Specification properties on uniform spaces
Fatemah Ayatollah Zadeh Shirazi, Zahra Nili Ahmadabadi,
Bahman Taherkhani,
Khosro Tajbakhsh
Abstract.
In the following text we introduce specification property (stroboscopical property) for
dynamical systems on uniform space.
We focus on two classes of dynamical systems: generalized shifts and
dynamical systems with Alexandroff compactification of a discrete space as phase space.
We prove that for a discrete finite topological space X with at least two elements,
a nonempty set Γ and a self–map φ:Γ→Γ the generalized shift
dynamical system (XΓ,σφ):
has (almost) weak specification property if and only if φ:Γ→Γ
does not have any periodic point,
has (uniform) stroboscopical property if and only if φ:Γ→Γ
is one-to-one.
Key words and phrases:
Fort space, generalized shift, specification, stroboscopical.
2010 Mathematics Subject Classification:
37B99, 54H20
1. Introduction
The main purpose
of this paper is to generalize tracing properties to uniform spaces and in particular
to compact Hausdorff spaces (one may find similar ideas in [12, 4]).
The action of a group G on metric space (Z,d) is sensitive if there exists
ϵ>0 such that for all x∈Z and any open neighbourhood U of x there exists
y∈U and g∈G with d(gx,gy)≥ϵ. T. Ceccherini–Silberstein and M. Coornaert [4]
indicate that the action of a group G on a uniform space (Y,F) is sensitive if there exists
α∈F such that for all x∈Y and any open neighbourhood U of x there exists
y∈U and g∈G with (gx,gy)∈/α. In this paper we introduce specification properties for
dynamical systems on uniform space .
We realize our generalizations in uniform spaces through two classes of dynamical systems
“generalized shift dynamical systems” and “dynamical systems with Alexandroff
compactification of a discrete space as phase space” on various specification and
stroboscopical properties.
2. Preliminaries
Let’s recall that for an arbitrary set Y we call the collection F of subsets of Y×Y a uniform
structure on Y if :
∀α∈F(ΔY⊆α);
∀α,β∈F(α∩β∈F);
∀α∈F∃β∈F(β∘β−1⊆α);
∀α∈F∀β⊆Y×Y(α⊆β⇒β∈F).
where for α,β⊆X×X we have
α−1={(y,x):(x,y)∈α} and α∘β={(x,z):∃y((x,y)∈β∧(y,z)∈α)} also ΔY={(x,x):x∈Y}) [6].
Moreover, for all α∈F and x∈Y let α[x]={y∈Y:(x,y)∈α}.
For uniform structure F on
Y, the collection {U⊆Y:∀x∈Y∃α∈F(α[x]⊆U)} is a topology on Y, we call it the uniform topology induced from F,
so accordingly we denote this topological space by uniform topological space (Y,F)
whenever we want to emphasize F.
We call the topological space Z uniformizable if there exists a
uniform structure G in Z
such that uniform topology induced from G coincides with original topology on Z, and
in this case we call G compatible uniform structure on Z.
Every compact Hausdorff (and in particular, compact metric)
space is uniformizable and has a unique compatible uniform structure.
Note to the fact that compact metric space(Z,d) has a unique
compatible uniform structure {D⊆Z×Z:∃κ>0({(x,y)∈Z×Z:d(x,y)<κ}⊆D)}.
In this text by a dynamical system (Y,h) we mean a topological space Y
and continuous map h:Y→Y.
Similar to the definition of specification properties in metric spaces
[5] we have the following
definition.
Definition 2.1**.**
For a uniform topological
space (Y,F), we say that the dynamical system
((Y,F),h) (or briefly (Y,h)) has almost weak specification property
if for all α∈F
there exists a map Nα:Z+→Z+
with n→∞limnNα(n)=0
such that for all y1,…,yn∈Y (n≥2) and
0≤l1≤k1<l2≤k2<…<ln≤kn with
li+1−ki≥Nα(ki+1−li+1)
(for all i=1,…,n−1) there exists x∈Y
such that
[TABLE]
If in the above definition we suppose in addition that Nα is a constant map
(resp. and x is a periodic point of h),
then we say that ((Y,F),h) has weak specification property
(resp. specification property).
