1 Introduction

Recently,fractional differential equations have drawn much attention.It is caused both by the theory of fractional calculus itself and by the applications in various fields of science and Engineering such as control,electrochemistry,electromagnetic,porous media,viscoelasticity,etc,for detail,see[1-5].

In this paper,we consider the following fractional Sturm-Liouville operator:

acting on the Hilbert space L2[0,1]with the following boundary condition:

where p(x)≠0,p(x)∈C1(0,1),q(x)∈C(0,1),0＜α＜1 and aij,bij∈R(i,j=1,2).,andare fractional integral operator,fractional derivative and Caputo fractional derivator acting on given functions respectively.Our purpose is to find sufficient conditions on the coefficients matrices A and B to guarantee a symmetric operator,where

We know that,the second-order Sturm-Liouville differential expression

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where p(x)≠0,,q∈L(0,1),with the following boundary condition:

when the coefficient matrices satisfy

generates a self-adjoint operator,where

This result has great significance in the spectral theory of Sturm-Liouville operator.

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2 Preliminaries

We will use the following properties of fractional integrals and derivatives.

Definition 2.1[3]For given α with R(α) ＞ 0,the left and right Riemann-Liouville integrals of order α are defined as

Moreover,

In particular,when 0＜α＜1,we have

Definition 2.3[3]Let R(α)∈ (n−1,n),where n ∈ N,D=.The left and right Caputo derivatives of order α are de fined as

In particular,when 0＜α＜1,we have

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Lemma 2.1[3]Let R(α)∈ (n−1,n),where n∈ N.If y∈ ACn[0,1],then the fractional derivatives andexist almost everywhere on[0,1]and can be represented in forms

is determined by U and Uc.

Lemma 2.3[3]Fractional integration operators andwith R(α)≥0 are bounded in Lp(0,1)(1≤p≤∞):

Corollary 2.1 Fractional integration operators and are operators defined on Lp(0,1)(1≤p≤∞).

Proof For all f∈Lp(0,1),it is easy to see that f satisfies

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so

Therefore,the integral operator is an operator from Lp(0,1)to Lp(0,1)(1≤p≤∞).

Lemma 2.4[3]If R(α)＞ 0 and f(x)∈ Lp(0,1)(1≤p≤ ∞),then the following equalities

hold almost everywhere on[0,1].

Lemma 2.5[3]If α/∈N,then the Caputo fractional derivatives coincide with the Riemann-Liouville fractional derivatives in the following cases:

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if

if

Lemma 2.6[3]The space ACn[0,1]consists of those and only those functions f(x)which can be represented in the form

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where φ ∈ L(0,1),ck(k=0,1,···,n − 1)are arbitrary constants,and

Consider the following fractional differential equation

Assume that p(x)≠0,p(x)∈C1(0,1)and q(x)∈C(0,1),obviously,l cannot act on the whole space L2[0,1].

Definition 2.4 The subset of L2[0,1]which satisfies:

is called the maximal operator domain of l,denoted by DM.The operator generated by it is called maximal operator,denoted by LM.

Definition 2.5 The subset of DMwhich satisfies:

is called the minimal operator domain of l,denoted by Do.The operator generated by it is called minimal operator,denoted by Lo.

From Table 2,it can be seen that there is only one interjection appeared in top 10 of the keyword list of MC —“oh”.Besides,the frequency of“oh”in MC is 55,which is far less than the number of 291 in FC.

Let y and z be two functions of DM.Using Lemma 2.2,we obtain

and

So,

T is then a formal adjoint of S,too.

[yz](x)is called the lagrange bilinear form about l,and it is also called the fit function of y and z.We denote by=[yz](1)−[yz](0).Then we obtain

Denote

Then

Q(x)is called the fit matrix of l.

Definition 2.6 Let y∈L2[0,1],the boundary type of y is defined as

where aij,bij∈ C(i=1,2,···,r;1≤ r≤ 4).

Denote

Obviously,a boundary type vector is self-conjugate,then its dimension r must satisfy r=4−r,that is r=2.

where C(y)0=C(y)|x=0,and C(y)1is defined in the same way.We call U(y)the boundary type vector.

Let

Definition 2.2[3]Let R(α)∈ (n−1,n),where n ∈ N,D=.The left and right Riemann-Liouville derivatives of order α are de fined as

If rank(A⊕B)=r,U(y)is called of r-dimensional,or U1,···,Urare linearly independent.We always assume they are linearly independent in the following discussion.

