September 27, 2004 16:46 WSPC/Book Trim Size for 9.75in x 6.5in GlobalAttractors/chapter 2
56 Global Attractors of Non-autonomous Dissipative Dynamical Systems
system (2.1) is compactly dissipative, then the set H
+
({x
n
}) is compact and, conse-
quently, we may suppose that the sequences {x
n
t
n
} and {h(x
n
)t
n
} are convergent.
Put ¯x := lim
n→+∞
x
n
t
n
and ¯y := lim
n→+∞
h(x
n
)t
n
.
We will show now that the sequence {t
n
} figuring in the equality (2.10) tends to
+∞. If we suppose that it is not true, then we may suppose that it is convergent.
Denote by t
0
:= lim
n→+∞
t
n
and, passing to limit in the inequality (2.10) and taking
into consideration that the set J satisfies the condition (C), we obtain
ρ(x
0
t
0
, J
h(x
0
)t
0
) ≥ ε
0
. (2.11)
On the other hand, ρ(x
n
, J
h(x
n
)
) < δ
n
and, consequently, x
0
∈ J
h(x
0
)
. Since the
set J is invariant, then from the last inclusion follows that x
0
t
0
∈ J
h(x
0
)t
0
. But it
contradicts the inequality (2.11). Thus, t
n
→ +∞ and, consequently, ¯x ∈ ω(K
0
) ⊆
J. From the equality (2.5) follows that ¯x ∈ X
¯y
, i.e. ¯x ∈ ω
¯y
(K) ⊆ J
¯y
. From the
inequality (2.6) it follows that ¯x ∈ X
¯y
, i.e., ¯x ∈ ω
¯y
(K) ⊆ J
¯y
.
Passing to limit in the inequality (2.10) as n → +∞ and taking into account
that ¯x ∈ J
¯y
and the fact that the set J possesses the property (C), we obtain ε
0
≤ 0.
But this contradicts the choice of the number ε
0
. Thus, the orbital stability of the
set J in the positive direction is proved.
Now we will prove the second statement of the theorem. Let K ⊆ X be an
arbitrary compact, then under the conditions of the theorem the set H
+
(K) is
compact and ω(K) ⊆ J. To finish the proof of the theorem it is sufficient to refer
to Lemma 2.2.
Remark 2.1 We note, that the problem of the stability in the sense of Lyapunov-
Barbashin of the Levinson center of a non-autonomous dynamical system has been
studied (in one special case) in the work
[
332
]
. We also note that in the work
[
332
]
stability means the equality (2.9), but not orbital stability. Using our terminology we
can formulate the results of the work
[
332
]
in the following way. Let X be a locally
compact space, the non-autonomous dynamical system (2.1) be pointwise dissipative
and Y be a compact minimal set. If the Levinson center J of the dynamical system
(X, T, π) satisfies the condition (C), then the non-autonomous dynamical system
h(X, T
1
, π), (Y, T
2
, σ), hi is compactly dissipative and its Levinson center attracts
every compact subset from X with respect to the non-autonomous dynamical system
(2.1).
This statement follows from Theorems 1.10 and 2.1. However, from the same
theorems follows that the Levinson center J is orbitally stable in the positive direc-
tion.
Theorem 2.2 Let h(X, T
1
, π), (Y, T
2
, σ), hi be a compact dissipative non-
autonomous dynamical system, its Levinson center J satisfy the condition (C) and
h(J) = Y , then the following conditions are equivalent: