Research Article An Existence Result for Nonlocal Impulsive Second-Order

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Hindawi Publishing Corporation
Abstract and Applied Analysis
Volume 2013, Article ID 724854, 8 pages
http://dx.doi.org/10.1155/2013/724854
Research Article
An Existence Result for Nonlocal Impulsive Second-Order
Cauchy Problems with Finite Delay
Fang Li and Huiwen Wang
School of Mathematics, Yunnan Normal University, Kunming 650092, China
Correspondence should be addressed to Fang Li; fangli860@gmail.com
Received 1 October 2012; Revised 7 December 2012; Accepted 9 December 2012
Academic Editor: Toka Diagana
Copyright © 2013 F. Li and H. Wang. This is an open access article distributed under the Creative Commons Attribution License,
which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
We deal with the existence of mild solutions of a class of nonlocal impulsive second-order functional differential equations with
finite delay in a real Banach space X. An existence result on the mild solution is obtained by using the theory of the measures of
noncompactness. An example is presented.
1. Introduction
The Cauchy problem for various delay equations in Banach
spaces has been receiving more and more attention during
the past decades (see, e.g., [1–5]).
The literature concerning second- and higher-order ordinary functional differential equations is very extensive. We
only mention the works [1, 6–15], which are directly related
to this work.
On the other hand, the impulsive conditions have advantages over traditional initial value problems because they can
be used to model phenomena that cannot be modeled by
traditional initial value problems, such as the dynamics of
populations subject to abrupt changes (harvesting, diseases,
etc.) (see [16–27] and references therein). For this reason,
the theory of impulsive differential equations has become
an important area of investigation in recent years. Partial
differential equations of first and second order with impulses
have been studied by Rogovchenko [26], Liu [25], Cardinali
and Rubbioni [19], Liang et al. [24], Henrı́quez and Vásquez
[1], Hernández et al., [21–23], Arthi and Balachandran [17],
and so forth.
Moreover, we consider the nonlocal condition π‘₯(0) =
𝑔(π‘₯) + π‘₯0 , where 𝑔 is a mapping from some space of functions
so that it constitutes a nonlocal condition (see [24, 28–30]
and the references therein), where it is demonstrated that
nonlocal conditions have better effects in applications than
traditional initial value problems.
In this paper, we pay our attention to the investigation
of the existence of mild solutions to the following impulsive
second-order functional differential equations with finite
delay in a real Banach space 𝑋:
𝑑2
π‘₯ (𝑑) = 𝐴π‘₯ (𝑑) + 𝑓 (𝑑, π‘₯𝑑 , π‘₯ (𝑑)) ,
𝑑𝑑2
(1)
𝑑 ∈ (0, 𝑇] , 𝑑 =ΜΈ π‘‘π‘˜ , π‘˜ = 1, 2, . . . , 𝑝,
π‘₯ (𝑑) = 𝑔 (π‘₯) (𝑑) + πœ™ (𝑑) ,
𝑑 ∈ [−π‘Ÿ, 0] ,
π‘₯σΈ€  (0) = πœ‰ ∈ 𝑋,
Δπ‘₯ (π‘‘π‘˜ ) = πΌπ‘˜ (π‘₯ (π‘‘π‘˜ )) ,
π‘˜ = 1, 2, . . . , 𝑝,
(2)
(3)
(4)
where 𝐴 is the infinitesimal generator of a strongly continuous cosine family of bounded linear operators {𝐢(𝑑)}𝑑∈R
on 𝑋. 𝑓, 𝑔 are given functions to be specified later. πœ™ ∈
𝐢([−π‘Ÿ, 0], 𝑋), where 𝐢([π‘Ž, 𝑏], 𝑋) denotes the space of all
continuous functions from [π‘Ž, 𝑏] to 𝑋.
The impulsive moments {π‘‘π‘˜ } are given such that 0 = 𝑑0 <
𝑑1 < ⋅ ⋅ ⋅ < 𝑑𝑝 < 𝑑𝑝+1 = 𝑇, πΌπ‘˜ : 𝑋 → 𝑋 (π‘˜ = 1, 2, . . . , 𝑝)
are appropriate functions, Δπ‘₯(π‘‘π‘˜ ) represents the jump of a
function π‘₯ at π‘‘π‘˜ , which is defined by Δπ‘₯(π‘‘π‘˜ ) = π‘₯(π‘‘π‘˜+ ) − π‘₯(π‘‘π‘˜− ),
where π‘₯(π‘‘π‘˜+ ) and π‘₯(π‘‘π‘˜− ) are, respectively, the right and the left
limits of π‘₯ at π‘‘π‘˜ .
For any continuous function π‘₯ defined on the interval
[−π‘Ÿ, 𝑇] and any 𝑑 ∈ [0, 𝑇], we denote by π‘₯𝑑 the element of
𝐢([−π‘Ÿ, 0], 𝑋) defined by π‘₯𝑑 (πœƒ) = π‘₯(𝑑 + πœƒ) for πœƒ ∈ [−π‘Ÿ, 0].
2
Abstract and Applied Analysis
In this paper, motivated by above works, we study (1)–(4)
in 𝑋 and obtain the existence theorem based on theory on
measures of noncompactness without the assumptions that
the nonlinearity 𝑓 satisfies a Lipschitz type condition and the
cosine family of bounded linear operators {𝐢(𝑑)}𝑑∈R generated
by 𝐴 is compact.
The following properties are well known [6, 7, 11, 12]:
(i) 𝐢 (𝑑) π‘₯ ∈ 𝐷 (𝐴) , 𝐢 (𝑑) 𝐴π‘₯ = 𝐴𝐢 (𝑑) π‘₯
for π‘₯ ∈ 𝐷 (𝐴) , 𝑑 ∈ R;
(ii) 𝑆 (𝑑) π‘₯ ∈ 𝐷 (𝐴) , 𝑆 (𝑑) 𝐴π‘₯ = 𝐴𝑆 (𝑑) π‘₯
for π‘₯ ∈ 𝐷 (𝐴) , 𝑑 ∈ R;
2. Preliminaries
𝑑
Throughout this paper, we set 𝐽 = [0, 𝑇], a compact interval
in R. We denote by 𝑋 a Banach space with norm β€– ⋅ β€–, by 𝐿(𝑋)
the Banach space of all linear and bounded operators on 𝑋.
We abbreviate ‖𝑒‖𝐿1 (𝐽,R+ ) with ‖𝑒‖𝐿1 , for any 𝑒 ∈ 𝐿1 (𝐽, R+ ).
Let
(iii) ∫ 𝑆 (𝑠) π‘₯𝑑𝑠 ∈ 𝐷 (𝐴) ,
𝑃𝐢 (𝐽, 𝑋) := {π‘₯ : 𝐽 󳨀→ 𝑋; π‘₯ (𝑑) is continuous at 𝑑 =ΜΈ π‘‘π‘˜ ,
(iv) 𝐢 (𝑑) π‘₯ − π‘₯ = ∫ 𝑆 (𝑠) 𝐴π‘₯𝑑𝑠
the right limit π‘₯ (π‘‘π‘˜+ ) exists for π‘˜ = 1, 2, . . . , 𝑝} .
(5)
It is easy to check that 𝑃𝐢(𝐽, 𝑋) is a Banach space with the
norm
𝑑∈𝐽
for any π‘₯ ∈ 𝑃𝐢 (𝐽, 𝑋) .
(6)
for π‘₯ ∈ 𝑋, 𝑑 ∈ R;
0
𝑑
for π‘₯ ∈ 𝐷 (𝐴) , 𝑑 ∈ R.
(11)
For more details on strongly continuous cosine and sine
families, we refer the reader to [6, 7, 11, 12].
Next, we recall that the Hausdorff measure of noncompactness πœ’(⋅) on each bounded subset Ω of Banach space π‘Œ is
defined by
πœ’ (Ω) = inf {πœ€ > 0; Ω has a finite πœ€-net in 𝑋} .
(12)
This measure of noncompactness satisfies some basic
properties as follows.
