Open Access

Existence of integro-differential solutions for a class of abstract partial impulsive differential equations

Journal of Inequalities and Applications20112011:135

DOI: 10.1186/1029-242X-2011-135

Received: 1 March 2011

Accepted: 7 December 2011

Published: 7 December 2011

Abstract

In this study, we investigate the existence of integro-differential solutions for a class of abstract partial impulsive differential equations.

Keywords

integro-differential equations neutral differential equations analytic semigroup of compact operators; non-autonomous operators family of evolution operators mild solutions

1. Introduction

In this study, we established two existence results of solutions for a class of impulsive functional differential equations which can be described in the following form
d d t D ( t , u t ) = A ( t ) D ( t , u t ) + f ( t , u t , 0 t e ( t , s , u s ) d s ) , t [ 0 , b ] , t t i ,
(1.1)
u 0 = φ , φ ,
(1.2)
Δ u ( t i ) = I i ( u t i ) , i { 1 , , m }
(1.3)

where A ( t ) : D ( A ( t ) ) X X is a family of unbounded linear closed operators such that for each t [0, b], A(t) is the infinitesimal generator of analytic semigroup of linear bounded operators (S t (s))s ≥ 0on a Banach space X , endowed with the norm X ; the history u t : ( - , 0 ] X is defined as u t (θ) = u(t + θ), θ ≤ 0; is a set of measurable functions φ : (-∞, 0] → X endowed with appropriate seminorm; the operator D(t, ϕ) is defined as D(t, ϕ) = ϕ(0) + g(t, ϕ), where the functions g : [ 0 , b ] × X , f : [ 0 , b ] × × X X and I i : X X , i are appropriate functions for all i {1, ..., m}; 0 < t1 < < t m < b is a sequence of fixed real numbers and the symbol Δξ(t) represents the jump of the function ξ at the moment t, this means that Δξ (t) = ξ (t+) - ξ(t-), where the notation ξ(t+) and ξ(t-) represent, respectively, the right and the left-hand side limits of the function ξ at t.

There are many physical phenomena that are described by means of impulsive differential equations, for instance, biological systems, electrical engineering, chemical reactions, among others can be modeled by impulsive differential equations, a good survey on impulsive differential equations can be found in [1] see also [2, 3]. However, impulsive actions can influence the behavior of solutions making the analysis more difficult. Motivated by this facts, the studies of such systems have drawn the attention of many researchers during last years.

Recently, Park et al. [4] have investigated the problem
d d t x ( t ) - g ( t , x t , 0 t a ( t , s , x s ) d s ) = A x ( t ) + f ( t , x t , 0 t e ( t , s , x s ) d s ) , t [ 0 , b ] , t t i , i = 1 , 2 , , m , Δ x ( t i ) = I i ( x ( t i - ) ) , i = 1 , 2 , , m , x 0 = φ h .
(1.4)
In this model, the operator A : D ( A ) X X is the infinitesimal generator of a compact analytic semigroup of bounded linear operators (T(t))t ≥ 0on a Banach space X such that 0 ρ(A), where ρ(A) is the resolvent set of the operator A ; a , e : [ 0 , b ] 2 × h X , f , g : [ 0 , b ] × h × X X and I i : X X , i = 1, 2,..., m are given functions that satisfy suitable conditions. Using the theory of fractional powers and priori estimates for compact operators, the authors established some existence result for the problem (1.4). Lately, Balachandran and Annapoorani [5] investigated the following class of abstract problem (1.5)
d d t x ( t ) - g ( t , x t ) = A ( t ) x ( t ) + f ( t , x t ) + 0 t e ( t , s , x s ) d s , t I = [ 0 , b ] , t t i , i = 1 , 2 , , m , Δ x ( t i ) = I i ( x ( t i - ) ) , i = 1 , 2 , , m , x 0 = φ h .
In the system (1.5), it was assumed that for each t [0, b] the operator A(t) is the infinitesimal generator of compact analytic semigroup of bounded linear operators on a Banach space X . Moreover, the domain, D(A(t)), of the operators A(t) is assumed to be independent of t [0, b] and dense in X , i.e., A ( t ) : D X X with D ¯ = X . To get their results, the authors used the conditions of Acquistapace and Terreni, see [6], to guarantee the existence of an evolution family of operators associated with the non-autonomous abstract Cauchy problem
u ( t ) = A ( t ) u ( t ) , t [ 0 , b ] , u ( 0 ) = x X .

Then, using fractional powers and operators theory the authors get some existence result based on a priori bounded estimates for compact operators.

Other authors have studied problems involving impulsive act, for retarded and neutral functional differential equations we cite [717], for applications of impulsive differential equations on biology and neural networks we cite [1821]. On the other hand impulsive fractional differential equations is a topic treated in [22, 23].

In this article, the study of a class of neutral impulsive integro-differential equations is proposed. To get our results, we used the technique involving the fixed point theory of compact and condensing operators. We pointed out that the problem studied in this article has not been considered in the literature, once that the approach used in this study is totally different from those studies mentioned above. Actually, the main difference is that in our study we need to use an assumptions of compactness on the nonlinear equation, and in applications, these assumptions make all differences, because, even in infinite dimensional Hilbert space it is not straightforward handedly with compact sets. However, in our applications, we overcome this difficult using a well-known criterion of compactness in L p (Ω) space [[24], Kolmogorov-Riesz-Weil theorem]. This is the principal motivation of this study.

We now turn to a summary of this study. The second section provides tools which are necessary to establish the main results that are the Theorems 2.3 and 2.4. In third section, we apply our abstract results in concrete examples.

2. Preliminaries

In this study, the symbols ( X , X ) and ( Y , Y ) stand for Banach spaces with their, respectively, norms and we denote by ( Y , X ) the Banach space of bounded linear operators from Y into X endowed with the uniform operator topology; particularly, we denote ( X ) when Y = X . we start defining the evolution operator associated with the family A(t), t [0. b].

Definition 2.1. A family of operators U(t, s), ts, t, s I is said to be an evolution family associated to the problem (2.1) if the following conditions hold:
  1. (a)

    U(t, s)U(s, r) = U(t, r) for all rst.

     
  2. (b)

    For each x X , the function (t, s) → U(t, s)x is continuous from {(t, s), ts, t, s I} into X .

     
  3. (c)

    For each t > s, the function tU(t, s) is continuous differentiable with respect to t and t U ( t , s ) = A ( t ) U ( t , s ) .

