Math Sci (2015) 9:189–192
DOI 10.1007/s40096-015-0166-5
ORIGINAL RESEARCH
Asymptotic equilibrium of integro-differential equations
with infinite delay
Le Anh Minh1 • Dang Dinh Chau2
Received: 25 June 2014 / Accepted: 2 September 2015 / Published online: 21 September 2015
Ó The Author(s) 2015. This article is published with open access at Springerlink.com
Abstract The asymptotic equilibrium problems of ordinary differential equations in a Banach space have been
considered by several authors. In this paper, we investigate
the asymptotic equilibrium of the integro-differential
equations with infinite delay in a Hilbert space.
Keywords Asymptotic equilibrium Á Integro-differential
equations Á Infinite delay
8
0
1
Zt
>
>
< dxðtÞ
¼ AðtÞ@ xðtÞ þ
kðt À hÞxðhÞdhA;
dt
>
À1
>
:
xðtÞ ¼ uðtÞ;
t > 0;
t60
ð1Þ
where AðtÞ : H ! H, u in the phase space B, and xt is
defined as
xt ðhÞ ¼ xðt þ hÞ;
À1\h 6 0:
Introduction
The asymptotic equilibrium problems of ordinary differential equations in a Banach space have been considered by
several authors, Mitchell and Mitchell [3], Bay et al. [1],
but the results for the asymptotic equilibrium of integrodifferential equations with infinite delay still is not presented. In this paper, we extend the results in [1] to a class
of integro-differential equations with infinite delay in a
Hilbert space H which has the following form:
Preliminaries
We assume that the phase space ðB; jj:jjB Þ is a seminormed
linear space of functions mapping ðÀ1; 0 into H satisfying the following fundamental axioms (we refer reader to
[2])
(A1 )
For a [ 0, if x is a function mapping ðÀ1; a into
H, such that x 2 B and x is continuous on [0, a],
then for every t 2 ½0; a the following conditions
hold:
(i)
(ii)
(iii)
& Le Anh Minh
Dang Dinh Chau
1
Department of Mathematical Analysis, Hong Duc University,
Thanh Ho´a, Vietnam
2
Department of Mathematics, Hanoi University of Science,
VNU, Hanoi, Vietnam
xt belongs to B;
jjxðtÞjj 6 Gjjxt jjB ;
jjxt jjB 6 KðtÞ sups2½0;t jjxðsÞjj þ MðtÞjjx0 jjB
where G is a possitive constant, K; M : ½0; 1Þ ! ½0; 1Þ,
K is continuous, M is locally bounded, and they are independent of x.
(A2 )
(A3 )
For the function x in (A1 ), xt is a B-valued
continuous function for t in [0, a].
The space B is complete.
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190
Math Sci (2015) 9:189–192
Example 1
(i)
(M4 )
Let BC be the space of all bounded continuous
functions from ðÀ1; 0 to H, we define C0 :¼
fu 2 BC : limh!À1 uðhÞ ¼ 0g and C1 :¼ fu 2
BC : limh!À1 uðhÞ exists in Hg endowed with the
norm
jjujjB ¼
(ii)
sup
&
'
u 2 CððÀ1; 0; XÞ : lim ech uðhÞ exists in H
T
herein S(0, 1) is a unit ball in H, j ¼ LðK þ MÞ þ
1; where K, M, L are given in (c1 ), (c2 ) and (M3 ).
h!À1
Theorem 1 If (M1 ), ðM2 Þ, ðM3 Þ and ðM4 Þ are satisfied,
then Eq. (1) has an asymptotic equilibrium.
Proof We shall begin with showing that all solutions of
(1) has a finite limit at infinity. Indeed, Eq. (1) may be
rewritten as
0
1
Z0
dxðtÞ
¼ AðtÞ@ xðtÞ þ
kðÀhÞxt ðhÞdhA ;
dt
À1
endowed with the norm
jjujjB ¼
sup
ð2Þ
jjuðhÞjj
h2ðÀ1;0
then C0 ; C1 satisfies (A1 )–(A3 ). However, BC
satisfies (A1 ) and (A3 ), but (A2 ) is not satisfied.