We let 𝐽0 = (𝑑0 , 𝑑1 ], 𝐽1 = (𝑑1 , 𝑑2 ], . . . , 𝐽𝑝 = (𝑑𝑝 , 𝑑𝑝+1 ].
For B ⊆ 𝑃𝐢(𝐽, 𝑋), we denote by B|𝐽𝑖 the set
B|𝐽𝑖 = {π‘₯ ∈ 𝐢 ([𝑑𝑖 , 𝑑𝑖+1 ] , 𝑋) ; π‘₯ (𝑑𝑖 ) = 𝑣 (𝑑𝑖+ ) , π‘₯ (𝑑) = 𝑣 (𝑑) ,
𝑑 ∈ 𝐽𝑖 , 𝑣 ∈ B}
Lemma 1 (see [31]). Let π‘Œ be a real Banach space, and let
𝐡, 𝐢 ⊆ π‘Œ be bounded. Then
(1) πœ’(𝐡) = 0 if and only if 𝐡 is precompact;
(7)
𝑖 = 0, 1, 2, . . . , 𝑝.
A family {𝐢(𝑑)}𝑑∈R in 𝐿(𝑋) is called a cosine function on
𝑋 if
(i) 𝐢(0) = 𝐼 is the identity operator in 𝑋;
(iii) The map 𝑑 → 𝐢(𝑑)π‘₯ is strongly continuous for each
π‘₯ ∈ 𝑋.
The associated sine function is the family {𝑆(𝑑)}𝑑∈R of operators defined by
𝑑
𝑆 (𝑑) π‘₯ = ∫ 𝐢 (𝑠) π‘₯ 𝑑𝑠,
for π‘₯ ∈ 𝑋, 𝑑 ∈ R.
0
(8)
One can define the infinitesimal generator 𝐴 of 𝐢(⋅) by
−2
𝐷 (𝐴) = {π‘₯ ∈ 𝑋; lim 2𝑑 (𝐢 (𝑑) π‘₯ − π‘₯) ∈ 𝑋}
𝑑→0
𝐴π‘₯ = lim 2𝑑−2 (𝐢 (𝑑) π‘₯ − π‘₯) ,
𝑑→0
(9)
π‘₯ ∈ 𝐷 (𝐴) .
In this paper, we assume there exist positive constants 𝑀
and 𝑁 such that
‖𝑆 (𝑑)β€– ≤ 𝑁
for every 𝑑 ∈ 𝐽.
(2) πœ’(𝐡) = πœ’(𝐡) = πœ’(π‘π‘œπ‘›π‘£π΅), where 𝐡 and π‘π‘œπ‘›π‘£π΅ mean
the closure and convex hull of 𝐡, respectively;
(3) πœ’(𝐡) ≤ πœ’(𝐢) if 𝐡 ⊆ 𝐢;
(4) πœ’(𝐡 ∪ 𝐢) ≤ max{πœ’(𝐡), πœ’(𝐢)};
(5) πœ’(𝐡 + 𝐢) ≤ πœ’(𝐡) + πœ’(𝐢), where 𝐡 + 𝐢 = {π‘₯ + 𝑦; π‘₯ ∈
𝐡, 𝑦 ∈ 𝐢};
(ii) 𝐢(𝑑 + 𝑠) + 𝐢(𝑑 − 𝑠) = 2𝐢(𝑑)𝐢(𝑠) for all 𝑠, 𝑑 ∈ R;
‖𝐢 (𝑑)β€– ≤ 𝑀,
𝑑
𝐴 ∫ 𝑆 (𝑠) π‘₯𝑑𝑠 = 𝐢 (𝑑) π‘₯ − π‘₯
0
left continuous at 𝑑 = π‘‘π‘˜ , and
β€–π‘₯‖𝑃𝐢 = sup β€–π‘₯ (𝑑)β€– ,
0
(10)
(6) πœ’(𝛼𝐡) = |𝛼|πœ’(𝐡), for any 𝛼 ∈ R;
(7) let 𝑍 be a Banach space and 𝑄 : 𝐷(𝑄) ⊆ π‘Œ → 𝑍 Lipschitz continuous with constant 𝜈. Then πœ’(𝑄𝐡) ≤ 𝜈 ⋅
πœ’(𝐡) for all 𝐡 ⊆ 𝐷(𝑄) being bounded.
Proposition 2 (see [32], Page 125). Let Ω be a bounded set
for a real Banach space 𝑋. Then, for every πœ€ > 0 there exists a
sequence {π‘₯𝑛 }∞
𝑛=1 in Ω such that
∞
πœ’ (Ω) ≤ 2πœ’ ({π‘₯𝑛 }𝑛=1 ) + πœ€.
(13)
In the sequel, we make use of the following formulation
of Theorem 4.2.2 of [33] obtained by using Theorem 2 of [34].
1
Proposition 3. Let {𝑓𝑛 }∞
𝑛=1 be a sequence in 𝐿 (𝐽, 𝑋) such that
1
there exist 𝑣, π‘ž ∈ 𝐿 + ([0, 𝑇]) with the properties:
(i) sup𝑛∈N ‖𝑓𝑛 (𝑑)β€– ≤ 𝑣(𝑑), π‘Ž.𝑒. 𝑑 ∈ 𝐽;
(ii) πœ’({𝑓𝑛 }∞
𝑛=1 ) ≤ π‘ž(𝑑), π‘Ž.𝑒. 𝑑 ∈ 𝐽.
Abstract and Applied Analysis
3
Then, for every 𝑑 ∈ 𝐽, we have
𝑑
∞
0
𝑛=1
πœ’ ({∫ 𝑆 (𝑑 − 𝑠) 𝑓𝑛 (𝑠) 𝑑𝑠}
(H2) πΌπ‘˜ : 𝑋 → 𝑋 are compact operators and there
exist positive constants 𝑀1 , 𝑀2 such that
𝑑
) ≤ 2𝑁 ∫ π‘ž (𝑠) 𝑑𝑠,
0
(14)
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©πΌπ‘˜ (π‘₯)σ΅„©σ΅„©σ΅„© ≤ 𝑀1 β€–π‘₯β€– + 𝑀2 ,
where 𝑁 is from (10).
A continuous map 𝑄 : π‘Š ⊆ π‘Œ → π‘Œ is said to be a πœ’contraction if there exists a positive constant 𝜈 < 1 such that
πœ’(𝑄𝐢) ≤ 𝜈 ⋅ πœ’(𝐢) for any bounded closed subset 𝐢 ⊆ π‘Š.
Theorem 4 (see [31] (Darbo-Sadovskii)). If π‘ˆ ⊆ π‘Œ is bounded
closed and convex, the continuous map F : π‘ˆ → π‘ˆ is a πœ’contraction, then the map F has at least one fixed point in π‘ˆ.
Definition 5. A function π‘₯ : [−π‘Ÿ, 𝑇] → 𝑋 is called a mild
solution of system (1)–(4) if π‘₯0 = 𝑔(π‘₯) + πœ™, π‘₯|𝐽 ∈ 𝑃𝐢(𝐽, 𝑋)
and
(H3) 𝑔 : 𝐢([−π‘Ÿ, 0], 𝑋) → 𝑋 is a compact operator
and there exists a constant 𝑁1 > 0 such that
σ΅„©
σ΅„©σ΅„©
󡄩󡄩𝑔 (π‘₯)σ΅„©σ΅„©σ΅„©[−π‘Ÿ,0] ≤ 𝑁1
for all π‘₯ ∈ 𝐢 ([−π‘Ÿ, 0] , 𝑋) ,
(21)
where ‖𝑔(π‘₯)β€–[−π‘Ÿ,0] = sup𝑑∈[−π‘Ÿ,0] ‖𝑔(π‘₯)(𝑑)β€–.
𝑇
(H4) There exists 𝑀∗ ∈ (0, 1) such that 8𝑁 ∫0 πœ‚(𝑠)𝑑𝑠 <
𝑀∗ .
Theorem 7. Assume that (H1)–(H4) are satisfied, then there
exists a mild solution of (1)–(4) on [−π‘Ÿ, 𝑇] provided that
𝑝𝑀𝑀1 < 1.