     

The family of evolution system U(t, s) is called exponential stable if there are positive constants M ̃ and α such that U ( t , s ) ( X ) M ̃ e - α ( t - s ) , for every t, s [0, b].

Throughout this study, A ( t ) : D ( A ( t ) ) X X denotes a family of unbounded closed linear operators defined in a common domain D, which is independent of t and dense in X . Moreover, we assume that the system
u ( t ) = A ( t ) u ( t ) , t s , t , s I , u ( s ) = x X ,
(2.1)

has an associated evolution family of operators U(t, s), ts, t, s I. For additional details and more properties about the family U(t, s), we refer the reader to [6, 25, 26].

To study the problem (2.1), we consider the space of normalized piecewise continuous functions P C ( [ 0 , τ ] , X ) , this means that, a function u : [ 0 , τ ] X belongs to P C ( [ 0 , τ ] , X ) if u is continuous at tt i , u ( t i - ) = u ( t i ) and u ( t i + ) < , for all i = 1,..., m. It is well known that if it is equipped with the norm u P C = sup s [ 0 , a ] u ( s ) X , then P C ( [ 0 , τ ] , X ) became a Banach space.

The technique used in this study is based on the compactness criterion. For this reason, we will make the following assumptions.

Put t0 = 0, tn+1= τ and for u P C ( [ 0 , τ ] , X ) we denote by u i ̃ P ( [ t i , t i + 1 ] ; X ) , i = 0 , , n , the function given by
ũ i ( t ) = u ( t ) , for t ( t i , t i + 1 ] , u ( t i + ) , for t = t i .

In particular, B ̃ i stands the set defined by B ̃ i = { u i ̃ , u B } , where B P C ( [ 0 , τ ] , X ) .

Lemma 2.1. ( [12]) A set B P C is relatively compact in P C if and only if the set B ̃ i is relatively compact in the space C ( [ t i , t i + 1 ] ; X ) , for every i = 0, 1,..., n.

The next step is to define the phase space. This will be done in the following way. The space , will be formed by all measurable functions φ : ( - , 0 ] X with seminorm . On the phase space we assume the following condition. Let x : ( - , b ] X , b > 0 be a function such that x0 = φ, φ and x [ 0 , b ] P C [ 0 , b ] ; X ) . Then the following properties hold true.
  1. (i)

    x t is in ;

     
  2. (ii)

    x ( t ) X H x t ;

     
  3. (iii)

    x t K ( t - σ ) s u p { x ( s ) X : σ s t } + M ( t - σ ) x σ , where H > 0 is a constant; K, M : [0, ∞) → [1, ∞), K(·) is continuous, M(·) is locally bounded and H, K, M are independent of x(·).

     

Remark 2.1. To treat retarded impulsive differential equation we suitable modified the axioms of the abstract phase space . Actually, we drop the condition of continuity of the -valued function tx t , since t x ( t ) P C in not a continuous function.

Following the ideas of [15], we used the notations K ̄ and M ̄ which is defined by
K ̄ : = sup s [ 0 , b ] K ( s ) and  M ̄ : = sup s [ 0 , b ] M ( s ) .

In what following we give some examples of phase spaces whose the above axioms are satisfied.

Example 2.1. Consider the function g(θ) = e γθ , θ ≤ 0, γ ≥ 0, and let L2([0, π], ) be the space of square integrable Lebesgue measure functions endowed with the norm ξ L 2 = ( 0 π ξ ( x ) 2 d x ) 1 2 . Then we define the phase space norm as being
B = φ : ( - , 0 ] L 2 ( [ 0 , π ] ; ) ; sup θ 0 e γ θ φ ( θ ) L 2 < ) .

If is endowed with the norm φ = sup θ 0 e γ θ φ ( θ ) L 2 , for all φ then it is well known that ( , ) is a phase space and the conditions (i)-(iii) are fulfilled. In these particular example it is possible to show that H = 1, K(t) = 1 and M(t) = e-γt, for all t ≥ 0.

Motivated by Pazy [16, 25] we adopt the following concept of mild solution to problem (1.1)-(1.3).

Definition 2.2. A function u : ( - , b ] X , b > 0 , is a local mild solution of problem (1.1)-(1.3) if the following conditions holds.
  1. (i)

    u0 = ϕ, φ ;

     
  2. (ii)

    the function u ( t ) P C ( [ 0 , b ] ; X ) , x ( t i + ) = x ( t i ) + I i ( x t i ) , for all i = 1,..., m;

     
  3. (iii)
    the integral equation below is satisfied,
    u ( t ) = U ( t , 0 ) ( φ ( 0 ) + g ( 0 , φ ) ) - g ( t , u t ) + 0 t U ( t , s ) f ( s , u s , 0 s e ( s , τ , u τ ) d τ ) d s + t i < t U ( t , t i ) I i ( u t i ) , t [ 0 , b ] ,
     

is satisfied.

The tools used in this study are based on point fixed theory. For this reason, the next two theorems play important role in the development of our results.

Theorem 2.1. [[27], Leray-Schauder Alternative] Let C be a convex subset of a Banach space X , and assume 0 C. Let F : CC be a completely continuous operator, and let
( F ) : = x C ; x = λ F ( x ) , λ ( 0 , 1 ) .

Then either ( F ) is unbounded or F has a fixed point.

Theorem 2.2. [[28], Corollary 4.3.2] Suppose that D is a closed bounded convex subset of the Banach space X and that B and C are continuous function from D to X with

(ma 1) Bx + Cx D, for all x D.

(ma 2) C ( D ) ¯ is compact set; and

(ma 3) there is a number 0 ≤ γ < 1 such that || Bx - By || ≤ γ || x - y ||, for all x, y D.

Then there is z D such that Bz + Cz = z.

Next, we stated some important conditions used in the proof of our results.

(H1) The function g : [ 0 , b ] × X satisfy the following condition

(H1.1) Let φ and consider the extension y : ( - , b ] X of ϕ which is given by
y ( t ) = φ ( t ) , t 0 , U ( t , 0 ) φ ( 0 ) , t [ 0 , b ] .
(2.2)

Then, each bounded set B of P C the family of functions {g(t, y t + u t ), t [0, b], u B} is equi-continuous.

(H1.2) There are constants c1 and c2 such that g ( t , φ ) c 1 φ + c 2 , for all t ≥ 0 and φ .

(H2) The function f : [ 0 , b ] × × X X satisfies the following conditions.

(H2.1) The function (x, ϕ) → f(t, ϕ, x) is continuous for almost everywhere t [0, b].

(H2.2) The function tf(t, ϕ, x) is strong measurable for each ( φ , x ) × X . .

