. Then for each j, the BVP (1.1)–(4.8) is resonant. Lety(t) =x(j)(t), then the IVP (1.1)–(3.1) can be written as













y(nj) = f

t,c+ 1 (j−1)!

Z t

0

(t−s)j1y(s)ds, 1 (j−2)!

Z t

0

(t−s)j2y(s)ds, . . . , Z t

0

(t−s)y(s)ds, Z t

0 y(s)ds,y,y0, . . . ,y(nj1)

, 0<t <1, y(i)(0) =0, i=0, 1, 2, . . . ,n−j−1,

(4.9)

wherec∈Rk. Define the Banach space(B,ˆˆ k · kˆˆ

B)as

Bˆˆ :=ny∈ Cnj1([0, 1],Rk):y(i)(0) =0, i=0, 1, 2, . . . ,n−j−1o

, kykˆˆ

B :=|y(nj1)|0. Adopting the similar techniques used for the BVP (1.1)–(1.3) in this section, we also can obtain the corresponding results for the BVP (1.1)–(4.8).

Acknowledgements

We would like to thank the anonymous referee for the valuable suggestions. This work was funded by National Natural Science Foundation of China (61273016) and Project 201408330015 supported by China Scholarship Council. This research was carried out while the author A. Yang was a Visiting Research Professor at Baylor University.

References

[1] M. Bartušek, M. Cecchi, Z. Došlá, M. Marini, Asymptotics for higher order differential equations with a middle term,J. Math. Anal. Appl.388(2012), 1130–1140.MR2869812;url [2] B. Du, L. Guo, W. Ge, S. Lu, Periodic solutions for generalized Liénard neutral equation

with variable parameter,Nonlinear Anal.70(2009), 2387–2394.MR2498338

(10)

[3] M. Frigon, Topological methods in differential equations and inclusions, Kluwer Academic Publishers, Dordrecht, 1995.MR1368670

[4] J. Geiser, A multiple iterative splitting method for higher order differential equations, J. Math. Anal. Appl.424(2015), 1447–1470.MR3292737

[5] L. Górniewicz, Homological methods in fixed point theory of multi-valued maps, PhD thesis, Polska Akademia Nauk, 1976.MR0394637

[6] J. R. Graef, M. Hill, Nonoscillation of all solutions of a higher order nonlinear delay dynamic equation on time scales,J. Math. Anal. Appl.423(2015), 1693–1703.MR3278223 [7] J. Henderson, Boundary data smoothness for solutions of higher order ordinary differ-

ential equations with integral boundary conditions,Comm. Appl. Nonlinear Anal.20(2013), 21–32.MR3136998

[8] J. Henderson, R. Luca, Existence and multiplicity for positive solutions of a system of higher-order multi-point boundary value problems, NoDEA Nonlinear Differential Equa- tions Appl.20(2013), 1035–1054.MR3057164

[9] J. Henderson, R. Luca, On a system of higher-order multi-point boundary value prob- lems,Electron. J. Qual. Theory Differ. Equ.2012, No. 49, 1–14.MR2948433

[10] Y. H. Li, Z. L. Wei, Positive solutions for a coupled system of mixed higher-order non- linear singular fractional differential equations, Fixed Point Theory 15(2014), 167–178.

MR3234533

[11] M. Mughetti, Hypoellipticity and higher order Levi conditions, J. Differential Equations 257(2014), 1246–1287.MR3210028

[12] Y. F. Pan, M. Wang, Y. Yan, A Hopf lemma for higher order differential inequalities and its applications,J. Differential Equations255(2013), 2826–2845.MR3090079

[13] M. Sabatini, The period functions’ higher order derivatives, J. Differential Equations 253(2012), 2825–2845.MR2964645

[14] K. Szyma ´nska-Debowska, On a generalization of the Miranda Theorem and its ap- plication to boundary value problems, J. Differential Equations 258(2015), 2686–2700.

MR3312640

[15] K. Wang, S. Lu, On the existence of periodic solutions for a kind of high-order neutral functional differential equation,J. Math. Anal. Appl.326(2007), 1161–1173.MR2280971 [16] A. J. Yang, H. L. Wang, Periodic solutions for a kind of higher-order neutral functional

differential equation with variable parameter, Adv. Difference Equ. 2014, No. 187, 10 pp.

MR3374734

[17] A. J. Yang, H. L. Wang, Positive solutions for higher-order nonlinear fractional differen- tial equation with integral boundary condition,Electron. J. Qual. Theory Differ. Equ.2011, No. 1, 1–15.MR2756026

[18] X. J. Yang, Y. I. Kim, K. Lo, Lyapunov-type inequalities for a class of higher-order linear differential equations,Appl. Math. Lett.34(2014), 86–89.MR3212234

Hivatkozások

KAPCSOLÓDÓ DOKUMENTUMOK

In this paper, we investigate the existence of solutions for multi-point boundary value problems of impulsive fractional differential equations at resonance by using the

In this paper we study questions on solvability of some boundary value problems for the Laplace equation with boundary integro-differential operators in the exterior of a unit ball..

Z amora , Non-resonant boundary value problems with singular φ-Laplacian operators, NoDEA Nonlinear Differential Equations Appl.. M awhin , Non-homogeneous boundary value problems

Different from the above works mentioned, motivated by the work [21], we will use the main fixed point theorem and properties of eigenvalue problems for a class of general

In this paper, by applying the coincidence degree theory which was first intro- duced by Mawhin, we obtain an existence result for the fractional three-point boundary value problems

We would mention the re- cent paper [14], by applying symmetric mountain-pass theorem, the author obtained the ex- istence results for nontrivial solutions and a sequence of high

Motivated by the above discussions, the main purpose of this paper is to establish some criteria for the global dynamic behaviors on existence of positive solutions, permanence,

In this paper, we establish the existence of at least three positive so- lutions for the system of higher order boundary value problems on time scales by using the