π‘₯ (𝑑) = 𝐢 (𝑑) (πœ™ (0) + 𝑔 (π‘₯) (0)) + 𝑆 (𝑑) πœ‰
𝑑
+ ∫ 𝑆 (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠)) 𝑑𝑠
(15)
0
+ ∑ 𝐢 (𝑑 − π‘‘π‘˜ ) πΌπ‘˜ (π‘₯ (π‘‘π‘˜ )) ,
for any π‘₯ ∈ 𝑋, π‘˜ = 1, 2, . . . , 𝑝.
(20)
𝑑 ∈ 𝐽.
Proof. Define the operator Λ : F(𝑇) → F(𝑇) in the following way:
0<π‘‘π‘˜ <𝑑
Remark 6. A mild solution of (1)–(4) satisfies (2) and (4).
However, a mild solution may be not differentiable at zero.
3. Existence Result and Proof
In this section, we study the existence of mild solutions for
the system (1)–(4).
Let F(𝑇) stand for the space
F (𝑇) = {π‘₯ : [−π‘Ÿ, 𝑇] → 𝑋; π‘₯|𝐽 ∈ 𝑃𝐢 (𝐽, 𝑋) ,
π‘₯0 ∈ 𝐢 ([−π‘Ÿ, 0] , 𝑋)}
(16)
endowed with norm
β€–π‘₯β€–F(𝑇) = sup β€–π‘₯ (𝑑)β€– + sup β€–π‘₯ (𝑑)β€– .
𝑑∈[−π‘Ÿ,0]
𝑑∈𝐽
(17)
We will require the following assumptions.
(H1) (i) 𝑓 : 𝐽×𝐢([−π‘Ÿ, 0], 𝑋)×𝑋 → 𝑋 satisfies 𝑓(⋅, 𝑣, 𝑀) :
𝐽 → 𝑋 is measurable for all (𝑣, 𝑀) ∈ 𝐢([−π‘Ÿ, 0], 𝑋) × π‘‹ and
𝑓(𝑑, ⋅, ⋅) : 𝐢([−π‘Ÿ, 0], 𝑋) × π‘‹ → 𝑋 is continuous for a.e. 𝑑 ∈ 𝐽,
and there exists a function πœ‡(⋅) ∈ 𝐿1 (𝐽, R+ ) such that
󡄩󡄩󡄩𝑓 (𝑑, 𝑣, 𝑀)σ΅„©σ΅„©σ΅„© ≤ πœ‡ (𝑑) (1 + ‖𝑀‖)
(18)
σ΅„©
σ΅„©
for almost all 𝑑 ∈ 𝐽;
(ii) there exists a function πœ‚ ∈ 𝐿1 (𝐽, R+ ) such that for any
bounded sets 𝐷1 ⊂ 𝐢([−π‘Ÿ, 0], 𝑋), 𝐷2 ⊂ 𝑋
πœ’ (𝑓 (𝑑, 𝐷1 , 𝐷2 )) ≤ πœ‚ (𝑑) ( sup πœ’ (𝐷1 (πœƒ)) + πœ’ (𝐷2 )) ,
πœƒ∈[−π‘Ÿ,0]
a.e. 𝑑 ∈ 𝐽.
(19)
𝑔 (π‘₯) (𝑑) + πœ™ (𝑑) ,
𝑑 ∈ [−π‘Ÿ, 0] ,
{
{
{
{
{
𝐢 (𝑑) (𝑔 (π‘₯) (0) + πœ™ (0)) + 𝑆 (𝑑) πœ‰
{
{
{
{ 𝑑
(Λπ‘₯) (𝑑) = {+ ∫ 𝑆 (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯ , π‘₯ (𝑠)) 𝑑𝑠
{
𝑠
{
{
0
{
{
{
{
𝑑 ∈ 𝐽.
{+ ∑ 𝐢 (𝑑 − π‘‘π‘˜ ) πΌπ‘˜ (π‘₯ (π‘‘π‘˜ )) ,
{ 0<π‘‘π‘˜ <𝑑
(22)
It is clear that the operator Λ is well defined, and the fixed
point of Λ is the mild solution of problems (1)–(4).
The operator Λ can be written in the form Λ = Λ 1 + Λ 2 ,
where the operators Λ 1 , Λ 2 are defined as follows:
𝑔 (π‘₯) (𝑑) + πœ™ (𝑑) ,
𝑑 ∈ [−π‘Ÿ, 0] ,
{
{
{
(Λ 1 π‘₯) (𝑑) = {𝐢 (𝑑) (𝑔 (π‘₯) (0) + πœ™ (0))
{
{
𝑑 ∈ 𝐽,
{+𝑆 (𝑑) πœ‰,
0,
𝑑 ∈ [−π‘Ÿ, 0] ,
{
{
{
𝑑
{
{
{
(Λ 2 π‘₯) (𝑑) = {∫0 𝑆 (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠)) 𝑑𝑠
{
{
{
{
{+ ∑ 𝐢 (𝑑 − π‘‘π‘˜ ) πΌπ‘˜ (π‘₯ (π‘‘π‘˜ )) , 𝑑 ∈ 𝐽.
{ 0<π‘‘π‘˜ <𝑑
(23)
Obviously, under the assumptions of 𝑔, Λ 1 is continuous.
For 𝑑 ∈ 𝐽, we can prove that Λ 2 is continuous.
Indeed, let {π‘₯𝑛 }𝑛∈N be a sequence such that π‘₯𝑛 → π‘₯ in
F(𝑇) as 𝑛 → ∞. Since 𝑓 satisfies (H1)(i), for almost every
𝑑 ∈ 𝐽, we get
𝑓 (𝑑, π‘₯𝑑𝑛 , π‘₯𝑛 (𝑑)) 󳨀→ 𝑓 (𝑑, π‘₯𝑑 , π‘₯ (𝑑)) ,
as 𝑛 󳨀→ ∞.
(24)
4
Abstract and Applied Analysis
Noting that π‘₯𝑛 → π‘₯ in F(𝑇), we can see that there exists
πœ€ > 0 such that β€–π‘₯𝑛 − π‘₯β€–F(𝑇) ≤ πœ€ for 𝑛 sufficiently large.
Therefore, we have
σ΅„©σ΅„©
σ΅„©
𝑛 𝑛
󡄩󡄩𝑓 (𝑑, π‘₯𝑑 , π‘₯ (𝑑)) − 𝑓 (𝑑, π‘₯𝑑 , π‘₯ (𝑑))σ΅„©σ΅„©σ΅„©
σ΅„©
σ΅„©
≤ πœ‡ (𝑑) (1 + σ΅„©σ΅„©σ΅„©π‘₯𝑛 (𝑑)σ΅„©σ΅„©σ΅„©) + πœ‡ (𝑑) (1 + β€–π‘₯ (𝑑)β€–)
σ΅„©
σ΅„©
≤ 2πœ‡ (𝑑) + πœ‡ (𝑑) σ΅„©σ΅„©σ΅„©π‘₯𝑛 (𝑑) − π‘₯ (𝑑)σ΅„©σ΅„©σ΅„© + 2πœ‡ (𝑑) β€–π‘₯ (𝑑)β€–
For 𝑑 ∈ 𝐽, π‘₯ ∈ 𝐡𝜌 , we have
σ΅„©
σ΅„© σ΅„©
σ΅„©
β€–(Λπ‘₯) (𝑑)β€– ≤ 󡄩󡄩󡄩𝐢 (𝑑) (𝑔 (π‘₯) (0) + πœ™ (0))σ΅„©σ΅„©σ΅„© + 󡄩󡄩󡄩𝑆 (𝑑) πœ‰σ΅„©σ΅„©σ΅„©
𝑑
σ΅„©
σ΅„©
+ ∫ 󡄩󡄩󡄩𝑆 (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠))σ΅„©σ΅„©σ΅„© 𝑑𝑠
0
σ΅„©
σ΅„©
+ ∑ 󡄩󡄩󡄩𝐢 (𝑑 − π‘‘π‘˜ ) πΌπ‘˜ (π‘₯ (π‘‘π‘˜ ))σ΅„©σ΅„©σ΅„©
(25)
0<π‘‘π‘˜ <𝑑
σ΅„©
σ΅„©
σ΅„©
σ΅„©
≤ 𝑀 (𝑁1 + σ΅„©σ΅„©σ΅„©πœ™ (0)σ΅„©σ΅„©σ΅„© + ∑ σ΅„©σ΅„©σ΅„©πΌπ‘˜ (π‘₯ (π‘‘π‘˜ ))σ΅„©σ΅„©σ΅„©)
≤ 2πœ‡ (𝑑) + πœ‡ (𝑑) πœ€ + 2πœ‡ (𝑑) β€–π‘₯β€–F(𝑇) .