(H2.3) There is a positive continuous function m : [0, b] → [0, ∞) and a nondecreasing positive continuous function ψ: → [0, ∞) such that
f ( t , φ , x ) X m ( t ) ψ ( φ + x X ) ,

for every ( t , φ , x ) [ 0 , b ] × × X .

(H3) The function e : [ 0 , b ] × [ 0 , b ] × X satisfy the following conditions.

(H3.1) The function ϕe(t, s, ϕ) is continuous almost everywhere for all t, s [0, b].

(H3.2) The function (t, s) → e(t, s, ϕ) is strong measurable for each φ .

(H3.3) There is a positive continuous function p : [0, b] → [0, ∞) and a nondecreasing integrable positive function Ω: → [0, ∞) such that
e ( t , s , φ ) X p ( s ) Ω ( φ ) ,

for all ( t , s , φ ) [ 0 , b ] × [ 0 , b ] × .

(H4) For each function u : ( - , b ] X , with u 0 and u ( ) [ 0 , b ] P C ( [ 0 , b ] ; X ) , τe(s, τ, u τ ), τ [0,b] and tf(t, u t , x), t [0, b] are measurable functions for almost everywhere s [0, b] and x X .

Now we are already to state and prove the main result of this article.

Theorem 2.3. Assume that the conditions (H1) - (H4) are satisfied. In addition, suppose that the following assumptions hold.

(t 1) The function g : [ 0 , b ] × X is completely continuous.

(t 2) The operators I i are completely continuous and there are positive constants, L i such that
I i ( x ) X L i φ ,

for all φ , x X , and i = 1,..., m.

(t3) For each bounded subsets B P C ( [ 0 , b ] ; X ) and G X the set
U ( t , s ) f ( s , x ̄ s + y s , z ) , x B , z G ,

is relatively compact for each ts, t, s [0, b], where x ̄ : ( - , b ] X is an extension of x in such manner that x ̄ ( t ) = 0 , t ≤ 0 and x ̄ ( t ) = x ( t ) , t [0, b].

If 1 - K ¯ ( M ̃ i = 1 m L i ) > 0 and
0 t ξ ( s ) d s < C ̃ d s ψ ( s ) + Ω ( s ) d s ,
where
C ̃ = ( K ¯ M ̃ + K ¯ M ̃ + M ¯ ) φ + c 2 ( M ̃ + 1 ) 1 - K ¯ ( M ̃ i = 1 m L i ) ,
and
ξ ( t ) = max ( K ¯ M ̃ + K ¯ M ̃ + M ) φ 1 - K ̃ ( M ̃ i = 1 m L i ) K ̃ M ̃ m ( t ) , p ( t ) , t [ 0 , b ] ,

then, the problems (1.1)-(1.3) have a mild solution.

Proof. Suppose that u : ( - , b ] X is a solution of (1.1)-(1.3) and let y : ( - , b ] X be a continuous extension of ϕ given in (H1). If we written the solution u(·) of the problem (1.1)-(1.3) as u(t) = x(t) + y(t), t (-∞, b], then we can see that x(t) = 0, t ≤ 0 and for t [0, b] the following integral equation hold true
x ( t ) = U ( t , 0 ) g ( 0 , φ ) - g ( t , x t + y t ) + 0 t U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s + t i < t U ( t , t i ) I i ( x t i + y t i ) , t [ 0 , b ] .
Motivated by this remark we consider the space
Λ = x : ( - , b ] X ; x ( θ ) = 0 , θ 0 , and x ( ) [ 0 , b ] P C ( [ 0 , b ] ; X ) ,
endowed with the norm x Λ = sup t [ 0 , b ] x ( t ) X . Moreover, on Λ we define the operators Γ i : Λ → Λ, i = 1, 2, 3 given by
Γ 1 x ( t ) = U ( t , 0 ) f ( 0 , φ ) - f ( t , x t + y t ) Γ 2 x ( t ) = 0 t U ( t , s ) g ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s Γ 3 x ( t ) = t i < t U ( t , t i ) I i ( x t i + y t i ) ,

for all t [0, b]. Using the fact that (U(t, s))tsis a evolution family of operators and assuming the conditions on f, g and the family of operator I i , i = 1,..., m, it is not difficult see that t → Γ i (t), t [0, b] is a normalized piecewise continuous function for all i = 1,..., m. This shows that Γ is well defined. In the next, we prove that the operator Γ = Γ1 + Γ2 + Γ3 satisfies all conditions of Theorem 2.1. As the proof is very long we split it into various steps.

Step 1. The operator 1 is completely continuous

Let x n Λ, n be a sequence of elements of Λ such that x n x as n → ∞ for some x Λ. From the boundedness of operators U(t, s) and the axioms of the phase space it is easy to see that the set x t n , x t , n , t [ 0 , b ] is bounded in , which implies from condition (H1) the uniformity convergence of
g ( t , x t n + y t ) g ( t , x t + y t ) , as n

on [0, b]. Thus, we have the continuity of Γ1. From condition (H 1), and the axiom (iii) follows immediately the Γ1 applies bounded sets of Λ into equi-continuous sets of Λ. On the other hand, again by (iii), and using the fact that f is a completely continuous function, soon as infers that, for each t [0, b], the set {g(t, x t + y t ), x B} is compact in X . The proof that Γ1 is a completely continuous operator is complete.

Step 2. The operator Γ2 is complete continuous

The condition (H3.1) permit us conclude that e ( t , s , x n s ) e ( t , s , x s ) as n → ∞ almost everywhere for t, s [0, b]. By (H3.3), and the Lebesgue's dominated convergence theorem we conclude that
0 t e ( t , s , x n s ) d s 0 t e ( t , s , x s ) d s ,
uniformly for t [0, b]. From the strong continuity of the operators (U(t, s))ts, we can conclude that
0 t U ( t , s ) f ( s , x s n + y s , 0 s e ( s , τ , x τ n + y τ ) d τ ) d s 0 t U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s ,
as n → ∞, uniformly for t [0, b]. This fact and the properties of the evolution family U(t, s) lead us to the continuity of the operator Γ2. Next, we show that Γ2 takes bounded sets into equi-continuous sets. First, we observe from conditions (H2.3), (H3.3) and the axioms of phase space that
e ( t , s , x s + y s ) , t , s [ 0 , b ] , x B ,
and
f ( t , x t + y t , 0 t e ( t , s , x s + y s ) d s ) ; t , s [ 0 , b ] , x B
(2.3)

are bounded sets in X .