Let’s recall that in the dynamical system (Z,f), for x∈Z and
strictly increasing sequence A={ni}i≥0 in N
we set ωf(A,x)={y∈Z:{fni(x)}i≥0 has a subsequence converging to y}.
Now for definition of various stroboscopical properties see [8].
Definition 2.2**.**
We say that (Z,f) has stroboscopical property (resp. strongly stroboscopical property)
if for all z∈Z and every
strictly increasing sequence A={ni}i≥0 in N,
{x∈Z:z∈ωf(A,x)} is a nonempty (resp. dense) subset of Z.
Moreover if (Z,F) is a uniform space and for all
strictly increasing sequence A={ni}i≥0 in N there exists
a subsequence B={ki}i≥0 of A and ϱ:Z→Z
such that the sequence {fki∘ϱ}i≥0 converges
uniformly to idZ, then we say that ((Z,F),f) has uniform stroboscopical property.
Generalized shifts
The one sided shift (xn)n≥1↦(xn+1)n≥1{1,…,k}N→{1,…,k}N
and two sided shift (xn)n∈Z↦(xn+1)n∈Z{1,…,k}Z→{1,…,k}Z
due to P. Walters [11] have been investigated very well from the ergodic theory and dynamical systems point of
view.
For nonempty sets X and Γ
and arbitrary map φ:Γ→Γ,
we call σφ:XΓ→XΓ with
σφ((xα)α∈Γ)=(xφ(α))α∈Γ
(for (xα)α∈Γ∈XΓ), a generalized shift.
Whenever X is a topological space and
XΓ is equiped with product (pointwise convergence) topology, it’s evident that
σφ:XΓ→XΓ is continuous and one may consider
dynamical system (XΓ,σφ).
Generalized shifts has been introduced for the first time in [2], moreover
their dynamical properties have been studied in several texts, like
[3] and [7].
Convention 2.3**.**
Suppose that X is a finite discrete topological space
with at least two elements, Γ is a nonempty set, and φ:Γ→Γ
is an arbitrary map. For H⊆Γ let:
[TABLE]
so
U:={D⊆XΓ×XΓ: there exists a finite subset
H of Γ with αH⊆D}
is the unique compatible uniform structure on XΓ
(which is equipped with product topology).
Note that, the compact Hausdorff topological space XΓ is metrizable if and only if
Γ is countable.
Alexandroff compactification and Fort spaces
For a topological
space Y choose a point b∈/Y and consider the set A(Y):=Y∪{b} with the topology
{U⊆Y:U is an open subset of Y}∪{V⊆A(Y):Y∖V
is a closed compact subset of Y}, then
we call A(Y) the Alexandroff compactification or one point compactification of Y [9, 10].
Obviously one may study a dynamical system
with Alexandroff compactification of a topological space as phase
space. Now suppose b∈F and consider F with the topology:
[TABLE]
then we say that F is a Fort space (with particular point b) [10, Counterexample 24].
It’s evident that
the class of Fort spaces is just the class of Alexandroff compactification of discrete spaces.
Convention 2.4**.**
From now on, consider F is a Fort space with the particular point b and
h:F→F is continuous. For H⊆F
let:
[TABLE]
so
K:={D⊆F×F: there exists a finite subset
H of F∖{b} with γH⊆D}
is the unique compatible uniform structure on F.
Note that, the compact Hausdorff topological space F is metrizable if and only if
F is countable.
Remark 2.5**.**
In Fort spaces Y1 with particular point b1 and Y2 with particular point b2,
f:Y1→Y2 is continuous if and only if one of the following conditions holds true [1, Lemma 5.1]:
f(b1)=b2 and f−1(y) is finite, for all y∈Y2∖{b2},
f(b1)=b2 and Y1∖f−1(f(b1)) is finite.
3. Weak specification property
In this section we show that (XΓ,σφ) has weak specification property
(almost weak specification property) if and only if
φ:Γ→Γ does not have any periodic point.
Moreover (XΓ,σφ) has specification property,
if and only if φ:Γ→Γ is one–to–one without any periodic point.
On the other hand (F,h) has weak specification property
(almost weak specification property) if and only if
⋂{hn(F):n≥1} is singleton. Finally, (F,h) has specification property
if and only if F is singleton.
Lemma 3.1**.**
If φ:Γ→Γ has a periodic point, then the dynamical system
(XΓ,σφ) does not have almost weak specification property.
Proof.
Suppose that λ is a periodic point of Γ, then there exists m≥1 with
φm(λ)=λ. Choose distinct p,q∈X and consider α:=α{λ}∈U.
If (XΓ,σφ) has
almost weak specification property, then there exists
Nα:Z+→Z+ such that for all 0≤l1≤k1<l2≤k2
with l2−k1≥Nα(k2−l2) there exists
x∈XΓ with the property:
[TABLE]
for y1=(p)θ∈Γ and y2=(q)θ∈Γ.
In particular for l1=k1=1,l2=Nα(m)+2,k2=Nα(m)+2+m
there exists (xθ)θ∈Γ such that:
[TABLE]
and
[TABLE]
which imply that xφ(λ)=p and xφi(λ)=q
for all i=Nα(m)+2,…,Nα(m)+2+m.
Choose j∈{Nα(m)+2,…,Nα(m)+2+m} such that there exists n≥1
with j=nm+1, thus φj(λ)=φ(λ) and
q=xφj(λ)=xφ(λ)=p which is a contradiction with
p=q. Therefore (XΓ,σφ)
does not have almost weak specification property.
∎
Note 3.2**.**
For a map φ:Γ→Γ and α,β∈Γ
we say α∼φβ if there exists i,j≥0
with φi(α)=φj(β). Then ∼φ is an equivalence relation
on Γ.
Lemma 3.3**.**
If φ:Γ→Γ does not have any periodic point, then the dynamical system
(XΓ,σφ) has weak specification property.
Proof.
Suppose φ:Γ→Γ does not have any periodic. For α∈U
there exists a finite subset F of Γ with αF⊆α. Also, there exist
β1,…,βm∈Γ and N≥1 such that
F⊆⋃{φ−i(βj):j=1,…,m,i=0,…,N} and
for all distinct s,t∈{1,…,m},
βs∼φβt. Now consider x1=(xθ1)θ∈Γ,…,xk=(xθk)θ∈Γ∈XΓ and
0≤i1≤j1<i2≤j2<⋯<ik≤jk with is+1−js≥N+1
for all s∈{1,…,k−1}. Choose p∈X and define
z=(zθ)θ∈Γ∈XΓ in the following way:
[TABLE]
First of all note that zθs are well-defined, otherwise there exist γ1,γ2∈F,
s1<s2, and t1<t2 with is1≤t1≤js1<is2≤t2≤js2
with
φt1(γ1)=φt2(γ2),
thus γ1∼φγ2 and there exists i∈{1,…,m}
and r1,r2∈{0,…,N} with φr1(γ1)=φr2(γ2)=βi, so by is2−js1≥N+1,
t2>N and φt1(γ1)=φt2(γ2)=φt2−r2(βi)=φt2−r2+r1(γ1). By t2−r2+r1≥t2−N≥is2−N>js1≥t1, we have
t2−r2+r1>t1 and φt1(γ1) is a periodic point of φ,
which is a contradiction, so zθs are well-defined.
It is easy to see that for all s∈{1,…,k}, γ∈F and
is≤t≤js we have xφt(γ)s=zφt(γ), i.e.
(σφt(z),σφt(xs))∈αF⊆α,
which completes the proof.
∎
Theorem 3.4**.**
The following statements are equivalent:
(XΓ,σφ) has weak specification property,
(XΓ,σφ) has almost weak specification property,
φ:Γ→Γ does not have any periodic point.
Proof.
Use Lemmas 3.1 and 3.3.
∎
Corollary 3.5**.**
The following statements are equivalent:
(XΓ,σφ) has specification property,
φ:Γ→Γ is one–to–one without any periodic point.
Proof.
“(1) ⇒ (2)” Suppose (XΓ,σφ)
has specification property, then for all x∈XΓ
and open neighbourhood U of x there exists α∈U with
α[x]⊆U. Since
(XΓ,σφ)
has specification property, there exists a periodic point z of σφ with
(x,z)∈α, i.e. z∈α[x]⊆U and the collection of all
periodic points of σφ is dense in XΓ. By [3, Theorem 2.6]
φ:Γ→Γ is one–to–one and using
Lemma 3.1 φ:Γ→Γ does not have
any periodic point.
“(2) ⇒ (1)” Suppose φ:Γ→Γ is one–to–one
without any periodic point. By using Theorem 3.4, we get that
(XΓ,σφ) has weak specification property. Consider
α∈U, there exists β∈U with
β−1∘β⊆α, moreover since
(XΓ,σφ) has weak specification property
there exists N≥1
such that for all y1,…,yn∈XΓ (n≥2) and
0≤l1≤k1<l2≤k2<…<ln≤kn with
li+1−ki≥N
(for all i=1,…,n−1) there exists x∈XΓ
such that
[TABLE]
Since σφ:XΓ→XΓ is uniformly continuous,
there exists μ∈U with:
[TABLE]
Since φ:Γ→Γ is one–to–one, the collection of all
periodic points of σφ is dense in XΓ by [3, Theorem 2.6].
Hence
there exists a periodic point z of σφ with (x,z)∈μ, thus
(σφi(x),σφi(z))∈β for all i∈{0,1,…,kn}.
Therefore (σφi(z),σφi(yj))∈β−1∘β⊆α for all j∈{1,…,n}
and i∈{lj,lj+1,…,kj},
which completes the proof.
∎
Theorem 3.6**.**
In the dynamical system (F,h) the following statements are equivalent:
the dynamical system (F,h) has weak specification property,
the dynamical system (F,h) has almost weak specification property,
⋂{hn(F):n≥1} is singleton.
Proof.
It’s evident that (a) implies (b).
(b) ⇒ (c): Suppose (F,h) has almost weak specification property. Note that
⋂{hn(F):n≥1}=∅ since F is a nonempty compact Hausdorff and
h:F→F is continuous. If ⋂{hn(F):n≥1} is not singleton, then there exist distinct points
z,y∈⋂{hn(F):n≥1}. We may suppose z=b.
There exists Nγ{z}:Z+→Z+ such that n→∞limnNγ{z}(n)=0 and for all y1,…,yn∈F and 0≤l1≤k1<l2≤k2<…<ln≤kn with
li+1−ki≥Nγ{z}(ki+1−li+1) (for all i=1,…,n−1) there exists x∈Z
such that
[TABLE]
Let:
[TABLE]
Choose w∈h−(l2+1)(z), hence there exists x1,x2∈F such that:
[TABLE]
and:
[TABLE]
By (3.1), x1=z=hl2(x1), thus z=hl2(z).
Considering (3.2)
we have x2=z and therefore
(z,hl2(w))=(hl2(z),hl2(w))=(hl2(x2),hl2(w))∈γ{z},
z=hl2(w), which leads to h(z)=hl2+1(w)=z.
Now for y∈⋂{hn(F):n≥1}∖{z} and choose v∈h−l2(y),
there exists x3∈F
such that:
[TABLE]
thus x3=z and (z,y)=(hl2(z),y)=(hl2(x3),hl2(v))∈γ{z}
which shows that y=z. Therefore ⋂{hn(F):n≥1}={z} which is in contradiction
with y=z. Thus ⋂{hn(F):n≥1} is singleton.
(c) ⇒ (a): Suppose ⋂{hn(F):n≥1} is singleton:
Case I: ⋂{hn(F):n≥1}={b}. Let α∈K. There exists finite
subset A of F∖{b} with γA⊆α. For all
y∈A there exists my≥1 with y∈/hmy(F), thus h−my(y)=∅.
