1. Introduction
Attractors of a given system are of crucial importance, this is because that much of longtime dynamics is represented by the dynamics on and near the attractors. It is well known that the global attractors of dynamical systems can be very complicated. The geometry can be very pathological, even in the finite dimensional situation. To have a better understanding on the dynamics of a system, it is quite necessary for us to study the topology and geometry of the attractors. In the past few decades, there appeared many studies. In [1], Kapitanski and Rodnianski studied the shape of attractors of continuous semi-dynamical systems on general metric spaces. They proved that the global attractor has the same shape as the state space. Moreover, using the results on the shape of attractors, they developed an elementary Morse theory for an attractor. Lately, the author of [2] studied the Morse theory of attractors for semiflows on complete metric spaces by constructing continuous Lyapunov functions, and he introduced the concept of critical groups for Morse sets and established Morse inequalities and Morse equations for attractors. To study the geometry of the attractors, some concepts such as Lyapunov exponents, the Hausdorff dimension and the fractal dimension were also proposed, see [3] [4] etc. Recently, in [5] author studied the geometrical property of the global attractor for a class of symmetric p-Laplacian equations by means of
index, obtained some lower estimates for the fractal dimension of the global attractor.
In this paper, by using Ljusternik-Schnirelmann category (category for short), we try to provide a new approach to studying the geometry of the global attractor. Category is a topological invariant, which often be used in the estimate of the lower bound of the number of critical points, see [6]. Here we investigate the relationship between attractor and attraction basin in the sense of category. In a complete metric space, for asymptotic compact semiflow, we obtain that the categories of attractor and attraction basin are always equal. This result match with the result in [1]. Now we can directly describe this result by category. The result will be of most interest when we choose
be some special metric space. Finally, we have to point out that it is generally not very easy to compute the category of a given space. However, we can see there are more and more new results and methods about calculation of category, see [7] [8] etc.
We will prove the main results in Section 3 and give some applications in Section 4. Before that we provide some preliminaries and results in Section 2.
2. Preliminaries
We recall some basic definitions and facts in the theory of dynamical systems for semiflows on complete metric spaces. Let
be a complete metric space with metric
.
Definition 2.1 A semiflow (semidynamical system) on
is a continuous mapping
that satisfies
for all
and
.
We usually write
as
. Therefore a semiflow
can be viewed as a family of operators
satisfying:

From now on, we will always assume that there has been given a semidynamical system
on
; Moreover, we assume
is asymptotically compact, that is,
satisfies the following assumption:
For any bounded sequence
and
, if the sequence
is bounded, then it has a convergent subsequence.
The asymptotic compactness property (A) is fulfilled by a large number of infinite dimensional semiflows generated by PDEs in application [4].
Let
be a subset of
. We say that
attracts
, if for any
there exists a
such that
![]()
The attraction basin of
, denote by
, is defined as:
![]()
The set
is said to be positively invariant (resp. invariant), if
![]()
Definition 2.2 A compact set
is said to be an attractor of
, if it is invariant and attracts a neighborhood of
itself. An attractor
is said to be the global attractor of
, if it attracts each bounded subset of
.
Let
be an open subset of
, and
be a closed subset of
with
.
Definition 2.3 A function
is said to be coercive with
, if for any
,
![]()
In order to prove our result, we need following theorem (see Theorem 3.5 in [2]). Let there be given an attractor
with attraction basin
.
Theorem 2.4 ([2]) The attractor
has radially unbounded Lyapunov function
on
such that
![]()
where
is a nonnegative function satisfying
![]()
Remark 2.5 We emphasize that the
is coercive with
on
.This point is not contained in the statement of Theorem 2.4, but we can obtain this result from the proof of the Theorem 3.5 in [2] easily.
In the following, we recall some basic results on the Ljusternik-Schnirelmann category (category for short).
Definition 2.6 Let
be a topological space,
be a closed subset. Set
![]()
A set
is called contractible (in
), if
such that
and
one point set.
The category defined above has properties as follows.
Lemma 2.7 Properties for the category:
1)
;
2) (Monotonicity)
;
3) (Subadditivity)
;
4) (Deformation nondecreasing) If
is continuous such that
, then
;
5) (Continuity) If
is compact, then there is a closed neighborhood
of
such that
and
;
6) (Normality)
.
For the proof of this lemma, we refer readers to [6].
Remark 2.8 By (2) and (5), we can easily obtain that if
is compact, then there exists a
-neighborhood
of
, such that
.
Just by the definition of category, we can prove the following lemma:
Lemma 2.9 Let
are topology spaces, and
. F is a subset of
. If
, then ![]()
3. Category of Attractor
The main results can be stated as follows:
Theorem 3.1 Let
be a complete metric space and
is a semiflow on
, which is asymptotically compact. Let
be an attractor of
on
with attraction basin
. Then
.
Proof. Since
, by monotonicity,
. (3.1)
Since
is compact, by continuity (Remark 2.8}), fixed
small enough, we have
(3.2)
If we find a set
such that
(3.3)
by using monotonicity again and (3.2}), we have
(3.4)
Then combine (3.1}) and (3.4), we will obtain the result ![]()
Now the rest of the work in this proof is in finding the appropriate set
, which is subset of
and satisfies (3.3). In order to obtain the proper set
, the key tool here is the level set of Lyapunov function on attractor
. Thanks to Theorem 2.4, we can construct a Lapunov function
. For
, we devote by
the level set of
in
,
![]()
is clearly positively invariant and satisfies
as
.
By the Remark 2.5,
is coercive with
, that is for the fixed
above, there exists
such that
![]()
Hence, let
, we have
.
We use the method in [2], Define a function
on
as
![]()
Here
and
is continuous on
. (See Theorem 5.1 and Lemma 5.2 in [2], in which
replaced by
.) Define
![]()
Then
satisfies:
![]()
Since
is continuous on
, we see that
is a continuous mapping, by deformation nondecreasing and monotonicity, we have
![]()
Now we just let
, which completes the proof.
Now to extend our result to non-autonomous case, we consider a skew-product system, which consists of a base semiflow, and a semiflow on the phase space that is in some sense driven by the base semiflow. More precisely, the base semiflow consists of the base space
, which we take to be a metric space with metric
, and a group of continuous transformations
from
into itself such that
;
for all
.
The dynamics on the phase space
is given by a family of continuous mappings
![]()
satisfy the cocycle property
1)
for all
;
2)
for all
and
;
3)
is continuous.
Then we can define an autonomous semigroup
on
by setting
![]()
If we assume that the autonomous semigroup
is asymptotically compact on
, and has an global attractor
, then we can generalize Theorem 3.1 to the non-autonomous case as follows:
Corollary 3.2 Let
is a asymptotically compact semiflow on
. If
is a global attractor of
on
. Then
.
4. Applications
In this section, we further apply our results to some special metric space
, we will see some interesting results.
Example 1. Assume
. Let
is a asymptotically compact semiflow on
. If
is a global attractor of
on
. Then
.
Proof. Suppose the contrary. Then there exist at least one point
such that
. Then we deduce that
. By the monotonicity, we have ![]()
Note that
is a punctured
-dimensional sphere,
![]()
Thus, we have ![]()
On the other hand, by virtue of Theorem, we have
which leads to a contradiction! Hence, the global attractor
must be phase space
itself.
Using similar arguments, one can prove the case of
.
Example 2. In skew-product flow case, we assume
. Let
is a asymptotically compact semiflow on
. If
is a global attractor of
on
. Then
.
Proof. Suppose the contrary. Then there exist at least one point
such that
. Then we deduce that
. By the monotonicity, we have
![]()
Note that
is a punctured
- dimensional ball, ![]()
By Lemma 2.9,
while by Theorem 15 in [7], we have
![]()
Thus, we have ![]()
On the other hand, by Virtue of Theorem 3.1, we have
which leads to a contradiction! Hence, we obtain
.
Remark 3.3 If
, since
and ![]()
we can obtain the same result.
Remark 3.4 By Theorem 15.7 in [9], if
is a global attractor of
on
. Then
with
is the pullback attractor of the skew-product flow
, where
is the section of
over
. Since corollary 3.2, we can show that the pull back attractor of the skew-product flow
must be
.
Acknowledgements
This work was supported by the National Nature Science Foundation of China (11261027) and Longyuan youth innovative talents support programs of 2014, and by the innovation Funds of principal (LZCU-XZ2014-05).
Support
This work was supported by the National Nature Science Foundation of China (11261027) and Longyuan youth innovative talents support programs of 2014, and by the innovation Funds of principal (LZCU-XZ2014-05).