Let ε > 0 be the arbitrary positive real number and t1, t2 [0, b], t1 > t2. Thus, take into account the previous notes and using the assumption (iii) we see that the set
U ( t 2 - ε , s ) g ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s , s [ 0 , t 2 - ε / 2 ] , x B
is relatively compact in X . Thus we have
Γ 2 u ( t 2 ) - Γ 2 u ( t 1 ) 0 t 2 - ε 2 [ U ( t 1 , t 2 - ε ) - U ( t 2 , t 2 - ε ) ] U ( t 2 - ε , s ) g ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s + t 2 t 2 - ε 2 [ U ( t 1 , s ) - U ( t 2 , s ) ] g ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s + t 2 t 1 U ( t 1 , s ) g ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s ,
thus, from the continuity of U(t, s) and the assumptions of compactness contained on the condition (t 3) we can infer the existence of 0 < δ < ε such that if |t1 - t2| < δ then
Γ 2 x ( t 1 ) - Γ 2 x ( t 2 ) ε ( t 2 - ε 2 ) + 2 ε 2 M ̃ sup s [ 0 , b ] f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s + ε M ̃ sup s [ 0 , b ] f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s .
This shows the equi-continuity of Γ2. In what follows, we show that for each t [0, b] the set
Θ ( t ) = 0 t U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s , x B ,
(2.4)
where B Λ, is pre-compact in Λ. To do that, we observe from (2.3) that for each s [0, t] the set
f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) , x B
is a bounded set. Then,
0 t U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s = 0 t - ε U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s + t - ε t U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s ,
which implies by [[28], Lemma 1.3]
0 t U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s t c o ̃ U ( t , s ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) , s [ 0 , t ] + C ε ,

with diam(C ε ) < ε, where diam(·) denotes the diameter of the set C ε and co {·} the convex hull. Taking all this into account we see that for each fixed t [0, b], the set Θ(t) in (2.4) is relatively compact set in X . This completes the proof that the operator Γ2 is completely continuous.

Step 3. The operator Γ3 is completely continuous

To show that is Γ3 is a completely continuous, consider a bounded subset B of Λ and for each i = 1,..., m, define the set Π ̃ i C ( [ t i , t i + 1 ] ; X ) as
Π ̃ i = j = 1 i - 1 U ( t , t j ) I j ( x t j ) , t [ t i , t i + 1 ] , x B ̃ i .
To prove that the sets Π ̃ i , i = 1,..., m, are precompacts in C ( [ t i , t i + 1 ] ; X ) , consider t1, t2 (t i , ti+1], t1 > t2. Using the continuity of (t, s) → U (t, s)x, and the compactness of sets I j (B), j = 1,..., m, given ε > 0 there is 0 < δ < ε such that if |t1 - t2| < δ we have
j = 1 i ( U ( t 1 , t j ) - U ( t 2 , t j ) ) I j ( x t j ) n ε ,
uniformly for x B. On the other hand for t (t i , ti+1) fixed, from our hypothesis it is not difficult see that the set
Π ̃ i ( t ) = j = 1 i U ( t , t j ) I j ( x t j ) , x B ,

is relatively compact in X

On the other hand, if t = t i , the set Π ̃ i ( t i ) became
Π ̃ i ( t i ) = j = 1 i - 1 U ( t , t j ) I j ( x t j ) , x B . ,
and proceeding as in the early case we infer that the set Π ̃ i ( t i ) is relatively compact in X , The prove that the set
j = 1 i - 1 ( U ( t i , t j ) - U ( t 2 , t j ) ) I j ( x t j )

is an equi-continuous set of functions is done in the same manner as at the beginning

of the section. The proof that Γ3 is completely continuous is finished.

In the next, we obtain a priori estimative of the solutions for the equation λ Γx λ = x λ , for λ (0, 1) and = Γ = Γ1 + Γ2 + Γ3. Let x be a solution of the equation λ Γ(x λ ) = x λ , in addition we use the notation m λ ( t ) = K ¯ sup s [ 0 , t ] x ( s ) + ( K ¯ M ̃ + M ¯ ) φ , then we have
x ( t ) U ( t , 0 ) ( X ) g ( 0 , φ ) + g ( t , x t + y t ) + 0 t U ( t , s ) ( X ) f ( s , x s + y s , 0 s e ( s , τ , x τ + y τ ) d τ ) d s + t j < t U ( t , t j ) ( X ) I j ( x t j ) ( X ) M ̃ φ + c 1 m λ ( t ) + c 2 ( M ̃ + 1 ) + M ̃ 0 t m ( s ) ψ ( m λ ( s ) + 0 s p ( τ ) Ω ( m λ ( τ ) ) d τ ) d s + M ̃ t i < t L i m λ ( t ) ,
this implies that
m λ ( t ) ( K ¯ M ̃ + K ¯ M ̃ + M ¯ ) φ + c 2 ( M ̃ + 1 ) 1 - K ¯ ( M ̃ i = 1 m L i ) + ( K ¯ M ̃ + K ¯ M ̃ + M ¯ ) φ 1 - K ¯ ( M ̃ i = 1 m L i ) M ̃ K ¯ 0 t m ( s ) ψ ( m λ ( s ) + 0 s p ( τ ) Ω ( m λ ( τ ) ) d τ ) d s .
If we take the right-hand side of the previous inequalities and call it of v(t) we have that m λ (t) ≤ v(t), for all t [0, b]. This leads us to the following inequality:
v ( t ) ( K ¯ M ̃ + K ¯ M ̃ + M ¯ ) φ + c 2 ( M ̃ + 1 ) 1 - K ¯ ( M ̃ i = 1 m L i ) + ( K ¯ M ̃ + K ¯ M ̃ + M ¯ ) φ 1 - K ¯ ( M ̃ i = 1 m L i ) K ¯ M ̃ 0 t m ( s ) ψ ( v ( s ) + 0 s p ( τ ) Ω ( v ( τ ) ) d τ ) d s ,
this yields
v ( t ) ( K ¯ M ̃ + K ¯ M ̃ + M ¯ ) φ 1 - K ¯ ( M ̃ i = 1 m L i ) K ¯ M ̃ m ( t ) ψ ( v ( t ) + 0 t p ( τ ) Ω ( v ( τ ) ) d τ ) .
Next, we considered the function ϖ ( t ) = v ( t ) + 0 t p ( s ) Ω ( v ( s ) ) d s , thus we have that v(0) = ϖ(0) and v(t) ≤ ϖ(t), for all t [0, b], using this and the non-decreasingly properties of the function ψ(·), we get
ϖ ( t ) ( K ¯ M ̃ + K ¯ M ̃ + M ¯ ) φ 1 - K ¯ ( M ̃ i = 1 m L i ) K ¯ M ̃ m ( t ) ψ ( ϖ ( t ) ) + p ( t ) Ω ( ϖ ( t ) ) , t [ 0 , b ] .
Observe that if we define the function ξ ( t ) = max { ( K ̃ M ̃ + K ̃ M ̃ + M ) φ 1 - K ̃ ( M ̃ i = 1 m L i ) K ̃ M ̃ m ( t ) , p ( t ) } , t [ 0 , b ] then we have
ϖ ( t ) ξ ( t ) ψ ( ϖ ( t ) ) + Ω ( ϖ ( t ) ) ,
which implies that
ϖ ( t ) ψ ( ϖ ( t ) ) + Ω ( ϖ ( t ) ) ξ ( t ) ,
for all t [0, b]. Integrating the early inequality from 0 to t we have
ϖ ( 0 ) ϖ ( t ) d s ψ ( s ) + Ω ( s ) 0 t ξ ( s ) d s < ϖ ( 0 ) d s ψ ( s ) + Ω ( s ) .

