Topological transitivity
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| Sergiy Kolyada and Ľubomír Snoha (2009), Scholarpedia, 4(2):5802. | revision #64940 [link to/cite this article] | |||||||||||||||||||
Curator: Dr. Sergiy Kolyada, Institute of Mathematics, NASU, Ukraine
Curator: Dr. Ľubomír Snoha, Department of Mathematics, Faculty of Natural Sciences, Matej Bel University, Banská Bystrica, Slovakia
The concept of topological transitivity goes back to G. D. Birkhoff [1] who introduced it in 1920 (for flows). This article will concentrate on topological transitivity of dynamical systems given by continuous mappings in metric spaces. Intuitively, a topologically transitive dynamical system has points which eventually move under iteration from one arbitrarily small open set to any other. Consequently, such a dynamical system cannot be decomposed into two disjoint sets with nonempty interiors which do not interact under the transformation.
Topological transitivity versus the existence of a dense orbit
Let
be a metric space with the metric
and
be continuous. The dynamical system
is called topologically transitive if it satisfies the following condition.
- (TT) For every pair of non-empty open sets
and
in
there is a non-negative integer
such that
However, some authors choose, instead of (TT), the following condition as the definition of topological transitivity.
- (DO) There is a point
such that the orbit
is dense in
Unfortunately, the two conditions are independent in general. To see that (DO) does not imply (TT), consider
endowed with the usual metric and
defined by
and
. To show that (TT) does not imply (DO), start with
and the standard tent map
from
to itself. Then let
be the union of all periodic orbits of
and
The system
does not satisfy the condition (DO), since
is infinite (dense in
) while the orbit of any periodic point is finite. On the other hand, every pair of subintervals of
shares a periodic orbit of the tent map and so
satisfies (TT).
Nevertheless, under some additional assumptions on the phase space (or on the map) the two conditions (TT) and (DO) are equivalent. In fact, if
has no isolated point then (DO) implies (TT) and if
is separable and second category then (TT) implies (DO) ([Silv]).
The systems satisfying (DO) are sometimes called point transitive. In the sequel, when speaking on transitivity, we have topological transitivity in mind.
Some of the equivalent definitions of transitivity
For subsets
and
of
define the hitting time set
. Let
be a dynamical system. Then the following are equivalent:
is topologically transitive (i.e., (TT) is fulfilled),
- for every pair of non-empty open sets
and
in
the hitting time set
is infinite,
- for every non-empty open set
in
the (forward) orbit of
is dense in
,
- for every non-empty open set
in
the backward orbit of
is dense in
,
- every proper closed (forward) invariant subset of
is nowhere dense,
- every backward invariant subset of
with non-empty interior is dense.
When studying topological transitivity, it is not restrictive to consider only phase spaces without isolated points. In fact, if a transitive system has an isolated point then the system is trivial, consisting of just one periodic orbit.
Some examples of transitive maps
Every minimal dynamical system is transitive (a system is minimal if all orbits are dense).
Example 1. Consider a homeomorphism of the
-torus,
,
of the form
, where
are rationally independent and
is defined in the obvious way. Then
is
minimal (and ergodic with respect to Lebesgue measure). M. Rees [R]
found a minimal homeomorphism
which is an extension of
(i.e.,
for some continuous surjection
of
) such that
has positive
topological entropy. In fact every
-manifold,
, which carries a minimal homeomorphism also carries a minimal homeomorphism with positive topological entropy [BCLR].
Example 2. Let
be a sequence of integers
. Let
be the set of all one-sided infinite sequences
for which
. Think of these sequences as 'integers' in multibase notation, the base of the
digit
being
. With the natural (product) topology,
is homeomorphic to the Cantor set. Define a map
which informally may be described as 'add 1 and carry' where the addition is performed at the leftmost term
and the carry proceeds to the right in multibase notation. Then
is a minimal homeomorphism and is called a generalized adding machine or an odometer.
Non-minimal transitive systems.
Example 3. The logistic map
defined on the interval
is topologically transitive. This follows from the fact that the tent map
is topologically conjugate to
, the conjugating homeomorphism being
.
Example 4. Symbolic dynamics provides many examples of transitive dynamical systems. A subshift of finite type is topologically transitive if and only if its transition matrix
is irreducible which means that for every
there is a positive integer
such that the
entry of the matrix power
is strictly positive.
Every compact, connected
-manifold (possibly with boundary),
, admits a transitive homeomorphism [Al]. Moreover, such homeomorphisms are typical, with respect to the uniform topology, in the space of all measure preserving homeomorphisms [DF]. The first results of this kind were [Ox] and [OU] (see also [AnK] and [AP]).
Concerning noncompact manifolds, Besicovitch [Bes] gave the first explicit example of a transitive homeomorphism of the plane. Transitive homeomorphisms exist in fact on
-compact connected
-manifolds,
, and in some cases they are dense, in the compact open topology, in the space of all measure preserving homeomorphisms [AP1]. See also [AP].
There are spaces, even metric continua, which do not admit transitive maps. Though for instance a characterization of locally compact subspaces of the real line admitting a transitive map is known (see [NK]), no characterization of compact metric spaces admitting transitive maps is known.
However, in [AC] it is proved that every finite union of disjoint nondegenerate Peano continua in
admits a transitive map.
Transitivity of a map and its iterates
A system
is called totally transitive, if the system
is transitive for every
. If
is topologically transitive but
is not, then there are an integer
dividing
and sets
such that:
-
,
- each
is regular closed (i.e., it is the closure of its interior),
-
is nowhere dense whenever
,
-
,
-
(hence also
) is transitive on each
.
For more details on this topic see [Ban].