For any real constant c, we define the functional
spaces Cc by
Cc ¼
There exists a constant T [ 0 such that
Z1
1
jjAðtÞhjjdt\q\ ;
sup
j
h2Sð0;1Þ
ech jjuðhÞjj:
h2ðÀ1;0
Then conditions (A1 )–(A3 ) are satisfied in Cc .
then for t > s > T we have
0
1
Z0
Zt
kðÀhÞxs ðhÞdhAds
xðtÞ ¼ xðsÞ þ AðsÞ@ xðsÞ þ
À1
s
Remark 1 In this paper, we use the following acceptable
hypotheses on K(t), M(t) in (A1 )(iii) which were introduced
by Hale and Kato [2] to estimate solutions as t ! 1,
and
jjxðtÞjj
*
0
1
+
Zt
Z0
kðÀhÞxs ðhÞdhAds; h
¼ sup xðsÞ þ AðsÞ@xðsÞ þ
h2Sð0;1Þ
s
À1
*
+
Z0
Z t
ds
xðsÞ þ
6 jjxðsÞjj þ sup
kðÀhÞx
ðhÞdh;AðsÞh
s
h2Sð0;1Þ
s
À1
!
(c1 ) K ¼ KðtÞ is a constant for all t > 0;
(c2 ) MðtÞ 6 M for all t > 0 and some M.
Example 2 For the functional space Cc in Example 1, the
hypotheses (c1 ) and (c2 ) are satisfied if c > 0.
Definition 1 Equation (1) has an asymptotic equilibrium
if every solution of it has a finite limit at infinity and, for
every h0 2 H, there exists a solution x(t) of it such that
xðtÞ ! h0 as t ! 1.
Main results
6 jjxðsÞjj þ q ðLK þ 1Þ sup jjxðnÞjj þ LMjjujjB
n2½0;t
ð3Þ
implies
À
Á
jjjxðtÞjjj 6 jjxðsÞjj þ q ðLK þ 1ÞjjjxðtÞjjj þ LMjjujjB
or
Now, we consider the asymptotic equilibrium of Eq. (1)
which satisfies the following assumptions:
(M1 )
(M2 )
(M3 )
A(t) is a strongly continuous bounded linear
operator for each t 2 Rþ ;
A(t) is a self-adjoint operator for each t 2 Rþ ;
k satisfies
Zþ1
jkðhÞjdh ¼ L\ þ 1;
0
and
123
jjjxðtÞjjj 6
jjxðsÞjj þ qLMjjujjB
1 À qðLK þ 1Þ
where
jjjxðtÞjjj ¼ sup jjxðnÞjj:
06n6t
ð4Þ
Math Sci (2015) 9:189–192
191
Now, we conclude that x(t) is bounded since
0\q\
1
1
1
¼
\
) qðLK þ 1Þ\1
j LðK þ MÞ þ 1 LK þ 1
and by (4).