The early inequalities enable us to conclude that the set {x λ , x λ = Γx λ , λ (0, 1)} is bounded. From Theorem 2.1 the problem (1.1)-(1.3) has a mild solution. The proof of theorem is completed.   □

In the next result, the following conditions are used.

(G 1 ) There is a positive constant L f such that
g ( t , φ ) - g ( t , ψ ) X L g φ - ψ ,

for every t [0, b] and φ , ψ .

(G 2 ) There are positive constants d i , i = 1,..., m, such that
I i ( x ) - I i ( y ) X d i x - y X ,

for every x, y X ..

Theorem 2.4. Assume that the condition (H 2)-(H 3) and (G1)-(G2) are satisfied. In addition, suppose that the assumption (iii) of Theorem (2.3) is satisfied. Then if
L g K ¯ + K ¯ M ̃ lim inf ξ ψ ( ξ + Ω ( ξ ) 0 b p ( τ ) d τ ) ξ 0 b m ( s ) d s + M ̃ K ¯ i = 1 n d i < 1 ,
and
( L g + M ̃ i = 1 n d i ) < 1 ,

then the problem (1.1)-(1.3) has a mild solution.

Proof. Let us consider the operator Γ: Λ → Λ defined as in Theorem 2.3. We claim that there is r > 0 such that Γ(B r ) B r . Suppose by contradiction that this assumption is false. Then for each r > 0 there are t r [0, b] and u r (·) B r such that Γ ( u r ) ( t r ) X r . This implies that
r M ̃ ( H φ + g ( 0 , φ ) X ) + M ̃ 0 t r f ( s , u s r + y s , 0 s e ( s , τ , u τ r + y τ ) d τ ) d s + t i < t r U ( t r , t i ) I i ( u t i r + y t i ) + g ( t r , u t r r + y t r ) X M ̃ ( H φ + g ( 0 , φ ) X ) + L g ( K ¯ r + ( K ¯ M ̃ H + M ¯ ) φ ) + sup s [ 0 , b ] g ( s , 0 ) + M ̃ ψ ( K ¯ r + ( K ¯ M ̃ H + M ¯ ) φ + Ω ( K ¯ r + ( K ¯ M ̃ H + M ¯ ) φ ) 0 b p ( τ ) d τ ) 0 b m ( s ) d s + M ̃ i = 1 n ( d i ( K ¯ r + ( K ¯ M ̃ H + M ¯ ) φ ) + I i ( 0 ) X ) ,
take the lim inf in the previous inequality, we have
1 L g K ¯ + K ¯ M ̃ liminf ξ ψ ( ξ + Ω ( ξ ) 0 b p ( τ ) d τ ) ξ 0 b m ( s ) d s + M ̃ K ¯ i = 1 n d i ,
which is contradictory with our assumptions. So let r > 0 be such a number and consider the restriction Γ B r of the operator Γ on B r , that is, Γ B r : B r B r Next, we split the operator Γ in the following way Γ = Γ1 + Γ2, where
Γ 1 ( u ) = U ( t , 0 ) ( φ ( 0 ) + g ( 0 , φ ) ) - g ( t , u t + y t ) + t i < t U ( t , t i ) I i ( u t i + y t i ) , t [ 0 , b ] and Γ 2 ( u ) = 0 t U ( t , s ) f ( s , u s + y s , 0 s e ( s , τ , u τ + y τ ) d τ ) d s , t [ 0 , b ] .
As shown in the proof of Theorem 2.3, it is not difficult to see that Γ2 is completely continuous and for u1, u2 Λ we have that
Γ 1 ( u 1 ) ( t ) - Γ 1 ( u 2 ) ( t ) X L f u t 1 - u t 2 + M ̃ i = 1 n d i u t i 1 - u t i 2 ( L f + M ̃ i = 1 n d i ) u 1 - u 2 Λ .

The previous inequality shows that Γ1 is contractive. Now, by Theorem 2.2, we can conclude that the problem (1.1)-(1.3) has a mild solution.   □

3. Applications

The main aim of this section is to apply our abstract results in concrete examples. To this end, we handle with a very special kind of operators. To be more specific, on the Banach space X = L 2 ( [ 0 , π ] , ) we define the operator A : D ( A ) X given by Ax(ξ) = x"(ξ), ξ [0, π] with domain
D ( A ) = x X ; x X and x ( 0 ) = x ( π ) = 0 .
It is well known that in this case A has a discrete spectrum which is given by -n2, n . Moreover, X has a completely orthonormal base formed by eigenfunctions of A associated with the eigenvalues -n2, which is given x n ( ξ ) = 2 π sin ( n ξ ) , n . This implies that the following conditions are satisfied.
  1. (i)

    For each f X , n = 1 f , x n x n ( ξ ) ,

     
  2. (ii)

    For each f D(A), we have A f ( ξ ) = - n = 1 n 2 f , x n x n ( ξ ) ,

     
where 〈·,·〉 represents the inner product in X . Taking into account all these information, it is possible to prove that the operator A is the infinitesimal generator of a compact semigroup of bounded linear operators (T(t))t ≥ 0, which is given by
T ( t ) f ( ξ ) = n = 1 e - n 2 t f , x n x n ( ξ ) , t 0 , ξ [ 0 , π ] .
To guarantee the existence of an evolution family associated with the problem
u ( t ) = A ( t ) u ( t ) , t s , t , s [ 0 , b ] u ( s ) = x X ,
(3.1)

the following assumptions on the function a0 : [0, b] × [0, π] → are made

( a 1 ) There are constants c > 0 and α (0, 1) such that
a 0 ( t , ξ ) - a 0 ( s , ξ ) t - s α ,

for all t, s [0, b] and almost everywhere ξ [0, π].

( b 0 ) there is a real number c0 such that
a 0 ( τ , ξ ) c 0 ,

for all τ [0, ∞) and ξ [0, π].

Letting D(A(t)) = D(A) for all t ≥ 0 and A(t)x(ξ) = a0(t, ξ)x"(ξ), ξ [0, π], we have that the system (3.1) has an associated evolution family of operators (U(t, s))tswhich is given explicitly by the following formula:
( U ( t , s ) f ) ( ξ ) = n = 0 e - n 2 s t a 0 ( τ , ξ ) d τ f , x n x n ( ξ ) , ξ [ 0 , π ] , t [ 0 , b ] .
Using the properties of semigroup (T(t))t ≥ 0it is straightforward to show that U(t, s) satisfies the condition
U ( t , s ) ( X ) e - c 0 ( t - s ) , t s .
Next, we consider the following partial differential equations
t u ( t , ξ ) + 0 ξ 0 t k 1 ( s , ξ 1 ) u ( s , ξ 1 ) sin ( ξ ) d s d ξ 1 = a 0 ( t , ξ ) 2 ξ 2 u ( t , ξ ) + 0 ξ 0 t k 1 ( s , ξ 1 ) u ( s , ξ 1 ) sin ( ξ ) d s d ξ 1 + - t k 2 ( - s ) P 2 ( s , u ( t , ξ ) ) d s + 0 t - s k 3 ( t - δ ) P 3 ( δ - t , u ( t , ξ ) d δ d s ) , u ( t , 0 ) = u ( t , π ) = 0 , s [ 0 , π ] , u ( s , ξ ) = φ ( s , ξ ) , s 0 , ξ [ 0 , π ] , u ( t i + , ξ ) = u ( t i , ξ ) + 0 ξ k 4 , i ( ξ ) u ( t i , ξ 1 ) d ξ 1 , i = 1 , , m .
(3.2)

To model the problem (3.2) we choose as the phase space the set formed by all piecewise continuous functions φ : ( - , 0 ] X which sups ≤ 0h(θ) || φ(s) || < ∞, where h(θ) = e βθ , θ ≤ 0, and we denote this space by h equipping it with the norm φ h = sup s 0 h ( s ) φ ( s ) . In order to show that the conditions (H1)-(H4) are satisfied we needed to consider the following assumptions.

( p 1 ) The function P2 : (-∞, 0] × → [0, ∞) satisfies the following conditions:

( p 1.1 ) for each η , sP2(s, η ) is a measurable and bounded function,

( p 1.2 ) there is a positive constant L P 2 such that
P 2 ( s , η 1 ) - P 2 ( s , η 2 ) L P 2 η 1 - η 2 ,

for all s ≤ 0, and η i , i = 1, 2.

( p 2 ) The functions s 0 π k 1 ( s , ξ 1 ) d ξ 1 and ξ - b 0 k 1 ( s , ξ ) d s are bounded almost everywhere on [-b, 0] × [0, π], s 0 π k 1 ( s , ξ 1 ) 2 e - β s d ξ 1 is integrable on the interval [-b, 0].

( p 3 ) k2(·) L((-∞, π]) and sP2(s, η ) is measurable and bounded function for each η . In addition we assume the existence of positive constant L P 2 such that the following inequality hold true
P 2 ( s , η 2 ) - P 2 ( s , η 1 ) L P 2 η 2 - η 1 ,

for almost everywhere s (-∞, 0] and η i [0, π], i = 1, 2.

( p 4 ) The function P3 : [-π, ∞) × satisfies the following conditions.

( p 4.1 ) for each η , sP3(s, η ), s [-∞, b), is a measurable and bounded function,

( p 4.2 ) there is a positive constant L P 3 such that
P 3 ( t , η 2 ) - P 3 ( t , η 1 ) L P 3 η 2 - η 1 ,

for all s [-π, ∞) and η i , i = 1, 2.

( p 4.3 ) The function k3(·) L([-π, ∞)).

To transform the problem (3.2) into the abstract system (1.1), we define the functions g : [ 0 , b ] × h X , f : [ 0 , b ] × × X X , e : [ 0 , T ] × [ 0 , T ] × h X and I i : X , i = 1, 2,..., n, respectively, given by,
g ( t , φ ) ( ξ ) = 0 ξ - t 0 φ ( s , ξ 1 ) sin ( ξ ) d s , t [ 0 , ) , ξ [ 0 , π ] , f ( t , φ , x ) ( ξ ) = - 0 k 2 ( - s ) P 2 ( s , φ ( 0 , ξ ) ) d s + x ( ξ ) , t [ 0 , b ] , ξ [ 0 , π ] e ( t , s , φ ) ( ξ ) = - s k 3 ( t - τ ) P 3 ( τ , φ ( 0 , ξ ) ) d τ , t , s [ 0 , T ] , ξ [ 0 , π ] , I i ( φ ) ( ξ ) = 0 ξ k 4 , i ( ξ ) φ ( 0 , ξ 1 ) d ξ 1 .
We shall show that the condition (H1) hold true. In fact, let x : (-∞, π] → L1(0, π) be a bounded function such that x [ 0 , π ] P C ( [ 0 , π ] ; L 1 ( 0 , π ) ) we have
g ( t + h , x t + h ) ( ξ ) - g ( t , x t ) ( ξ ) 0 ξ t t + h x ( s , ξ 1 ) sin ( ξ ) d s d ξ t t + h 0 ξ x ( s , ξ 1 ) 2 d ξ 1 1 2 0 ξ k 1 ( s , ξ 1 ) 2 d ξ 1 1 2 sin ( ξ ) d s sup s [ - b , 0 ] 0 π x ( s , ξ 1 ) 2 d ξ 1 1 2 t t + h 0 π k 1 ( s , ξ 1 ) 2 d ξ 1 1 2 sin ( ξ ) d s .
The previous inequalities jointly with the assumption ( p 2 ) show that the function tg(t, x t ) is uniformly continuous on bounded subsets of P C ( [ 0 , b ] , L2(0, π)) which implies that the condition (H1.1) hold true. To prove that the condition (H1.2) is satisfied, we observe that
g ( t , φ ) ( ξ ) 0 ξ - t 0 k 1 ( s , ξ 1 ) φ ( s , ξ 1 ) d s d ξ 1 - t 0 0 ξ k 1 ( s , ξ 1 ) 2 e - β s d ξ 1 1 2 0 ξ φ ( s , ξ 1 ) 2 e β s d ξ 1 1 2 d s sup s 0 0 ξ φ ( s , ξ 1 ) 2 e β s d ξ 1 1 2 - t 0 0 π k 1 ( s , ξ 1 ) 2 e - β , s d ξ 1 1 2 d s ,

which implies the condition (H1.2).