For r=1,2,3,let Ur+1,···,U4be 4−r linearly independent boundary types,and their vector form is Ucy.If the boundary type vector

is 4-dimensional,we say that U(y)and Uc(y)are complementary.Apparently,it is possible to find complementary boundary type vector of any boundary type vector.

3 Main Results

Theorem 3.1 For given r-dimensional boundary type vector U(y)and its complementary(4−r)-dimensional boundary type vector Uc(y),there is a unique r-dimensional Vc(z)and its(4−r)-dimensional boundary type vector V(z),which satisfy

where “·” is the inner product of Euclidean space.

Proof Let

where A and B are(r×2)-dimensional matrices, and are(4−r)×2-dimensional matrices.

Let

Since U and Ucare complementary,H is a non-singular matrix,so we obtain

By(2.4),

Let

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thencan be changed into

Apparently, is a non-singular matrix.So(H−1)∗is a non-singular matrix.Let

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then it is a 4-dimensional boundary type vector,where Vc(z)is an r-dimensional boundary type vector,V(z)is its complementary(4−r)-dimensional boundary type vector.Since(z)is determined by H,

Lemma 2.2[3]Let α ∈(n−1,n),where n∈N.Then operators ,,andsatisfy the following integrations by parts,

Definition 3.1 V(z)is called the adjoint boundary type vector of U(y),where V(z)and U(y)are defined as above.

If V(z)is an adjoint boundary type vector of U(y),then U(y)is an adjoint boundary type vector of V(y),and they are adjoint boundary type vectors of each other.

Definition 3.2 If two boundary type vectors V(y)and V ′(y)satisfy V ′(y)=CV(y),where C is a non-singular matrix,then they are called equivalent;if a boundary type vector V(y)is equivalent with its adjoint boundary type vector,we call it is self-conjugate.

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So U(y)can be expressed in the following form

A nature thought is to imitate the second-order Sturm-Liouville problem,and thereby the self-adjoined description of the fractional Sturm-Liouville problem is given.However,a fractional derivation operator is quite different from an ordinary differential operator in some properties,especially we fail to get the existence and uniqueness of the fractional equation till now.Therefore,the method can not be completely applied to study our problem.

Definition 3.3 If U(y)and V(z)are adjoint boundary type vectors of each other,we say that U(y)=0 and V(z)=0 are adjoint boundary conditions of each other;if U(y)is self-conjugate,we say that U(y)=0 is a self-conjugate boundary condition.

Definition 3.4 Assume that H1and H2are Hilbert spaces,T is an operator from H1into H2,and S is an operator from H2into H1.The operator S is called a formal adjoint of T if we have

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Denote

Theorem 3.2 Let L and L′be operators generated by l(y).The domain of L is defined by the boundary condition U(y)=0,and the domain of L′is defined by the boundary condition V(y)=0.If U(y)=0 and V(y)=0 are adjoint boundary conditions of each other,then L and L′are formal adjoints of each other.

ProofFor all y∈ D(L),z∈ D(L′),we have U(y)=0,V(z)=0.Since U(y)=0 and V(z)=0 are adjoint boundary conditions of each other,by Theorem 3.1,there is

so we conclude that(l(y),z)−(y,l(z))=0,that is(l(y),z)=(y,l(z)),for any y∈D(L)and z∈D(L′).Therefore,L and L′are formal adjoints of each other.

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Theorem 3.3 Let the domain of L be defined by U(y)=0.If U(y)=0 is self-conjugate,then L is a Hermitian operator.

Proof For the above U(y)and any of its complementary boundary type vector Uc(y),there exists one and only one V(z)and Vc(z),satisfying

Since U(y)=0 is self-adjoint,there is a non-singular matrix C satisfing V(z)=CU(Z).Therefore,

For all y,z∈D(L),we have U(y)=V(z)=0.Therefore,(l(y),z)−(y,l(z))==0.So

We conclude that L is a Hermitian operator.

Theorem 3.4 Let U(y)=AC(y)0+BC(y)1and V(y)=SC(y)0+TC(y)1be an r-dimensional and the corresponding(4−r)-dimensional boundary type vectors respectively,if

then U(y)=0 and V(y)=0 are adjoint boundary conditions of each other,where Q(x)is a fit matrix of l(y).