Transitive and intransitive points
Any point with dense orbit is called a transitive point. A point which is not transitive is called intransitive. The image of an intransitive point is intransitive and if the phase space has no isolated point then also the image of a transitive point is transitive. Further, if the phase space of a system
has a countable base
of open sets then the set of transitive points can be expressed in the form
and so it is a
set.
The set of transitive or intransitive points of
will be denoted by
or
, respectively. Assume that
is a compact metric space without isolated points. Then one of the following holds (see [Kin] or [KS]):
-
and
-
and
(in this case the system
is called minimal),
-
is dense
and
is dense
.
Hitting times and notions related to transitivity
A system
is called topologically weakly mixing when the product system
is topologically transitive. An equivalent definition is that for every pair of non-empty open subsets
and
of
the hitting time set
contains arbitrarily long intervals of positive integers ([Fur], see also [Ak1]). Some stronger notions of mixing in topological dynamics can also be characterized in terms of hitting time sets (see [GW]).
Transitivity and chaos
Transitivity is a widely accepted feature of chaos. It is often required in definitions of chaos as one of several ingredients. However, transitivity alone is pretty compatible with a very regular behavior of trajectories --- in fact, a transitive system is either very regular or very non-regular. To describe this dichotomy in more details, we need to recall some definitions.
A point
is called Lyapunov stable if, for any
, there exists
such that the inequality
yields
for all integers
. This condition means that the iteration sequence
is equicontinuous at the point
. A point of this type is therefore also called an equicontinuity point. The system
is called almost equicontinuous if there is a dense
set of equicontinuity points.
So, a point
is not Lyapunov stable if there is
such that arbitrarily close to
there are points
with
for some
. We then say that
is Lyapunov
-unstable. A system
is said to exhibit sensitive dependence on initial conditions (or is shortly called sensitive) if there exists
such that every point
is Lyapunov
-unstable. The notion of sensitivity for a system
is equivalent to the condition that there exists
such that for every non-empty open set
in
there exist
with
.
A transitive system
is either sensitive or almost equicontinuous. In the latter case the set of equicontinuity points coincides with the set of transitive points and the map
is a homeomorphism and is uniformly rigid (see [AAB]). For more information on the relation between transitivity and various concepts of chaos see [AK], [Bl], [Kol], [XJ].
Transitivity and topological entropy
In compact metric spaces in general there is no connection between topological transitivity and topological entropy. A system with positive topological entropy need not of course be transitive (transitivity is a global property of a system while a system may have positive topological entropy on some small invariant subset, without being transitive). On the other hand, a transitive system may have zero topological entropy. However, in some spaces topologically transitive maps have necessarily positive topological entropy. For instance, on a real compact interval every transitive map has topological entropy at least
and there is a transitive map with topological entropy equal
. For more information on best lower bounds for the topological entropy of transitive maps in various spaces see [AKLS], [BS].
Transitivity of (semi)group actions
Topological transitivity can be studied in a more general setting. An action of a semigroup
on a space
is called topologically transitive if, for every pair of non-empty open sets
and
in
, there is an element
such that
. Usually it is at least assumed that the action is separately continuous in the space variable which means that, for each element
, the corresponding map
is continuous. When
is a group, usually it is required that for each element
, the corresponding map
be a homeomorphism, see e.g. [CKN].
However, note that the required partial continuity of an action of a (semi)group is just the minimum requirement in topological dynamics. In fact, abstract topological dynamics is usually developed in the context of (semi)flows. A (semi)flow is a jointly continuous action of a topological (semi)group
on a space
.
In this article we have in fact considered topological transitivity of
-actions where
is the additive semigroup
. Such an action is given by a map
. We have assumed continuity of
and so our dynamical system was a particular case of a semiflow (
is a topological semigroup with respect to the discrete topology).
For more information on topological transitivity of flows see [GH] and [dV] (in [GH] it is called regional transitivity and in [dV] it is called topological ergodicity). Topological transitivity of partially continuous actions of groups is discussed in [CKN].
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Internal references
- Olaf Sporns (2007) Complexity. Scholarpedia, 2(10):1623.
- Yuri A. Kuznetsov (2007) Conjugate maps. Scholarpedia, 2(12):5420.
- James Meiss (2007) Dynamical systems. Scholarpedia, 2(2):1629.
- Tomasz Downarowicz (2007) Entropy. Scholarpedia, 2(11):3901.
- Jeff Moehlis, Kresimir Josic, Eric T. Shea-Brown (2006) Periodic orbit. Scholarpedia, 1(7):1358.
- Philip Holmes and Eric T. Shea-Brown (2006) Stability. Scholarpedia, 1(10):1838.
- David H. Terman and Eugene M. Izhikevich (2008) State space. Scholarpedia, 3(3):1924.
- Brian Marcus and Susan Williams (2008) Symbolic dynamics. Scholarpedia, 3(11):2923.
- Joseph Auslander (2008) Topological dynamics. Scholarpedia, 3(6):3449.
- Roy Adler, Tomasz Downarowicz, Michał Misiurewicz (2008) Topological entropy. Scholarpedia, 3(2):2200.
See also
Chaos, Complexity, Entropy, Entropy in Chaotic Dynamics, Ergodic theory, Topological dynamics, Topological entropy.
External links
Wikipedia: Topological entropy
Wikipedia: Topological entropy (in physics)
PlanetMath: Topological entropy
| Sergiy Kolyada, Ľubomír Snoha (2009) Topological transitivity. Scholarpedia, 4(2):5802, (go to the first approved version) Created: 3 December 2007, reviewed: 18 February 2009, accepted: 18 February 2009 |
| Invited by: | Prof. James Meiss, Applied Mathematics University of Colorado |
| Action editor: | Prof. James Meiss, Applied Mathematics University of Colorado |