The next step is a proof that the function (x, ϕ) → f(t, ϕ, x) is continuous. However, with the help of condition ( p 2 ) we have
0 π f ( t , φ 2 , x 2 ) ( ξ ) - f ( t , φ 1 , x 1 ) ( ξ ) 2 4 L P 2 0 π φ 2 ( 0 , ξ ) - φ 1 ( 0 , ξ ) 2 d ξ + 4 0 π x 2 ( ξ ) - x 1 ( ξ ) 2 d ξ 4 L P 2 sup s 0 0 π e β s φ 2 ( s , ξ ) - φ 1 ( s , ξ ) 2 d ξ + 4 0 π x 2 ( ξ ) - x 1 ( ξ ) 2 d ξ ,
for all φ i , x i X , i = 1, 2. Thus we have shown that the condition (H2.1) is fulfilled. In particular, as P2 is continuous in the second variable we have that for each ( φ , x ) × X fixed the function ξ - 0 k 2 ( - s ) P 2 ( s , φ ( 0 , ξ ) ) d s is measurable. Thus from [[24], Theorem 1.2.1] we infer that tf(t, ϕ, x) is measurable for each ( φ , x ) × X . On the other hand, assuming that sP2(s, 0), s (-∞, 0] is bounded function, we have that
f ( t , φ , x ) ( ξ ) 2 4 L P 2 φ ( 0 , ξ ) - 0 k 2 ( - s ) d s 2 + 16 - 0 k 2 ( - s ) P 2 ( s , 0 ) d s 2 + 16 x ( ξ ) 2 ,
which implies that
f ( t , φ , x ) X 4 L P 2 - 0 k 2 ( - s ) d s 2 , 4 π - 0 k 2 ( - s ) P 2 ( s , 0 ) d s 2 , 4 1 2 ( φ + x X ) .
(3.3)

Thus the condition (H2.3) is fulfilled.

On the other hand, the same idea applied to prove that the previous functions is of Caratheádory type can be used to show that function e(·,·,·) satisfies the same property. Here it is mentioned that the functions that appear in the condition (H3.3) are given by
e ( t , s , φ ) X 4 max L P 2 - s k 2 ( - δ ) d δ 2 , 4 π - s k 2 ( - δ ) P 2 ( δ , 0 ) d δ 2 , 4 1 2 φ .
(3.4)
Finally, it remains that the condition (H 4) is valid. However, we observe that
h L h ( ( - , 0 ] , L 2 ( ( 0 , π ) ) ) ,
where a function ϕ : (-∞, 0] → L2(0, π) is an element of L h ( ( - , 0 ] , L2(0, π)) if and only if
e s s sup s 0 0 π h ( s ) φ 2 ( s , ξ ) d ξ < ,
with the norm defined by φ L h = inf { a ; μ { θ ( - , 0 ] ; φ L 2 > a } = 0 } , where μ = hdξ, and representing the Lebesgue measure on (-∞, 0]. Thus, following the ideas of [[29], Theorem 3.8] and using the fact that h(θ - t) ≤ G(-t)h(θ), θ ≤ 0, G(-t) = e-βt, t ≥ 0, we see that if u : (0, -∞] → L2(0, π) is admissible function in the sense of [29], then we derive the mensurability of tu t , t [0, b]. Thus, as e(·,·,·) and f(·,·,·) are measurable functions we infer that τe(t, τ, u τ ) and τf(t, u τ , x) for all t, τ [0, b], x L2(0, π). Now we will see that the conditions of the Theorem 2.3 hold. To see this, we observe that
g ( t , φ ) ( ξ + h ) - g ( t , φ ) ( ξ ) 0 ξ - t 0 φ ( s , ξ 1 ) ( sin ( ξ + h ) - sin ( ξ ) ) d s d ξ 1 + ξ ξ + h - t 0 φ ( s , ξ 1 ) sin ( ξ ) d s d ξ 1 ,
taking the advantage of the previous inequality we have
g ( t , φ ) ( ξ + h ) - g ( t , φ ) ( ξ ) b sup s 0 0 π e β s φ ( s , ξ 1 ) 2 d ξ 1 0 π - h ( sin ( ξ + h ) - sin ( ξ ) ) d s + b h sup s 0 0 π e β s φ ( s , ξ 1 ) 2 d ξ 1 2 sin ( ξ + h ) d s ,

which implies from [[24], Theorem A.5.2] the assumption (t1).

The same idea which was used to prove the compactness of the function g can be used to prove that compactness of the operators I i , i = 1,..., m. Regarding the inequality that appear in the condition (t 2), we observe that to exhibit explicitly the c i constants, i = 1,..., m, the following account is necessary
I i ( φ ) 2 π φ 2 0 π k 4 , i 2 ( ξ ) d ξ ,

for all i = 1,..., m.

As we choose the phase space as being h , then it is possible to show that the constant H and the functions K(·) and M(·) that appear in the axioms (ii) and (iii) are given, respectively, by H = 1, K(t) = 1 and M(t) = e-βt, for all t ≥ 0.

Taking into account what was said before we derive the following result.

Theorem 3.1. Assume that all previous conditions are fulfilled. Assume in addition that the following inequalities hold,
3 φ 1 - i = 1 m L i b p ( s ) d s < ,

where p(·) represents the right-hand side of the inequalities (3.4). Then the problem (3.2) has a mild solution.