Proof We only need to prove that if there are(4−r)×2 matrices S1and T1 with rank(S1⊕T1)=4−r,which satisfy AQ(0)−1=BQ(1)−1,then we can find a non-singular matrix C satisfying S1=CS,T1=CT,thereby

is equivalent to V(z).So U(y)=0 and V(y)=0 are adjoint boundary conditions of each other.

Since we assume that rank(A⊕B)=r,the linear space spanned by r linearly independent row vector of(A⊕B)is denoted by T.Since

we have

which shows that the column vectors of matrix

all belong to T⊥.Since

and rank(S1+T1)=4−r,we conclude that rankR1=4−r,which shows that all(4−r)column vectors of R1are linearly independent,therefore they make up the basis of T⊥.

Since S,T and S1,T1satisfy the above conditions,we can get that the rank of matrix

is(4−r),and all(4−r)column vectors make up the basis of T ⊥.Therefore we can find a(4−r)×(4−r)non-singular matrix C satisfying S1=CS,T1=CT,and this shows that V1(z)is equivalent to V(z),thereby U(y)=0 and V(y)=0 are adjoint boundary conditions of each other.

Corollary 3.1 If the boundary condition U(y)=AC(y)0+BC(y)1satisfies AQ−1(0)A∗=BQ−1(1)B∗,then U(y)=0 define a Hermitian operator.

Lemma 3.1is an operator from AC2(0,1)into L2(0,1).

Proof The operator

could be rewritten as

We known that,for the two-order Sturm-Liouville operator,the maximum operator map AC2(0,1)into L2(0,1).So when z(x)∈AC2(0,1),(Dp(x)Dz)(x)∈L2(0,1).By Corollary 3.1,

Remark 3.1 By the definition of fractional derivative,l(y)can be rewritten as

In order to make sure that l is an operator on L2[0,1],we con fine that z(x)=belongs to AC2[0,1],since we limit∈AC[0,1]in the definition of DM.Based on the above discussion,we describe DMin more detail:

Consider a subspace of DM:

Now we define a new operator:

Theorem 3.5 T is an invertible operator from E to AC2[0,1],further,T−1=

Proof By Lemma 2.4,when y(x)∈E⊆L2(0,1),

that is=I.When z(x)∈TE,

Since z(0)=0,by Lemma 2.4,that is T=I.Therefore T is an invertible operator from E to AC2[0,1],and T−1=

Lemma 3.2 Space AC2[0,1]is a subspace of AC[0,1].

Proof For all y(x) ∈ AC2[0,1],|y′(x)|has a upper bound K,therefore y(x)is a Lipschitz continuous function on[0,1],thus it belongs to AC[0,1].

Corollary 3.2 AC[0,1]is a dense subspace of L2(0,1).

Proof For the second-order Sturm-Liouville operator,the minimum operator domain

is a dense subspace of L2(0,1),howeveris a subspace of AC[0,1].

Theorem 3.6 The maximal operator LMis a densely defined operator.

Proof Since E is a subspace of DM,it is necessary to prove that E is a dense subspace of L2(0,1).

For all y(x) ∈ TE,by Lemma 2.1,Denote F=D(TE),then E=F.By Lemma 2.3,is a bounded operator on L2(0,1),thus we only need to prove that F is a dense subspace of L2(0,1).In fact,TE={z(x)∈AC2[0,1]|z(0)=0},by Lemma 2.6,D(TE)=D(AC2[0,1])=AC[0,1].By Corollary 3.2,it is a dense subset of L2(0,1).

Theorem 3.7 The minimal operator Lois a densely defined operator.

Proof According to the definition of Minimal operator,

thus

Similarly to the above discussion,we obtain

By Corollary 3.2,

is a dense subspace of L2(0,1).Combined with the boundedness of,we finish the proof.

Remark 3.2 If we con fine y(x)|x=1=0 in addition,that is

When These functions can not be dense in L2[0,1],since=0 does not hold in the definition of minimal operator.

Theorem 3.8 The boundary conditions of l(y):

satisfing

generate a symmetry operator by l,where

Proof Since the minimal operator Lois a densely defined operator,that is,

is a dense subspace of L2(0,1),therefore the functions with

are dense in L2(0,1),thus the functions with

are also dense in L2(0,1).

By Theorems 3.3 and 3.4,if

the operator with the above boundary condition is symmetry.

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