Existence of nonnegative solutions for a fractional m-point boundary value problem at resonance
Qu and Liu Boundary Value Problems 2013, 2013:127
http://www.boundaryvalueproblems.com/content/2013/1/127
RESEARCH
Open Access
Existence of nonnegative solutions for a
fractional m-point boundary value problem
at resonance
Haidong Qu1* and Xuan Liu2
*
Correspondence:
1
Department of Mathematics,
Hanshan Normal University,
Chaozhou, Guangdong 521041,
China
Full list of author information is
available at the end of the article
Abstract
We consider the fractional differential equation
q
D0+ u(t) = f (t, u(t)),
0 < t < 1,
satisfying the boundary conditions
p
p–1
p–n+1
D0+ u(t)|t=0 = D0+ u(t)|t=0 = · · · = D0+
u(t)|t=0 = 0,
u(1) =
m–2
αi u(ξi ),
i=1
q
where D0+ is the Riemann-Liouville fractional order derivative. The parameters in the
multi-point boundary conditions are such that the corresponding differential
operator is a Fredholm map of index zero. As a result, the minimal and maximal
nonnegative solutions for the problem are obtained by using a fixed point theorem of
increasing operators.
MSC: 26A33; 34A08
Keywords: fractional order; coincidence degree; at resonance
1 Introduction
Let us consider the fractional differential equation
q
D+ u(t) = f t, u(t) ,
< t < ,
(.)
with the boundary conditions (BCs)
⎧
⎨Dp u(t)| = Dp– u(t)| = · · · = Dp–n+ u(t)| = ,
t=
t=
t=
+
+
+
⎩u() = m– αi u(ξi ),
i=
(.)
q–
where n ≥ , max{q – , } ≤ p < q – , n < q ≤ n + , m–
= , αi > , < ξ <
i= αi ξi
ξ < · · · < ξm– < , m ≥ . We assume that f : [, ] × [, ∞) → [, ∞) is continuous.
A boundary value problem at resonance for ordinary or fractional differential equations
has been studied by several authors, including the most recent works [–] and the references therein. In the most papers mentioned above, the coincidence degree theory was
© 2013 Qu and Liu; licensee Springer. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any
medium, provided the original work is properly cited.
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applied to establish existence theorems. But in [], Wang obtained the minimal and maximal nonnegative solutions for a second-order m-point boundary value problem at resonance by using a new fixed point theorem of increasing operators, and in this paper we
use this method of Wang to establish the existence theorem of equations (.) and (.).
For the convenience of the reader, we briefly recall some notations.
Let X, Z be real Banach spaces, L : dom(L) ⊂ X → Z be a Fredholm map of index zero
and P : X → X, Q : Z → Z be continuous projectors such that Im(P) = Ker(L), Ker(Q) =
Im(L) and X = Ker(L) ⊕ Ker(P), Z = Im(L) ⊕ Im(Q). It follows that L|Ker(P)∩dom(L) : Ker(P) ∩
dom(L) → Im(L) is invertible. We denote the inverse of the map by KP : Im(L) → Ker(P) ∩
dom(L). Since dim Im(Q) = dim Ker(L), there exists an isomorphism J : Im(Q) → Ker(L).
Let Ω be an open bounded subset of X. The map N : X → Z will be called L-compact on Ω
if QN(Ω) and KP (I – Q)(Ω) are compact. We take H = L + J – P, then H : dom(L) ⊂ X → Z
is a linear bijection with bounded inverse and (JQ + KP (I – Q))(L + J – P) = (L + J – P)(JQ +
KP (I – Q)) = I. We know from [] that K = H(K ∩ dom(L)) is a cone in Z.
Theorem . [] N(u) + J – P(u) = H(ũ), where
ũ = P(u) + JQN(u) + KP (I – Q)N(u)
and ũ is uniquely determined.
From the above theorem, the author [] obtained that the assertions
(i) P(u) + JQN(u) + KP (I – Q)N(u) : K ∩ dom(L) → K ∩ dom(L) and
(ii) N(u) + J – P(u) : K ∩ dom(L) → K are equivalent.