Putting
and
jjx1 ðtÞjj 6 jjh0 jjð1 þ qjÞ:
Now, we consider the functional
g2 ðt; hÞ ¼ hh0 ; hi
0
1 +
Zþ1*
Zs
À
AðsÞ@x1 ðtÞ þ
kðs À hÞx1 ðhÞdhA; h ds:
M Ã ¼ sup jjxðtÞjj;
t2R
À1
t
we have
By an argument analogous to the previous one, we get
jjxðtÞ À xðsÞjj ¼ sup j \xðtÞ À xðsÞ; h [ j
h2Sð0;1Þ
0
1
Zt
Z0
ds
\AðsÞ@xðsÞ þ
A
kðÀhÞx
ðhÞdh
;
h
[
6 sup
s
;
h2Sð0;1Þ
À1
s
Ã
6 ½M ðLK þ 1Þ þ LMjjujjB sup
h2Sð0;1Þ
Zt
jg2 ðt; hÞj 6 jjh0 jj½jjhjj þ qj þ ðqjÞ2
and there exists an element x2 ðtÞ in H, such that
g2 ðt; hÞ ¼ hx2 ðtÞ; hi
with
jjAðsÞhjjds ! 0
jjx2 ðtÞjj 6 jjh0 jjð1 þ qj þ ðqjÞ2 Þ:
s
as t > s ! þ1. That means all solutions of (1) have a
finite limit at infinity. To complete the proof, it remains to
show that for any h0 2 H, there exists a solution x(t) of (1)
such that
lim xðtÞ ¼ h0 :
Continuing this process, we obtain the linear continuous
functional
gn ðt; hÞ ¼ hh0 ; hi
0
1 +
Zþ1*
Zs
À
AðsÞ@xnÀ1 ðtÞ þ
kðs À hÞxnÀ1 ðhÞdhA; h ds
À1
t
t!þ1
Indeed, let h0 be an arbitrary fixed element of H; we choose
the initial function u belongs to B such that uð0Þ ¼ h0 and
jjujjB 6 jjh0 jj and consider the functional
g1 ðt; hÞ ¼ hh0 ; hi
0
1 +
Z1*
Zs
À
AðsÞ@h0 þ
kðs À hÞx0 ðhÞdhA; h ds
ð5Þ
and xn ðtÞ 2 H such that
gn ðt; hÞ ¼ hxn ðtÞ; hi
satisfies the following estimate
jjxn ðtÞjj 6 ð1 þ qj þ ðqjÞ2 þ Á Á Á þ ðqjÞn Þjjh0 jj 6
À1
t
jjh0 jj
:
1 À qj
Futhermore,
We have
jg1 ðt; hÞj 6 jjh0 jjjjhjj þ
Zþ1
kxn ðtÞ À xnÀ1 ðtÞk 6 jjh0 jjðqjÞn :
kx0 ðsÞ
t
þ
Zs
kðs À hÞx0 ðhÞdhkjjAðsÞhjjds::
À1
Since x0 ðsÞ h0 ; then
jg1 ðt; hÞj 6 jjh0 jjðjjhjj þ qjÞ:
It follows from Riesz representation theorem that there
exists an element x1 ðtÞ in H, such that
g1 ðt; hÞ ¼ hx1 ðtÞ; hi
This inequality shows that fxn ðtÞg is uniformly convergent
on ½T; þ1Þ since qj\1. Put
xðtÞ ¼ lim xn ðtÞ:
n!þ1
In (5), let n ! þ1; we have
hxðtÞ; hi ¼ hh0 ; hi
0
1 +
Zþ1*
Zs
À
AðsÞ@xðtÞ þ
kðs À hÞxðhÞdhA; h ds
t
À1
ð6Þ
and since
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Math Sci (2015) 9:189–192
jhxn ðtÞ; h0 ij\
Zþ1
kxnÀ1 ðsÞ
T
þ
Zs
creativecommons.org/licenses/by/4.0/), which permits unrestricted
use, distribution, and reproduction in any medium, provided you give
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link to the Creative Commons license, and indicate if changes were
made.
kðs À hÞxnÀ1 ðhÞdhkk AðsÞhkds
À1
or
jjh0 jjq
;
jhxn ðtÞ; h0 ij 6
1 À qj
we have xn ðtÞ ! h0 as q ! 0, which means that there
exists a solution of (1) converging to h0 . The theorem is
proved.
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123
References
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2. Hale, J.K., Kato, J.: Phase space for retarded equations with
infinite delay. Fukcialaj Ekvacioj 21, 11–41 (1978)
3. Mitchell, A.R., Mitchell, R.W.: Asymptotic equilibrium of ordinary differential systems in a Banach space. Theory Comput. Syst.
9(3), 308–314 (1975)