September 27, 2004 16:46 WSPC/Book Trim Size for 9.75in x 6.5in GlobalAttractors/chapter 2
Non-autonomous Dissipative Dynamical Systems 77
Proof. Necessity. Let h(X, T
1
, π), (Y, T
2
, σ), hi be convergent, then (X, T
1
, π) is
compactly dissipative and J
X
= L
X
. It is easy to see that the Conditions 1 and 2
are fulfilled. We will show that Condition 3 is fulfilled too. Suppose that it is not
so, then there exist ε
0
> 0, δ
n
↓ 0, {x
n
} from X, {y
n
} from J
Y
and t
n
→ +∞ such
that ρ(x
n
, x
y
n
) < δ
n
(y
n
= h(x
n
)) and
ρ(x
n
t
n
, x
y
n
t
n
) ≥ ε
0
. (2.49)
Since the sets J
Y
and J
X
are compact, then we can suppose that the sequences {y
n
}
and {x
y
n
} are convergent. Let y
0
= lim
n→+∞
y
n
, then x
y
0
= lim
n→+∞
x
y
n
= lim
n→+∞
x
n
.
By the compact dissipativity of the dynamical system (X, T
1
, π) we can suppose
that the sequence {x
n
t
n
} is convergent and let ¯x = lim
n→+∞
x
n
t
n
. Since y
n
t
n
∈ J
Y
,
then the sequence {y
n
t
n
} can be considered convergent too. Let ¯y = lim
n→+∞
y
n
t
n
and we note that h(¯x) = lim
n→+∞
h(x
n
)t
n
= lim
n→+∞
y
n
t
n
= ¯y, ¯x ∈ J
X
and hence
¯x ∈ J
X
T
X
¯y
= {x
¯y
}, i.e., ¯x = x
¯y
. On the other hand, passing to limit in (2.49) as
n → +∞ we obtain ρ(¯x, x
¯y
) ≥ ε
0
. The obtained contradiction proves the statement
required.
Sufficiency. Suppose that Conditions 1, 2 and 3 of the theorem are fulfilled. For
the convergence of the system h(X, T
1
, π), (Y, T
2
, σ), hi it is sufficient to show that
under the conditions of the theorem the dynamical system (X, T
1
, π) is compactly
dissipative. By the condition of the theorem (X, T
1
, π) is point dissipative and
Ω
X
=
S
{ω
x
| x ∈ X} ⊆ L
X
. Note, that the set L
X
is closed. We will show that
the set L
X
is orbitally stable. If we suppose that it is not true, then there exist
ε
0
> 0, x
n
→ x
0
∈ L
X
and t
n
→ +∞ such that
ρ(x
n
t
n
, L
X
) ≥ ε
0
.
Since y
n
→ y
0
= h(x
0
), where y
n
= h(x
n
), then under the conditions of the theorem
x
y
n
→ x
y
0
= x
0
and, consequently, ρ(x
n
, x
y
n
) ≤ ρ(x
n
, x
0
) + ρ(x
0
, x
y
n
) → 0. From
this relation and Condition 3 of the theorem follows that ρ(x
n
t
n
, x
y
n
t
n
) → 0. This
relation and the inequality (2.49) are contradictory. Thus, L
X
is compact, invariant
and orbitally stable. Since Ω
X
⊆ L
X
, then J
+
(Ω
X
) ⊆ L
X
. Let us show that
J
+
(Ω
X
) = J
X
. In fact, let ¯x ∈ L
X
and ϕ : S → L
X
be a whole trajectory
of (X, T
1
, π) passing through point ¯x for t = 0. Denote by α
ϕ
¯x
:=
T
t≤0
S
τ≤t
ϕ(τ),
then Ω
X
T
α
ϕ
¯x
6= ∅. Let p ∈ α
ϕ
¯x
T
Ω
X
, then there exists t
n
→ −∞ such that
ϕ(t
n
) → p and, consequently, π
−t
n
ϕ(t
n
) = ϕ(0) = ¯x, i.e., ¯x ∈ J
+
p
⊆ J
+
(Ω
X
).
Thus, L
X
⊆ J
+
(Ω
X
), i.e. L
X
= J
+
(Ω
X
) is compact and orbitally stable and
by Theorem 1.13 the dynamical system (X, T
1
, π) is compactly dissipative. The
theorem is proved.
Theorem 2.13 Let h(X, T
1
, π), (Y, T
2
, σ), hi be a non-autonomous dynamical
system and Y be a compact minimal set, then the following conditions are equivalent: