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Smallest Eigenvalues for a Right Focal Boundary Value Problem

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Published/Copyright: March 22, 2016

Abstract

We establish the existence of smallest eigenvalues for the fractional linear boundary value problems D0+αu+λ1p(t)u=0 and D0+αu+λ2q(t)u=0, 0<t<1 with each satisfying the right focal boundary conditions u(0)=u(1)=0. A comparison result is then obtained.

1 Introduction

We consider the eigenvalue problems

(1.1)D0+αu+λ1p(t)u=0,0<t<1,
(1.2)D0+αu+λ2q(t)u=0,0<t<1,

satisfying the boundary conditions

(1.3)u(0)=u(1)=0

where 1 < α ≤ 2 is a real number, D0+α is the standard Riemann-Liouville derivative, and p(t) and q(t) are continuous nonnegative functions on [0,1] where neither p(t) nor q(t) vanishes identically on any nondegenerate compact subinterval of [0,1]. In this paper, we modify an approach developed by the authors in [5] to show the existence of smallest eigenvalues (1.1), (1.3)and (1.2),(1.3). We will then compare these smallest eigenvalues under the assumption that p(t)q(t).

Using Krein-Rutman theory [14] to show the existence of and compare smallest eigenvalues for boundary value problems has been a well-studied area (see [1, 2, 3, 4, 7, 8, 10, 15, 16] for some examples). However, just recently, the existence and comparison of smallest eigenvalues and applications of these results have been studied for fractional boundary value problems in [5, 6, 9].In [5] the authors studied the second order linear fractional eigenvalue problems with conjugate boundary conditions. The standard approach used in the papers same above was modified to account for the unbounded slope of the Green’s function for D0+α=0,u(0)=u(1)=0at 0. The Green’s function for D0+α=0,u(0)=u(1)=0 also has an unbounded slope at 0. Therefore, in this paper, we use the approach established in [5] to show the existence of and compare smallest eigenvalues for the right focal fractional boundary value problems. The difference inthis analysis to the work done on the conjugate problem is that the Banach space for the right focal problem does not involve C(1) functions since showing the interior of the cone used in this paper does not involve the mean value theorem or the sign of the derivative at 1.

2 Preliminary Definitions and Theorems

Definition 2.1

Let 1 < α ≤ 2. The α-th Riemann-Liouville fractional derivative of the function u : [0,1] → ℝ, denoted D0+αu, is defined as

D0+αu(t)=1Γ(2α)d2dt20t(ts)1αu(s)ds,

provided the right-hand side exists.

Definition 2.2

Let 𝓑 be a Banach space over ℝ. A closed nonempty subset 𝓟 of 𝓑 is said to be a cone, provided:

  1. αu+βv𝓟, for all u,v𝓟 and all α,β0, and

  2. u𝓟 and u𝓟implies u = 0.

Definition 2.3

A cone 𝓟 is solid if the interior, 𝓟⁰, of 𝓟, is nonempty. A cone 𝓟 is reproducing if 𝓑 = 𝓟 −𝓟; i.e., given w ∈ 𝓑, there exist u, v ∈ 𝓟 such that w = u - v.

Remark 2.1

Krasnosel’skii [13] showed that every solid cone is reproducing.

Cones give rise to a natural partial ordering on a Banach space.

Definition 2.4

Let 𝓟 be a cone in a real Banachspace 𝓑. If u, v ∈ 𝓑, uv with respect to 𝓟 if vu ∈ 𝓟. If both M, N : 𝓑 → 𝓑 are bounded linear operators, MN with respect to 𝓟 if MuNu for all u ∈ 𝓟.

Definition 2.5

A bounded linear operator M : 𝓑 → 𝓑 is u0-positive with respect to 𝓟 if there exists u0 ∈ 𝓟\{0} such that for each u ∈ 𝓟\{0}, there exist k1(u) > 0 and k2(u) > 0 such that k1u0Muk2u0 with respect to 𝓟.

The following two results are fundamental to our comparison results and are attributed to Krasnosel’skii [13]. The proof of Theorem 2.1 can be found in [13], and the proof of Theorem 2.2 is provided by Keener and Travis [12] as an extension of Krasnosel’skii’s results.

Theorem 2.1

Let 𝓑 be a real Banach space and let be 𝓟⊂𝓑 are producing cone. Let L : 𝓑→𝓑 be a compact, u0-positive, linear operator.Then L has an essentially unique eigenvector in 𝓟, and the corresponding eigenvalue is simple, positive and larger than the absolute value of anyother eigenvalue.

Theorem 2.2

Let 𝓑 be a real Banach space and 𝓟 ⊂ 𝓑 be a cone.Let both M, N : 𝓑 → 𝓑 be bounded, linear operators and assume that at least one of the operators is u0-positive. IfMN,Mu1λ1u1for some u1 ∈ 𝓟 and someλ1>0,andNu2λ2u2for someu2𝒫and some λ₂ > 0, then λ1λ2. Futhermore, λ1 = λ2 implies u1 is a scalar multiple of u2.

3 Comparison of Smallest Eigenvalues

In [11], Kaufmann and Mboumi showed that the Green’s function for D0α+u(t)=0 satisfying (1.3) is given by

(3.1)G(t,s)={tα1(1s)α2(ts)α1Γ(α),0st1,tα1(1s)α2Γ(α),0ts<1.

Therefore, if u(t)=λ101G(t,s)p(s)u(s)ds,u(t) solves (1.1), (1.3). Similarly, if u(t)=λ201G(t,s)q(s)u(s)ds,u(t) solves (1.2),(1.3). Notice that G(t, s) ≥ 0 on [0, 1] × [0, 1) and G(t, s)>0 on (0,1]×(0,1).

Define the Banach space

𝓑={u:u=tα1v,vC[0,1]},

with the norm

u=|v|0,

where |v|0=supt[0,1]|v(t)|denotes the usual supremum norm. Notice that for u ∈ 𝓑

|u|0=|tα1v|0tα1u,

implying

|u|0u.

Define the linear operators

(3.2)Mu(t)=01G(t,s)p(s)u(s)ds,

and

(3.3)Nu(t)=01G(t,s)q(s)u(s)ds.

Now,

Mu(t)=01tα1(1s)Γ(α)α2p(s)u(s)ds01(ts)Γ(α)α1p(s)u(s)ds=tα-1(01(1s)Γ(α)α2p(s)u(s)dst1α01(ts)Γ(α)α1p(s)u(s)ds).

Notice that since α > 1,

|01(1s)α2Γ(α)p(s)u(s)ds||p|0|v|0Γ(α)|01sα1(1s)α2ds|=|p|0|v|0Γ(α1)Γ(2α1)<.

Therefore, the first term inside the parentheses is well-defined.

Set

g(t)={0,t=0,t1αot(ts)α1Γ(α)p(s)u(s)ds,0<t1.

In the proof of Theorem 3.1 in [5], it was shown gC[0, 1]. Therefore, M : 𝓑 → 𝓑. An application of the Arzelà Ascoli theorem shows M is compact. A similar argument can be made for N. Thus, we have the following result.

Theorem 3.1

The operators M, N : 𝓑 → 𝓑 are compact.

Next, we define the cone

P={uB|u(t)0 for t[0,1]}.
Lemma 3.1

The cone 𝓟 is solid in 𝓑 and hence reproducing.

Proof. Define

(3.4)Ω:={u= tα1 v B : u(t)>0  for t (0,1], v(0) > 0}.

We will show Ω ⊂ 𝓟⁰. Let u ∈ Ω. Since, v(0) > 0, there exists an ϵ1 > 0 such that v(0)– ϵ1 > 0. Since vC[0,1], there exists an a ∈(0,1) such that v(t) > ϵ1 for all t ∈ (0,a). So u(t) = tα−1v(t) > ϵ1tα−1 for all t ∈ (0,a). Also, since u(t)>0 on [a 1], there exists an ϵ2 > 0 with u(t) – ϵ2 > 0 for all t ∈ [a, 1].

Let ϵ=min{ϵ12,ϵ22} . Define Bϵ(u)={u^ϵB:uu^<ϵ}.Let u^ϵBε(u) . So u^=tα1v^, where v^C[0,1]. Now |u^(t)u(t)|tα1u^u<εtα1. So for t ∊ (0, a) u^(t)>u(t)tα1ϵ>tα1ϵ1tα1ϵ1/2=tα1ϵ1/2. So u^(t)>0 for t ∊ (0, a). Also, |u^(t)u(t)|u^u<ε . So for t ∊ [a, 1] u^(t)>u(t)ε>ε2ε2/2>0. So u^P for all t ∊ [a, 1] . So u^(t)>0 and thus ΩP . So Bϵ(u)P.

Lemma 3.2

The bounded linear operators M and N are u0-positive with respect to 𝓟

Proof. First, we show M: 𝓟\{0}Ω𝓟0. Let u ∊ 𝓟. So u(t) ≥ 0. Then since G(t, s) ≥ 0 on [0, 1] × [0, 1) and p(t) ≥ 0 on [0, 1], Mu(t)=01G(t,s)p(s)u(s)ds0, for 0 ≤ t ≤ 1 So M : PP

Now let u ∊ 𝓟\{0}. So there exists a compact interval [α, β] ⊂ [0,1] such that u(t) > 0 and p(t) > 0 for all t ϵ[α, β].Then, since G(t, s) > 0 on (0, 1] × (0, 1),

Mu(t)=01G(t,s)p(s)u(s)dsαβG(t,s)p(s)u(s)ds>0,

for 0 < t ≤ 1. Now,

Mu(t)=tα1(01(1s)α2Γ(α)p(s)u(s)dst1α0t(ts)α1Γ(α)p(s)u(s)ds)

Let

v(t)=01(1s)α2Γ(α)p(s)u(s)dst1α0t(ts)α1Γ(α)p(s)u(s)ds.

So,

v(0)=01(1s)α2Γ(α)p(s)u(s)ds>0

, thus M:𝓟\{0}Ω𝓟o.

Now choose u⁰ ϵ𝓟\{0}, and let uϵ𝓟\{0} . So MuϵΩ𝓟o . Choose k1>0sufficiently small and k2sufficiently large so that Muk1u0ϵ𝓟o and u01k2Muϵ𝓟o . So k1u0Mu with respect to 𝓟 and Muk2u0 with respect to 𝓟 . Thus k1u0Muk2u0 with respect to 𝓟 and M is u0-positive with respect to 𝓟. A similar argument shows N is u0-positive.

Lemma 3.3

The eigenvalues of (1.1),(1.3) are reciprocals of eigenvalues of M, andconversely.Similarly, eigenvalues of (1.2),(1.3) are reciprocals of eigenvalues of N, andconversely.

Proof. Let Λ be an eigenvalue of M with corresponding eigenvector u(t). Notice that

Λu(t)=Mu(t)=01G(t,s)p(s)u(s)ds,

if and only if

u(t)=1Λ01G(t,s)p(s)u(s)ds,

if and only if

D0+αu(t)+1Λp(t)u(t)=0,0<t<1,

With

u(0)=u(1)=0.

So

1Λ

is an eigenvalue of (1.1),(1.3). A similar argument can be made for eigenvalues of N.

Theorem 3.2

Let 𝓑, 𝓟, M, and N be defined as earlier. Then M (and N) has an eigenvalue that is simple, positive, and larger than the absolute value of any other eigenvalue, with an essentially unique eigenvector that can be chosen to be in 𝓟⁰

Proof. Since M is a compact linear operator that is u0-positive with respect to 𝓟, by Theorem 2.1, M has an essentially unique eigenvector, say, u ϵ 𝓟 and eigenvalue Λ with the above properties. Since u ≠ 0 MuϵΩ𝓟oand u=M(1Λu)ϵ𝓟o.

Theorem 3.3

Let 𝓑, 𝓟, M and N be defined as earlier. Let p(t)≤q(t) on [0,1]. Let Λ1 and Λ2 be the eigenvalues defined in Theorem 3.2 associated with M and N, respectively, with the essentially unique eigenvectors u1 and u2 ϵ P⁰. Then Λ1≤Λ2, and Λ1 = Λ2if and only if p(t) = q(t) on [0,1].

Proof. Let p(t)q(t) on [0, 1]. So for any u ∊ 𝓟 and t ϵ [0,1],

(NuMu)(t)=01G(t,s)(q(s)p(s))u(s)ds0

So NuMu ∊ 𝓟 for all u ∊ 𝓟, or MN with respect to 𝓟 . Then by Theorem 2.2 Λ1 ≤ Λ2

If p(t) = q(t), then Λ1 = Λ2. Now suppose p(t)q(t). So p(t) < q(t) on some subinterval [α,β] ⊂ [0,1] .Then, using an argument similar to the proof that N was u0-positive, (NM)u1 ∊ Ω ⊂P⁰ and so there exists ε > 0 such that (NM)u1 − εu1ϵP. So Λ1u1 + εu1 = Mu1 + εu1Nu1, implying Nu1≥(Λ1+ε)u1. Since NN and Nu2 = Λ2u2 by Theorem 2.2 Λ1 + ε ≤ Λ1, or Λ1 < Λ2.

Since the eigenvalues of (1.1),(1.3) are reciprocals of eigenvalues of Mand conversely, and the eigenvalues (1.2),(1.3) of are reciprocals of eigenvalues of N and conversely, the following theorem is an immediate consequence of Theorems 3.2 and 3.3

Theorem 3.4

Assume the hypotheses of Theorem 3.3 Then there exists smallest positive eigenvalues λ1 and λ2 of (1.1),(1.3) and (1.2),(1.3), respectively, each of which is simple, positive, and less than the absolute v alue of any other eigenvalue of the corresponding problems. Also, eigenfunctions corresponding to λ1and λ2 be chosen to belong to 𝓟 ⁰. Finally, λ1λ2, and λ1=λ2 if and if p(t) = q(t) for all t ∊ [0,1]

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  1. Please cite to this paper as published in: Fract. Calc. Appl. Anal., vol. 19, No 1 (2016), pp. 1–10, DOI: 10.1515/fca-2016-0002

Received: 2015-3-5
Published Online: 2016-3-22
Published in Print: 2016-3-1

© 2016 Diogenes Co., Sofia

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