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2 Periodic Oscillatory Solutions
In this section, we will consider the periodic oscillatory solutions of system (1),
we give the following assumption.
τ
ij CR
(,[0, )
ω
for ,
ij
=
, ,
, .
n
(A2)
are periodic functions with periodic
cCR a THuICRR
(
, (0,
)),
,
αβ
,
,
,
,
,
(
,
)
(A3)
are periodic functions
i
ij
ij
ij
ij
ij
j
i
We will use the coincidence degree theory to obtain the existence of an
ω
j f CRRi
(, ,,
j
=
1,2, ,.
n
with common periodic
and
ω
-
periodic solution to system (1).
Lemma 3. [12] Let L be a Fredholm mapping of index zero and let N be L -compact
on
Ω
. Suppose that
λ ∈
(0,1)
, every solution x of Lx
=
λ
Nx
is such that x
∉∂Ω
(a) for each
.
QNx
0
for each x
∈∂Ω
KerL
and deg{
JQN
,
Ω
Ker L
, 0}
0
(b)
.
Then the equation Lx Nx
.
To be convenience, in the rest of paper, for a continuous function
=
has at least one solution lying in DomL
Ω
g
:[0,
ω
]
,
R
we denote
1
ω
g
+
=
max
g t
( )
g
=
min
g t
( )
g
=
g t dt
()
,
,
ω
0
t
[0,
ω
]
t
[0,
ω
]
k
=+
(
ωαβ
)(|
a
|
+
|
|
+
|
|)
p
1
Theorem 1. Under assumptions (A1); (A2) and (A3),
,
ij
c
ij
ij
ij
j
Kk ×
=
()
ij n n
ρ
()1
K
<
ω
.Suppose that
, then system (1) has at least an
-periodic
solution.
T
n
XZxt xtxt xt CRRxt xt
==
{()(( ,( ,,( )
=
(, ):(
+ =
ω
) ( }
Proof. Take
.
1
2
n
x
=
max
max
|
x t
( ) |
and denote
. Equipped with the norm
, both
1
≤≤
in
t
[0,
ω
]
i
X and Z are Banach space. For any
xt X
()
, it is easy to check that
n
n
Θ= −
( , ):
xt ctxt atf xt
() ()
+
() ( ())
+ ∧
α
() ( (
tf xt t It
τ
()))
+
()
i
i
i
ij
j
j
ij
j
j
ij
i
j
=
1
j
=
1
n
n
n
+∨
β
()(
tft t Ttut Htut Z
τ
( )
+∧
()()
+∨
()()
ij
j
ij
ij
j
ij
j
j
=
1
j
=
1
j
=
1
Let
1
ω
LDomL x Xx CRR x x Z
:
=∈
{
:
( ,
n
)}
'
( )
⋅∈
.
PX x
:
xtdt X
( )
ω
0
 
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