0<π‘‘π‘˜ <𝑑
It follows from the Lebesgue’s dominated convergence theorem that
𝑑
σ΅„© σ΅„©
+𝑁 (σ΅„©σ΅„©σ΅„©πœ‰σ΅„©σ΅„©σ΅„© +∫ πœ‡ (𝑠) (1+𝑒𝐿𝑠 𝑒−𝐿𝑠 β€–π‘₯ (𝑠)β€–) 𝑑𝑠)
0
σ΅„©
σ΅„©
= β„“ + 𝑀 ∑ σ΅„©σ΅„©σ΅„©πΌπ‘˜ (π‘₯ (π‘‘π‘˜ ))σ΅„©σ΅„©σ΅„©
𝑑
σ΅„©
σ΅„©
∫ 󡄩󡄩󡄩𝑆 (𝑑 − 𝑠) [𝑓 (𝑠, π‘₯𝑠𝑛 , π‘₯𝑛 (𝑠)) − 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠))]σ΅„©σ΅„©σ΅„© 𝑑𝑠
0
𝑑
σ΅„©
σ΅„©
≤ 𝑁 ∫ 󡄩󡄩󡄩𝑓 (𝑠, π‘₯𝑠𝑛 , π‘₯𝑛 (𝑠)) − 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠))σ΅„©σ΅„©σ΅„© 𝑑𝑠
0
󳨀→ 0,
0<π‘‘π‘˜ <𝑑
𝑑
+ 𝑁 ∫ πœ‡ (𝑠) 𝑒𝐿𝑠 𝑒−𝐿𝑠 β€–π‘₯ (𝑠)β€– 𝑑𝑠,
(26)
0
as 𝑛 󳨀→ ∞.
(34)
then
Moreover, noting that (H2), we obtain that
σ΅„©
σ΅„©
lim σ΅„©σ΅„©Λ 2 π‘₯𝑛 − Λ 2 π‘₯σ΅„©σ΅„©σ΅„©F(𝑇) = 0.
𝑛 → ∞σ΅„©
(27)
This shows that Λ 2 is continuous. Therefore, Λ is continuous.
Let us introduce in the space F(𝑇) the equivalent norm
defined as
−𝐿𝑑
β€–π‘₯β€–∗ = sup β€–π‘₯ (𝑑)β€– + sup (𝑒
𝑑∈𝐽
𝑑∈[−π‘Ÿ,0]
β€–π‘₯ (𝑑)β€–) ,
σ΅„©
σ΅„©
𝑒−𝐿𝑑 β€–(Λπ‘₯) (𝑑)β€– ≤ 𝑒−𝐿𝑑 [β„“ + 𝑀 ∑ σ΅„©σ΅„©σ΅„©πΌπ‘˜ (π‘₯ (π‘‘π‘˜ ))σ΅„©σ΅„©σ΅„©
0<π‘‘π‘˜ <𝑑
𝑑
+𝑁 ∫ πœ‡ (𝑠) 𝑒𝐿𝑠 𝑒−𝐿𝑠 β€–π‘₯ (𝑠)β€– 𝑑𝑠]
0
(28)
≤ β„“ + πœŒπ‘π‘€π‘€1 + 𝑝𝑀𝑀2
𝑑
where 𝐿 > 0 is a constant chosen so that
+ 𝑁 ∫ πœ‡ (𝑠) 𝑒−𝐿(𝑑−𝑠) 𝑑𝑠 ⋅ β€–π‘₯β€–∗ ,
0
𝑑
𝑁sup ∫ πœ‡ (𝑠) 𝑒−𝐿(𝑑−𝑠) 𝑑𝑠 < 1.
𝑑∈𝐽
0
therefore,
1
Noting that for any πœ“ ∈ 𝐿 (𝐽, 𝑋), we have
𝑑
0
sup (𝑒−𝐿𝑑 β€–(Λπ‘₯) (𝑑)β€–)
𝑑∈𝐽
−𝐿(𝑑−𝑠)
lim sup ∫ 𝑒
𝐿 → +∞ 𝑑∈𝐽
πœ“ (𝑠) 𝑑𝑠 = 0,
(30)
𝐡𝜌 = {π‘₯ ∈ F (𝑇) ; β€–π‘₯β€–∗ ≤ 𝜌} ,
1 − 𝑝𝑀𝑀1
(36)
+ [𝑝𝑀𝑀1 + sup (𝑁 ∫ πœ‡ (𝑠) 𝑒−𝐿(𝑑−𝑠) 𝑑𝑠)] 𝜌.
𝑑∈𝐽
(31)
where 𝜌 is a constant chosen so that
σ΅„© σ΅„©
𝑁1 + σ΅„©σ΅„©σ΅„©πœ™σ΅„©σ΅„©σ΅„©[−π‘Ÿ,0] + β„“ + 𝑝𝑀𝑀2
≤ β„“ + 𝑝𝑀𝑀2
𝑑
so, we can take the appropriate 𝐿 to satisfy (29).
Consider the set
𝜌≥
(35)
(29)
0
It results that
β€–Λπ‘₯β€–∗ = sup β€–(Λπ‘₯) (𝑑)β€– + sup (𝑒−𝐿𝑑 β€–(Λπ‘₯) (𝑑)β€–)
𝑑∈𝐽
𝑑∈[−π‘Ÿ,0]
> 0,
σ΅„© σ΅„©
≤ 𝑁1 + σ΅„©σ΅„©σ΅„©πœ™σ΅„©σ΅„©σ΅„©[−π‘Ÿ,0] + β„“ + 𝑝𝑀𝑀2
(32)
𝑑
+ (𝑝𝑀𝑀1 + 𝑁sup ∫ πœ‡ (𝑠) 𝑒−𝐿(𝑑−𝑠) 𝑑𝑠) 𝜌.
where β„“ := 𝑀(𝑁1 + β€–πœ™(0)β€–) + 𝑁(β€–πœ‰β€– + β€–πœ‡β€–πΏ1 ) and β€–πœ™β€–[−π‘Ÿ,0] =
sup𝑑∈[−π‘Ÿ,0] β€–πœ™(𝑑)β€–.
Now, if 𝑑 ∈ [−π‘Ÿ, 0], π‘₯ ∈ 𝐡𝜌 , then
σ΅„©
σ΅„©
σ΅„© σ΅„©
β€–(Λπ‘₯) (𝑑)β€– = 󡄩󡄩󡄩𝑔 (π‘₯) (𝑑) + πœ™ (𝑑)σ΅„©σ΅„©σ΅„© ≤ 𝑁1 + σ΅„©σ΅„©σ΅„©πœ™σ΅„©σ΅„©σ΅„©[−π‘Ÿ,0] .
(37)
(33)
𝑑∈𝐽
0
Let 𝐿 → +∞, we obtain
σ΅„© σ΅„©
β€–Λπ‘₯β€–∗ ≤ 𝑁1 + σ΅„©σ΅„©σ΅„©πœ™σ΅„©σ΅„©σ΅„©[−π‘Ÿ,0] + β„“ + 𝑝𝑀𝑀2 + 𝑝𝑀𝑀1 𝜌 ≤ 𝜌. (38)
Hence for some positive number 𝜌, Λ𝐡𝜌 ⊂ 𝐡𝜌 .