Declarations

Authors’ Affiliations

(1)
Departamento De Matemática, Universidade Federal De Pernambuco
(2)
Faculdade De Ciência E Tecnologia De Caruaru, Universidade De Pernambuco

References

  1. Bainov DD, Pavel S: Impulsive Differential Equations: Periodic Solutions and Applications. In: Pitman Monographs and Surveys in Pure and Applied Mathematics. Volume 66. Longman Scientific & Technical, Harlow, UK; 1993:x+228.Google Scholar
  2. Samoilenko AM, Perestyuk NA: Impulsive Differential Equations. World Scientific, Singapore; 1995.Google Scholar
  3. Lakshmikanthan V, Bainov D, Simeonov P: Theory of Impulsive Differential Equations. In series in Modern Applied Mathematics. World Scientific, Teaneck, NJ 1989., 6:Google Scholar
  4. Park JY, Balachandran K, Annapoorani N: Existence results for impulsive neutral functional integrodifferential equations with infinite delay. Nonlinear Anal 2009, 71: 3152–3162. 10.1016/j.na.2009.01.192MATHMathSciNetView ArticleGoogle Scholar
  5. Balachandran K, Annapoorani N: Existence results for impulsive neutral evolution integrodifferential equations with infinite delay. Nonlinear Anal Hybrid Syst 2009, 3: 674–684. 10.1016/j.nahs.2009.06.004MATHMathSciNetView ArticleGoogle Scholar
  6. Schnaubelt R: Asymptotic behavior of parabolic nonautonomous evolution equations. In Functional Analytic Methods for Evolution Equations. Lecture Notes in Mathematics. Volume 1855. Springer, Berlin; 2004:401–472.View ArticleGoogle Scholar
  7. Hernández E, Prokopezyk A, Ladeira L: A note on partial functional differential equations with state-dependent delay. Nonlinear Anal Real World Appl 2006,7(4):510–519. 10.1016/j.nonrwa.2005.03.014MATHMathSciNetView ArticleGoogle Scholar
  8. Baghli S, Benchohra M: Perturbed functional and neutral functional evolution equations with infinite delay in Fréchet spaces. Elec J Differ Equ 2008, 69: 1–19.MathSciNetView ArticleGoogle Scholar
  9. Ahmad S, Stamov GT: Almost periodic solutions of N -dimensional impulsive competitive systems. Nonlinear Anal Real World Appl 2009,10(3):1846–1853. 10.1016/j.nonrwa.2008.02.020MATHMathSciNetView ArticleGoogle Scholar
  10. Ahmad S, Stamov GT: On almost periodic processes in impulsive competitive with delay and impulsive perturbations. Nonlinear Anal Real World Appl 2009,10(5):2857–2863. 10.1016/j.nonrwa.2008.09.003MATHMathSciNetView ArticleGoogle Scholar
  11. Hernádez E, Henráquez H: Existence of periodic solutions of partial neutral functional differential equations with unbounded delay. J Math Anal Appl 1998,221(1):499–522.MathSciNetView ArticleGoogle Scholar
  12. Hernïández E, Pierri M, Gonáalves G: Existence results for an impulsive abstract partial differential equation with state-dependent delay. Comput Math Appl 2006,52(3–4):411–420. 10.1016/j.camwa.2006.03.022MathSciNetView ArticleGoogle Scholar
  13. Hernández E, Rabelo M, Henráquez H: Existence of solutions for impulsive partial neutral functional differential equations. J Math Anal Appl 2007, 331: 1135–1158. 10.1016/j.jmaa.2006.09.043MATHMathSciNetView ArticleGoogle Scholar
  14. Chang YK, Anguraj A, Arjunan MM: Existence results for impulsive neutral functional differential equations with infinite delay. Nonlinear Anal Hybrid Syst 2008, 2: 209–218. 10.1016/j.nahs.2007.10.001MATHMathSciNetView ArticleGoogle Scholar
  15. Cuevas C, Hernández E, Rabelo M: The existence of solutions for impulsive neutral functional differential equations. Comput Math Appl 2009,58(4):744–757. 10.1016/j.camwa.2009.04.008MATHMathSciNetView ArticleGoogle Scholar
  16. Hernández E, Hernráquez HR: Impulsive partial neutral differential equations. Appl Math Lett 2006, 19: 215–222. 10.1016/j.aml.2005.04.005MATHMathSciNetView ArticleGoogle Scholar
  17. Hernádez E, McKibben M, Henráquez HR: Existence results for abstract impulsive second order neutral functional differential equations. Nonlinear Anal Theory Methods Appl 2009,70(7):2736–2751. 10.1016/j.na.2008.03.062View ArticleGoogle Scholar
  18. Stamov GT: On the existence of almost periodic solutions for the impulsive Lasota-Wazewska model. Appl Math Lett 2009,22(4):516–520. 10.1016/j.aml.2008.07.002MATHMathSciNetView ArticleGoogle Scholar
  19. Stamov GT: Almost periodic models of impulsive Hopfield neural networks. J Math Kyoto Univ 2009,49(1):56–67.MathSciNetGoogle Scholar
  20. Stamov GT: Stability processes of moving invariant manifolds in uncertain impulsive differential-difference equations. Math Bohem 2009,134(1):67–76.MATHMathSciNetGoogle Scholar
  21. Stamov GT: Existence of almost periodic solutions for impulsive cellular neural networks. Rocky Mountain J Math 2008,38(4):1271–1284. 10.1216/RMJ-2008-38-4-1271MATHMathSciNetView ArticleGoogle Scholar
  22. Benchohra M, Slimani BA: Existence and uniqueness of solutions to impulsive fractional differential equations. Elec J Differ Equ 2009,2009(10):11.MathSciNetGoogle Scholar
  23. Agarwal RP, Benchohra M, Slimani BA: Existence results for differential equations with fractional order and impulses. Mem Diff Equ Math Phys 2008, 44: 1–21.MATHMathSciNetGoogle Scholar
  24. Vrabie II: C 0 -semigroups and applications. North-Holland Mathematics Studies. Volume 191. North-Holland Publishing Co., Amsterdam; 2003:xii+373.Google Scholar
  25. Pazy A: Semigroups of linear operators and applications to partial differential equations. In Applied Mathematical Sciences. Volume 44. Springer, New York; 1983.Google Scholar
  26. Lunardi A: Analytic Semigroups and Optimal Regularity in Parabolic Problems. In Progress in Nonlinear Differential Equations and Their Applications. Volume 16. Birkháauser Verlag, Basel; 1995.Google Scholar
  27. Granas A, Dugundji J: Fixed Point Theory. Springer, New York; 2003.View ArticleGoogle Scholar
  28. Martin RH Jr: Nonlinear Operators and Differential Equations in Banach Spaces. In Pure and Applied Mathematics. Wiley, New York; 1976:xi+440.Google Scholar
  29. Hino Y, Murakami S, Naito T: Functional-Differential Equations with Infinite Delay. Lectures Notes in Mathematics. Volume 1473. Spring, New York; 2003.Google Scholar

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