We also need the following definition and theorem.
Definition . [] Let K be a normal cone in a Banach space X, u ≤ v , and u , v ∈
K ∩ dom(L) are said to be coupled lower and upper solutions of the equation Lx = Nx if
⎧
⎨Lu ≤ Nu ,
⎩Lv ≥ Nv .
Theorem . [] Let L : dom(L) ⊂ X → Z be a Fredholm operator of index zero, K be a
normal cone in a Banach space X, u , v ∈ K ∩ dom(L), u ≤ v , and N : [u , v ] → Z be
L-compact and continuous. Suppose that the following conditions are satisfied:
(C ) u and v are coupled lower and upper solutions of the equation Lx = Nx;
(C ) N + J – P : K ∩ dom(L) → K is an increasing operator.
Then the equation Lx = Nx has a minimal solution u∗ and a maximal solution v∗ in [u , v ].
Moreover,
u∗ = lim un ,
n→∞
v∗ = lim vn ,
n→∞
where
–
N + J – P un– ,
un = L + J – P
–
N + J – P vn– ,
vn = L + J – P
n = , , , . . . and u ≤ u ≤ u ≤ · · · ≤ un ≤ · · · ≤ vn ≤ · · · ≤ v ≤ v ≤ v .
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2 Preliminaries
In this section, we present some necessary basic knowledge and definitions about fractional calculus theory.
q
Definition . (see Equation .. in []) The R-L fractional integral I+ u of order q ∈ R
(q > ) is defined by
q
I+ u(t) :=
t
Γ (q)
u(τ ) dτ
(t
– τ )–q
(t > ).
Here Γ (q) is the gamma function.
q
Definition . (see Equation .. in []) The R-L fractional derivative D+ u of order
q ∈ R (q > ) is defined by
d
dt
q
D+ u(t) =
=
n
n–q
I+ u(t)
d
Γ (n – q) dt
n
t
u(τ ) dτ
(t
– τ )q–n+
n = [q] + , t > ,
where [q] means the integral part of q.
Lemma . [] If q , q > , q > , then, for u(t) ∈ Lp (, ), the relations
q
q +q
q
I+ I+ u(t) = I+ u(t)
and
q
q
D+ I+ u(t) = u(t)
hold a.e. on [, ].
q
Lemma . (see []) Let q > , n = [q] + , D+ u(t) ∈ L (, ), then we have the equality
q
q
I+ D+ u(t) = u(t) +
n
Ci t q–i ,
i=
where Ci ∈ R (i = , , . . . , n) are some constants.
q
Lemma . (see Corollary . in []) Let q > and n = [q] + , the equation D+ u(t) = is
valid if and only if u(t) = ni= Ci t q–i , where Ci ∈ R (i = , , . . . , n) are arbitrary constants.
Let X = Z = C[, ] with the norm u = supt∈[,] |u(t)|, then X and Z are Banach spaces.
Let K = {u ∈ X : u(t) ≥ , t ∈ [, ]}. It follows from Theorem .. in [] that K is a
normal cone.
q
Let dom(L) = {u(t) ∈ X | D+ u(t) ∈ Z, u(t) satisfies BCs (.)}.
We define the operators L : dom(L) → Z by
q
(Lu)(t) = D+ u(t)
(.)
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and N : K → Z by
(Nu)(t) = f t, u(t) ,
then BVPs (.) and (.) can be written as Lu = Nu, u ∈ K ∩ dom(L).
Lemma . If the operator L is defined in (.), then
(i) Ker(L) = {c · t q– | c ∈ R},
q– s
(ii) Im(L) = {y ∈ Z | ( – s)q– m–
i= αi ξi
ξi s y(τ ) dτ ds = } =: L.
Proof (i) It can be seen from Lemma . and BCs (.) that Ker(L) = {c · t q– | c ∈ R}.
q
(ii) If y ∈ Im(L), then there exists a function u ∈ dom(L) such that y(t) = D+ u(t), by
Lemma ., we have
q
I+ y(t) = u(t) + c t q– + · · · (...truncated)