Abstract and Applied Analysis
5
Using the strong continuity of {𝐢(𝑑)}𝑑∈R and the compactness condition on the operators πΌπ‘˜ , for πœ€ > 0, there exists 𝛿 > 0
such that
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©(𝐢 (𝑑 + β„Ž) − 𝐢 (𝑑)) πΌπ‘˜ (π‘₯)σ΅„©σ΅„©σ΅„© ≤ πœ€,
π‘₯ ∈ 𝐡𝜌 ,
(39)
𝑑 ∈ 𝐽, π‘˜ = 1, 2, . . . , 𝑝,
when |β„Ž| < 𝛿. If 𝑑 ∈ [π‘‘π‘˜ , π‘‘π‘˜+1 ] and β„Ž < 𝛿 such that 𝑑 + β„Ž ∈
[π‘‘π‘˜ , π‘‘π‘˜+1 ], then
Μƒ ⊂ 𝑃𝐢(𝐽, 𝑋), by applying
For every bounded subset Ω
Proposition 2, for any πœ€ > 0 there exists a sequence {π‘₯𝑛 }∞
𝑛=1 ⊂
Μƒ such that
Ω
Μƒ ≤ 2πœ’π‘π‘ (Λ 2 {π‘₯𝑛 }) + πœ€,
πœ’π‘π‘ (Λ 2 Ω)
noting that the definition of πœ’π‘π‘ , we have
Μƒ ≤ 2 max πœ’π‘– (Λ 2 {π‘₯𝑛 } | ) + πœ€.
πœ’π‘π‘ (Λ 2 Ω)
𝐽𝑖
𝑖=0,1,...,𝑝
σ΅„©σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©
σ΅„©
σ΅„©σ΅„© ∑ (𝐢 (𝑑 + β„Ž − 𝑑 ) − 𝐢 (𝑑 − 𝑑 )) 𝐼 (π‘₯ (𝑑 ))σ΅„©σ΅„©σ΅„©
σ΅„©σ΅„©
π‘˜
π‘˜
π‘˜
π‘˜ σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©0<π‘‘π‘˜ <𝑑
σ΅„©σ΅„©
σ΅„©
(44)
(45)
Then, noting the equicontinuity of Λ 2 |𝐽𝑖 , 𝑖 = 0, 1, . . . , 𝑝, we
can apply Lemmas 2.1 and 2.2 of [35] to obtain
𝑝
σ΅„©
σ΅„©
≤ ∑ σ΅„©σ΅„©σ΅„©(𝐢 (𝑑 + β„Ž − π‘‘π‘˜ ) − 𝐢 (𝑑 − π‘‘π‘˜ )) πΌπ‘˜ (π‘₯ (π‘‘π‘˜ ))σ΅„©σ΅„©σ΅„© ≤ π‘πœ€.
π‘˜=1
πœ’π‘– (Λ 2 {π‘₯𝑛 } |𝐽𝑖 ) = supπœ’ (Λ 2 {π‘₯𝑛 } (𝑑)) .
𝑑∈𝐽𝑖
(40)
For π‘₯ ∈ 𝐡𝜌 , by the hypothesis (H1)(i) and (40), we get
σ΅„©σ΅„©
σ΅„©
σ΅„©σ΅„©(Λ 2 π‘₯) (𝑑 + β„Ž) − (Λ 2 π‘₯) (𝑑)σ΅„©σ΅„©σ΅„©
σ΅„©σ΅„© 𝑑+β„Ž
σ΅„©
≤ σ΅„©σ΅„©σ΅„©σ΅„©∫ 𝑆 (𝑑 + β„Ž − 𝑠) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠)) 𝑑𝑠
σ΅„©σ΅„© 0
(46)
Then from (45) and (46), we have
Μƒ ≤ 2 max (supπœ’ (Λ 2 {π‘₯𝑛 } (𝑑)))
πœ’π‘π‘ (Λ 2 Ω)
𝑖=0,1,...,𝑝
𝑑∈𝐽𝑖
(47)
+ πœ€ = 2supπœ’ (Λ 2 {π‘₯𝑛 } (𝑑)) + πœ€.
𝑑∈𝐽
σ΅„©σ΅„©
σ΅„©
− ∫ 𝑆 (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠)) 𝑑𝑠󡄩󡄩󡄩 + π‘πœ€
σ΅„©σ΅„©
0
𝑑
For every bounded subset Ω ⊂ F(𝑇), we have
𝑑
σ΅„©
σ΅„©
≤ π‘πœ€ + ∫ σ΅„©σ΅„©σ΅„©(𝑆 (𝑑 + β„Ž − 𝑠) − 𝑆 (𝑑 − 𝑠)) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠))σ΅„©σ΅„©σ΅„© 𝑑𝑠
0
+∫
𝑑+β„Ž
𝑑
+ sup πœ’ ((Λ 2 Ω) (𝑑)) = πœ’π‘π‘ ((Λ 2 Ω) |𝑃𝐢(𝐽,𝑋) ) ,
σ΅„©σ΅„©
σ΅„©
󡄩󡄩𝑆 (𝑑 + β„Ž − 𝑠) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠))σ΅„©σ΅„©σ΅„© 𝑑𝑠
𝑑
𝑑+β„Ž
0
𝑑
≤ π‘πœ€ + [π‘€β„Ž ∫ πœ‡ (𝑠) 𝑑𝑠 + 𝑁 ∫
𝑑∈[−π‘Ÿ,0]
(48)
πœ‡ (𝑠) 𝑑𝑠] ⋅ (1 + 𝜌) .
(41)
As β„Ž → 0 and πœ€ → 0, the right-hand side of the inequality
above tends to zero independent of π‘₯, so Λ 2 maps bounded
sets into equicontinuous sets.
For bounded set 𝐡 ⊂ 𝑃𝐢(𝐽, 𝑋), we consider the map
πœ’π‘π‘ (𝐡) = max πœ’π‘– (𝐡|𝐽𝑖 ) ,
𝑖=0,1,...,𝑝
(42)
where πœ’π‘– is the Hausdorff measure of noncompactness on the
Banach space 𝐢(𝐽𝑖 , 𝑋) and 𝐡|𝐽𝑖 is defined in (7).
Furthermore, we define the Hausdorff measure of noncompactness πœ’F on F(𝑇) as follows:
πœ’F (Y ) := πœ’π‘π‘ (Y |𝑃𝐢(𝐽,𝑋) ) + sup πœ’ (Y (𝑑)) ,
𝑑∈[−π‘Ÿ,0]
πœ’F (Λ 2 Ω) = πœ’π‘π‘ ((Λ 2 Ω) |𝑃𝐢(𝐽,𝑋) )
Y ⊂ F (𝑇) .
(43)
moreover, by applying Proposition 2, for any πœ€ > 0 there exists
a sequence {𝑦𝑛 }∞
𝑛=1 ⊂ Ω such that
πœ’F (Λ 2 Ω) ≤ 2πœ’F (Λ 2 {𝑦𝑛 }) + πœ€
= 2πœ’π‘π‘ ((Λ 2 {𝑦𝑛 }) |𝑃𝐢(𝐽,𝑋) ) + πœ€.
(49)
Combining with (48) and (49), we have
πœ’F (Λ 2 Ω) = πœ’π‘π‘ ((Λ 2 Ω) |𝑃𝐢(𝐽,𝑋) )
≤ 2πœ’π‘π‘ ((Λ 2 {𝑦𝑛 }) |𝑃𝐢(𝐽,𝑋) ) + πœ€.
(50)
Using the induction of (45)–(47) above, we can see
πœ’F (Λ 2 Ω) = πœ’π‘π‘ ((Λ 2 Ω) |𝑃𝐢(𝐽,𝑋) )
≤ 2supπœ’ (Λ 2 {𝑦𝑛 } (𝑑) |𝑑∈𝐽 ) + πœ€.
𝑑∈𝐽
(51)
6
Abstract and Applied Analysis
Thus, from (51), (H2) and Proposition 3 and (3) in Lemma 1,
we can see
πœ’F (Λ 2 Ω) ≤ 2supπœ’ (Λ 2 {𝑦𝑛 } (𝑑) |𝑑∈𝐽 ) + πœ€
Combining with (H3), we have
πœ’F (ΛΩ) ≤ πœ’F (Λ 1 Ω) + πœ’F (Λ 2 Ω)
𝑑∈𝐽
𝑇
≤ 8𝑁 ∫ πœ‚ (𝑠) 𝑑𝑠 ⋅ πœ’F (Ω) < 𝑀∗ πœ’F (Ω) ,
𝑑
0
= 2sup [πœ’ ({ ∫ 𝑆 (𝑑−𝑠)𝑓 (𝑠, 𝑦̃𝑛𝑠 , 𝑦̃𝑛 (𝑠)) 𝑑𝑠
0
𝑑∈𝐽
+ ∑ 𝐢 (𝑑−π‘‘π‘˜ ) πΌπ‘˜ (𝑦̃𝑛 (π‘‘π‘˜ ))})]+πœ€
0<π‘‘π‘˜ <𝑑
𝑑
≤ 2sup [2𝑁 ∫ πœ‚ (𝑠) ( sup πœ’ ({𝑦𝑛 (𝑠 + πœƒ)})
0
𝑑∈𝐽
πœƒ∈[−π‘Ÿ,0]
+πœ’ ({𝑦̃𝑛 (𝑠)}) ) 𝑑𝑠] + πœ€,
(52)
where 𝑦̃𝑛 (𝑑) := 𝑦𝑛 (𝑑)|𝑑∈𝐽 .
Noting that
hence Λ is a πœ’F -contraction on F(𝑇). According to Theorem 4, the operator Λ has at least one fixed point π‘₯ in 𝐡𝜌 .
This completes the proof.
Next, we establish a condition that guarantee that a mild
solution satisfies (3).
Proposition 8. Assume that the hypotheses of Theorem 7 are
fulfilled and that πœ™(0) + 𝑔(π‘₯)(0) ∈ 𝐷(𝐴). If π‘₯(⋅) is a mild
solution of (1)–(4), then condition (3) holds.
𝑑
Proof. Clearly, (1/𝑑) ∫0 𝑆(𝑑 − 𝑠)𝑓(𝑠, π‘₯𝑠 , π‘₯(𝑠))𝑑𝑠 → 0 as 𝑑 → 0.
Moreover, noting that πœ™(0)+𝑔(π‘₯)(0) ∈ 𝐷(𝐴) and (11), we have
𝐢(⋅)(πœ™(0) + 𝑔(π‘₯)(0)) is of class 𝐢1 . Therefore, we can see that
lim
sup πœ’ ({𝑦𝑛 (𝑠 + πœƒ)}) ≤ sup πœ’ ({𝑦𝑛 (πœƒ)})
πœƒ∈[−π‘Ÿ,0]
𝑑 → 0+
πœƒ∈[−π‘Ÿ,0]
π‘₯ (𝑑) − π‘₯ (0)
𝑑
1
= lim+ [ (𝐢 (𝑑) − 𝐼) (πœ™ (0) + 𝑔 (π‘₯) (0)) + 𝑆 (𝑑) πœ‰
𝑑→0 𝑑
+ supπœ’ ({𝑦̃𝑛 (𝑠)})
𝑠∈𝐽
≤ sup πœ’ (Ω (πœƒ))
4. Application
πœƒ∈[−π‘Ÿ,0]
In this section, we consider an application of the theory
developed in Section 3 to the study of an impulsive partial
differential equation with unbounded delay.
+ πœ’π‘π‘ (Ω) = πœ’F (Ω) ,
≤ πœ’π‘π‘ (Ω) .
(54)
Thus, by (52), we see
𝑑
πœ’F (Λ 2 Ω) ≤ 2sup [2𝑁 ∫ πœ‚ (𝑠) ( sup πœ’ ({𝑦𝑛 (𝑠 + πœƒ)})
0
0
which shows the assertion.
𝑠∈𝐽
𝑑∈𝐽
+ ∫ 𝑆 (𝑑 − 𝑠) 𝑓 (𝑠, π‘₯𝑠 , π‘₯ (𝑠)) 𝑑𝑠] = πœ‰,
(53)
+ supπœ’ (Ω (𝑠))
πœ’ ({𝑦̃𝑛 (𝑠)}) ≤ πœ’ (Ω (𝑠))
Example 9. 𝑋 = 𝐿2 ([0, πœ‹]), 𝐴 : 𝐷(𝐴) ⊆ 𝑋 → 𝑋 is the map
defined by π΄πœ— = πœ—σΈ€ σΈ€  with domain 𝐷(𝐴) = {πœ— ∈ 𝑋 : πœ—σΈ€ σΈ€  ∈
𝑋, πœ—(0) = πœ—(πœ‹) = 0}.
We consider the following integrodifferential model:
πœ•2
πœ•2
󡄨
󡄨
𝑣
πœ‰)
=
𝑣 (𝑑, πœ‰) + sin 󡄨󡄨󡄨𝑣 (𝑑, πœ‰)󡄨󡄨󡄨
(𝑑,
πœ•π‘‘2
πœ•πœ‰2
πœƒ∈[−π‘Ÿ,0]
+πœ’ ({𝑦̃𝑛 (𝑠)}) ) 𝑑𝑠] + πœ€
𝑑
󡄨
󡄨󡄨
𝑑
󡄨𝑣 (πœƒ, πœ‰)󡄨󡄨󡄨
+ 𝑑2 ∫ 𝛾 (πœƒ − 𝑑) ⋅ cos ( 󡄨
) π‘‘πœƒ,
𝑑
𝑑−π‘Ÿ
≤ 2sup (4𝑁 ∫ πœ‚ (𝑠) 𝑑𝑠) ⋅ πœ’F (Ω) + πœ€
𝑣 (𝑑, πœ‹) = 𝑣 (𝑑, 0) = 0,
0
𝑑∈𝐽
(58)
𝑑
≤ sup πœ’ (Ω (πœƒ))
πœƒ∈[−π‘Ÿ,0]
(57)
πœ‹
𝑇
𝑣 (πœƒ, πœ‰) = 𝑣0 (πœƒ, πœ‰) + ∫ 𝑐 (πœ‰, 𝑠) sin (1 + 𝑣 (πœƒ, 𝑠)) 𝑑𝑠,
= 8𝑁 ∫ πœ‚ (𝑠) 𝑑𝑠 ⋅ πœ’F (Ω) + πœ€.
0
0
(55)
Since πœ€ is arbitrary, we can obtain
𝑇
πœ’F (Λ 2 Ω) ≤ 8𝑁 ∫ πœ‚ (𝑠) 𝑑𝑠 ⋅ πœ’F (Ω) .
0
− π‘Ÿ ≤ πœƒ ≤ 0,
πœ‹
(56)
πœ•
𝑣 (0, πœ‰) = πœ” (πœ‰) ,
πœ•π‘‘
Δ𝑣 (π‘‘π‘˜ , πœ‰) = ∫ πœŒπ‘˜ (πœ‰, 𝑦) 𝑑𝑦 ⋅ cos2 (𝑣 (π‘‘π‘˜ , πœ‰)) ,
0
1 ≤ π‘˜ ≤ 𝑝,
(59)
Abstract and Applied Analysis
7
where 𝑑 ∈ [0, 𝑇], π‘Ÿ > 0, πœ‰ ∈ [0, πœ‹], 0 < 𝑑1 < 𝑑2 < ⋅ ⋅ ⋅ < 𝑑𝑝 < 𝑇,
πœ” ∈ 𝑋 and 𝑣𝑑 (πœƒ, πœ‰) = 𝑣(𝑑 + πœƒ, πœ‰). 𝛾 : [−π‘Ÿ, 0] → R and 𝑐(πœ‰, 𝑠),
πœŒπ‘˜ (πœ‰, 𝑧) ∈ 𝐿2 ([0, πœ‹] × [0, πœ‹], R) satisfy the following assumptions.
(1) The function 𝛾 : [−π‘Ÿ, 0] → R is a continuous func0
tion and ∫−π‘Ÿ |𝛾(πœƒ)|π‘‘πœƒ < ∞.
(2) The function 𝑐(πœ‰, 𝑠), πœ‰, 𝑠 ∈ [0, πœ‹] is measurable and there exists a constant 𝑁1 such that
πœ‹
πœ‹
(πœ‹ ∫0 ∫0 𝑐2 (πœ‰, 𝑠)π‘‘π‘ π‘‘πœ‰)
1/2
≤ 𝑁1 .
(3) For every π‘˜ = 1, 2, . . . , 𝑝, the function πœŒπ‘˜ (πœ‰, 𝑧), 𝑧 ∈
[0, πœ‹], is measurable and there exists a constant 𝑁
such that
πœ‹
πœ‹
0
0
2
1/2
(∫ (∫ πœŒπ‘˜ (πœ‰, 𝑧)𝑑𝑧) π‘‘πœ‰)
≤ 𝑁.
(60)
𝐴𝑒 = 𝑒󸀠󸀠 .
0
󡄨
󡄨
σ΅„©
σ΅„©σ΅„©
2
󡄩󡄩𝑓 (𝑑, πœ‘, π‘₯ (𝑑))σ΅„©σ΅„©σ΅„© ≤ β€–π‘₯ (𝑑)β€– + 𝑑 ∫ 󡄨󡄨󡄨𝛾 (πœƒ)󡄨󡄨󡄨 π‘‘πœƒ
−π‘Ÿ
(63)
≤ πœ‡ (𝑑) (1 + β€–π‘₯ (𝑑)β€–) ,
0
where πœ‡(𝑑) := max{1, 𝑑2 ∫−π‘Ÿ |𝛾(πœƒ)|π‘‘πœƒ}.
For any π‘₯1 , π‘₯2 ∈ 𝑋, πœ‘, πœ‘Μƒ ∈ 𝐢([−π‘Ÿ, 0], 𝑋),
σ΅„©σ΅„©
Μƒ π‘₯2 (𝑑)) (πœ‰)σ΅„©σ΅„©σ΅„©σ΅„©
󡄩󡄩𝑓 (𝑑, πœ‘, π‘₯1 (𝑑)) (πœ‰) − 𝑓 (𝑑, πœ‘,
0
σ΅„©
󡄨󡄩
σ΅„©
σ΅„©
󡄨
≤ σ΅„©σ΅„©σ΅„©π‘₯1 (𝑑) − π‘₯2 (𝑑)σ΅„©σ΅„©σ΅„© + 𝑑 ∫ 󡄨󡄨󡄨𝛾 (πœƒ)󡄨󡄨󡄨 σ΅„©σ΅„©σ΅„©πœ‘ (πœƒ) (πœ‰) − πœ‘Μƒ (πœƒ) (πœ‰)σ΅„©σ΅„©σ΅„© π‘‘πœƒ.
−π‘Ÿ
(64)
Therefore, for any bounded sets 𝐷1 ⊂ 𝐢([−π‘Ÿ, 0], 𝑋), 𝐷2 ⊂
𝑋, we have
0
󡄨
󡄨
πœ’ (𝑓 (𝑑, 𝐷1 , 𝐷2 )) ≤ πœ’ (𝐷2 ) + 𝑑 ∫ 󡄨󡄨󡄨𝛾 (πœƒ)󡄨󡄨󡄨 πœ’ (𝐷1 (πœƒ)) π‘‘πœƒ
−π‘Ÿ
To treat the above problem, we define
𝐷 (𝐴) = 𝐻2 ([0, πœ‹]) ∩ 𝐻01 ([0, πœ‹]) ,
For 𝑑 ∈ [0, 𝑇], we can see
0
󡄨
󡄨
≤ πœ’ (𝐷2 ) + 𝑑 sup πœ’ (𝐷1 (πœƒ)) ∫ 󡄨󡄨󡄨𝛾 (πœƒ)󡄨󡄨󡄨 π‘‘πœƒ
−π‘Ÿ
−π‘Ÿ≤πœƒ≤0
(61)
≤ πœ‚ (𝑑) ( sup πœ’ (𝐷1 (πœƒ)) + πœ’ (𝐷2 )) ,
𝐴 is the infinitesimal generator of a strongly continuous
cosine function {𝐢(𝑑)}𝑑∈R on 𝑋. Moreover, 𝐴 has a discrete
spectrum, the eigenvalues are −𝑛2 , 𝑛 ∈ N, with the corresponding normalized eigenvectors πœ”π‘› (π‘₯) = √(2/πœ‹) sin(𝑛π‘₯);
the set {πœ”π‘› ; 𝑛 ∈ N} is an orthonormal basis of 𝑋 and the
following properties hold.
2
(a) If πœ” ∈ 𝐷(𝐴), then π΄πœ” = − ∑∞
𝑛=1 𝑛 βŸ¨πœ”, πœ”π‘› βŸ©πœ”π‘› .
−π‘Ÿ≤πœƒ≤0
a.e. 𝑑 ∈ [0, 𝑇] ,
(65)
0
where πœ‚(𝑑) := max{1, 𝑑 ∫−π‘Ÿ |𝛾(πœƒ)|π‘‘πœƒ}.
For π‘₯ ∈ 𝑋,
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©πΌπ‘˜ (π‘₯)σ΅„©σ΅„©σ΅„© ≤ 𝑁 (1 + β€–π‘₯β€–) ,
π‘˜ = 1, 2, . . . , 𝑝.
(66)
(b) For each πœ” ∈ 𝑋, 𝐢(𝑑)πœ” = ∑∞
𝑛=1 cos(𝑛𝑑)βŸ¨πœ”, πœ”π‘› βŸ©πœ”π‘› and
(sin(𝑛𝑑)/𝑛)βŸ¨πœ”,
πœ”π‘› βŸ©πœ”π‘› . Consequently,
𝑆(𝑑)πœ” = ∑∞
𝑛=1
‖𝐢(𝑑)β€– = ‖𝑆(𝑑)β€– ≤ 1 for 𝑑 ∈ R, and {𝑆(𝑑)} is compact
for every 𝑑 ∈ R.
Μƒ∗ ∈ (0, 1)
Suppose further that there exists a constant 𝑀
𝑇
∗
Μƒ and 𝑝𝑁 < 1, then (59) has at least
such that 8 ∫0 πœ‚(𝑠)𝑑𝑠 < 𝑀
a mild solution by Theorem 7.
For πœ‰ ∈ [0, πœ‹] and πœ‘ ∈ 𝐢([−π‘Ÿ, 0], 𝑋), we set
Acknowledgments
This work was partly supported by the NSF of China
(11201413), the NSF of Yunnan Province (2009ZC054M), the
Educational Commission of Yunnan Province (2012Z010)
and the Foundation of Key Program of Yunnan Normal
University.
π‘₯ (𝑑) (πœ‰) = 𝑣 (𝑑, πœ‰) ,
πœ™ (πœƒ) (πœ‰) = 𝑣0 (πœƒ, πœ‰) ,
πœƒ ∈ [−π‘Ÿ, 0] ,
πœ‹
𝑔 (πœ‘ (πœƒ)) (πœ‰) = ∫ 𝑐 (πœ‰, 𝑠) sin (1 + πœ‘ (πœƒ) (𝑠)) 𝑑𝑠,
0
󡄨
󡄨
𝑓 (𝑑, πœ‘, π‘₯ (𝑑)) (πœ‰) = sin 󡄨󡄨󡄨π‘₯ (𝑑) (πœ‰)󡄨󡄨󡄨
References
󡄨
󡄨󡄨
0
σ΅„¨πœ‘ (πœƒ) (πœ‰)󡄨󡄨󡄨
+ 𝑑2 ∫ 𝛾 (πœƒ) ⋅ cos ( 󡄨
) π‘‘πœƒ,
𝑑
−π‘Ÿ
πœ‹
πΌπ‘˜ (π‘₯ (π‘‘π‘˜ )) (πœ‰) = ∫ πœŒπ‘˜ (πœ‰, 𝑦) 𝑑𝑦 ⋅ cos2 (π‘₯ (π‘‘π‘˜ ) (πœ‰)) .
0
(62)
Then the above equation (59) can be reformulated as the
abstract (1)–(4).
[1] H. R. Henrı́quez and C. H. Vásquez, “Differentiability of solutions of second-order functional differential equations with
unbounded delay,” Journal of Mathematical Analysis and Applications, vol. 280, no. 2, pp. 284–312, 2003.
[2] F. Li, “Solvability of nonautonomous fractional integrodifferential equations with infinite delay,” Advances in Difference
Equations, vol. 2011, Article ID 806729, 18 pages, 2011.
[3] F. Li, “An existence result for fractional differential equations of
neutral type with infinite delay,” Electronic Journal of Qualitative
Theory of Differential Equations, no. 52, pp. 1–15, 2011.
8
[4] J. Liang and T. J. Xiao, “Solvability of the Cauchy problem for
infinite delay equations,” Nonlinear Analysis: Theory, Methods
& Applications, vol. 58, no. 3-4, pp. 271–297, 2004.
[5] T. J. Xiao and J. Liang, “Blow-up and global existence of solutions to integral equations with infinite delay in Banach spaces,”
Nonlinear Analysis: Theory, Methods & Applications, vol. 71, no.
12, pp. e1442–e1447, 2009.
[6] H. O. Fattorini, Second Order Linear Differential Equations in
Banach Spaces, vol. 108 of North-Holland Mathematics Studies,
North-Holland, Amsterdam, The Netherlands, 1985.
[7] J. A. Goldstein, Semigroups of Linear Operators and Applications,
Oxford Mathematical Monographs, Oxford University Press,
New York, NY, USA, 1985.
[8] J. Kisyński, “On cosine operator functions and one-parameter
groups of operators,” Studia Mathematica, vol. 44, no. 1, pp. 93–
105, 1972.
[9] J. Liang and T. J. Xiao, “A characterization of norm continuity
of propagators for second order abstract differential equations,”
Computers & Mathematics with Applications, vol. 36, no. 2, pp.
87–94, 1998.
[10] J. Liang, R. Nagel, and T. J. Xiao, “Approximation theorems for
the propagators of higher order abstract Cauchy problems,”
Transactions of the American Mathematical Society, vol. 360, no.
4, pp. 1723–1739, 2008.
[11] C. C. Travis and G. F. Webb, “Second order differential equations in Banach space,” in Nonlinear Equations in Abstract Spaces (Proc. Internat. Sympos., Univ. Texas, Arlington, Tex., 1977),
pp. 331–361, Academic Press, New York, NY, USA, 1978.
[12] T. J. Xiao and J. Liang, “Second order linear differential equations with almost periodic solutions,” Acta Mathematica Sinica
(New Series), vol. 7, no. 4, pp. 354–359, 1991.
[13] T. J. Xiao and J. Liang, “Differential operators and 𝐢-wellposedness of complete second order abstract Cauchy problems,”
Pacific Journal of Mathematics, vol. 186, no. 1, pp. 167–200, 1998.
[14] T. J. Xiao and J. Liang, The Cauchy Problem for Higher-Order
Abstract Differential Equations, vol. 1701 of Lecture Notes in
Mathematics, Springer, Berlin, Germany, 1998.
[15] T. J. Xiao and J. Liang, “Higher order abstract Cauchy problems:
their existence and uniqueness families,” Journal of the London
Mathematical Society, vol. 67, no. 1, pp. 149–164, 2003.
[16] N. U. Ahmed, “Optimal feedback control for impulsive systems
on the space of finitely additive measures,” Publicationes Mathematicae Debrecen, vol. 70, no. 3-4, pp. 371–393, 2007.
[17] G. Arthi and K. Balachandran, “Controllability of secondorder impulsive functional differential equations with statedependent delay,” Bulletin of the Korean Mathematical Society,
vol. 48, no. 6, pp. 1271–1290, 2011.
[18] M. Benchohra, J. Henderson, and S. Ntouyas, Impulsive Differential Equations and Inclusions, vol. 2 of Contemporary Mathematics and Its Applications, Hindawi Publishing Corporation,
New York, NY, USA, 2006.
[19] T. Cardinali and P. Rubbioni, “Impulsive semilinear differential
inclusions: topological structure of the solution set and solutions on non-compact domains,” Nonlinear Analysis: Theory,
Methods & Applications, vol. 69, no. 1, pp. 73–84, 2008.
[20] T. Cardinali and P. Rubbioni, “Impulsive mild solutions for semilinear differential inclusions with nonlocal conditions in
Banach spaces,” Nonlinear Analysis: Theory, Methods & Applications, vol. 75, no. 2, pp. 871–879, 2012.
Abstract and Applied Analysis
[21] E. Hernández, K. Balachandran, and N. Annapoorani, “Existence results for a damped second order abstract functional differential equation with impulses,” Mathematical and Computer
Modelling, vol. 50, no. 11-12, pp. 1583–1594, 2009.
[22] E. Hernández M., H. R. Henrı́quez, and M. A. McKibben, “Existence results for abstract impulsive second-order neutral functional differential equations,” Nonlinear Analysis: Theory, Methods & Applications, vol. 70, no. 7, pp. 2736–2751, 2009.
[23] E. Hernández M. and S. M. T. Aki, “Global solutions for abstract
impulsive differential equations,” Nonlinear Analysis: Theory,
Methods & Applications, vol. 72, no. 3-4, pp. 1280–1290, 2010.
[24] J. Liang, J. H. Liu, and T. J. Xiao, “Nonlocal impulsive problems
for nonlinear differential equations in Banach spaces,” Mathematical and Computer Modelling, vol. 49, no. 3-4, pp. 798–804,
2009.
[25] J. H. Liu, “Nonlinear impulsive evolution equations,” Dynamics
of Continuous, Discrete and Impulsive Systems, vol. 6, no. 1, pp.
77–85, 1999.
[26] Y. V. Rogovchenko, “Impulsive evolution systems: main results
and new trends,” Dynamics of Continuous, Discrete and Impulsive Systems, vol. 3, no. 1, pp. 57–88, 1997.
[27] S. T. Zavalishchin, “Impulse dynamic systems and applications
to mathematical economics,” Dynamic Systems and Applications, vol. 3, no. 3, pp. 443–449, 1994.
[28] J. Liang, J. Liu, and T. J. Xiao, “Nonlocal Cauchy problems governed by compact operator families,” Nonlinear Analysis: Theory, Methods & Applications, vol. 57, no. 2, pp. 183–189, 2004.
[29] J. Liang and T. J. Xiao, “Semilinear integrodifferential equations
with nonlocal initial conditions,” Computers & Mathematics
with Applications, vol. 47, no. 6-7, pp. 863–875, 2004.
[30] T. J. Xiao and J. Liang, “Existence of classical solutions to nonautonomous nonlocal parabolic problems,” Nonlinear Analysis:
Theory, Methods & Applications, vol. 63, no. 5–7, pp. e225–e232,
2005.
[31] J. Banaś and K. Goebel, Measures of Noncompactness in Banach
Spaces, vol. 60 of Lecture Notes in Pure and Applied Mathematics,
Marcel Dekker, New York, NY, USA, 1980.
[32] D. Bothe, “Multivalued perturbations of π‘š-accretive differential
inclusions,” Israel Journal of Mathematics, vol. 108, pp. 109–138,
1998.
[33] M. Kamenskii, V. Obukhovskii, and P. Zecca, Condensing Multivalued Maps and Semilinear Differential Inclusions in Banach
Spaces, vol. 7 of De Gruyter Series in Nonlinear Analysis and
Applications, Walter de Gruyter, Berlin, Germany, 2001.
[34] T. Cardinali and P. Rubbioni, “On the existence of mild solutions
of semilinear evolution differential inclusions,” Journal of Mathematical Analysis and Applications, vol. 308, no. 2, pp. 620–635,
2005.
[35] A. Ambrosetti, “Un teorema di esistenza per le equazioni differenziali negli spazi di Banach,” Rendiconti del Seminario Matematico della UniversitaΜ€ di Padova, vol. 39, pp. 349–361, 1967.
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