Let m=y∈AΣmy, then h−m(A)=∅.
So for all n≥m , hn(F)∩A=∅. Let Nα=m, then
for all
y1,…,yn∈F and 0≤l1≤k1<l2≤k2<…<ln≤kn with
li+1−ki≥m (for all i=1,…,n−1),
m≤l2. Thus for all i≥l2(≥m) and j≥2,
hi(y1),hi(yj)∈/A, so (hi(y1),hi(yj))∈γA⊆α.
On the other hand for 0≤i≤k1, (hi(y1),hi(y1))∈γA⊆α.
Hence
[TABLE]
which completes the proof.
Case II: ⋂{hn(F):n≥1}={c} and c=b. In this case h(b)=b
and h(F) is finite, so by ⋂{hn(F):n≥1}={c}, there exists m≥1 such that:
[TABLE]
Now for all
y1,…,yn∈F and 0≤l1≤k1<l2≤k2<…<ln≤kn with
li+1−ki≥m (for all i=1,…,n−1), l2≥m
and hi(yj)=hi(y1) for all i∈{lj,…,kj} and j∈{1,…,n}.
Thus (F,h) has weak specification property.
∎
Theorem 3.7**.**
The dynamical system (F,h) has specification property,
if and only if F={b}.
Proof.
It’s clear that for F={b}, (F,h) has specification property.
Conversely, suppose (F,h) has specification property, then it has weak specification property.
By Theorem 3.6, ⋂{hn(F):n≥1} is singleton. For
z∈F∖{b} there exists a periodic point x∈F such that for
l1=0, (x,z)=(hl1(x),hl1(z))∈γ{z} so z=x
and z is a periodic point of h. Thus
[TABLE]
hence F∖{b} has at most one element.
Suppose that F={x,b}. We may consider the following cases, for x=b:
Case I: ⋂{hn(F):n≥1}={x}={b}. In this case h(x)=h(b)=x. So
Per(f)={x}, thus for l1=0 , (x,b)=(hl1(x),hl1(b))∈γ{x}
which leads to the contradiction x=b, hence this case does not occur.
Case II: ⋂{hn(F):n≥1}={b}={x}. In this case we have the contradiction
x∈F∖{b}⊆Per(h)⊆⋂{hn(F):n≥1}={b}
hence this case does not occur too.
Considering the above cases, we get x=b and F={b}.
∎
4. Stroboscopical property
In this section we show that (XΓ,σφ) has uniform stroboscopical property,
(stroboscopical property) if and only if φ:Γ→Γ is one–to–one. Also
(F,h) has uniform stroboscopical property
(stroboscopical property) if and only if all points of F are periodic points of h.
Lemma 4.1**.**
If (XΓ,σφ) has stroboscopical property, then
φ:Γ→Γ is one–to–one.
Proof.
Suppose φ:Γ→Γ is not one–to–one, then there are distinct points
β,λ∈Γ such that φ(β)=φ(λ).
Choose distinct p,q∈X.
Consider z=(zα)α∈Γ∈XΓ with:
[TABLE]
then for all (xα)α∈Γ∈XΓ and n≥1
, xφn(β)=xφn(λ). Thus there is not any sequence
{ni}i≥0 in N with i→∞limσφni((xα)α∈Γ)=z. Therefore
(XΓ,σφ) does not have stroboscopical property.
∎
Lemma 4.2**.**
If A={mi1}i≥0 is a strictly increasing sequence in N, then:
there exists a map f:N→N, and A has a subsequence
{ni}i≥0
such that for all m≥1 and i≥m, ni≡f(m)(modm)
and f(m)≤m;
A has a subsequence
{mi}i≥0 such that mi+1−mi>2i for all i≥0.
Proof.
1.
Suppose A={mi1}i≥0=:A1 and k1=1, then there exists k2∈{1,2}
and A has a subsequence
A2={mi2}i≥0 such that for all i≥0, mi2≡k2(mod2).
For s≥2, suppose that we have chosen subsequences A1={mi1}i≥0,…,As={mis}i≥0 and natural numbers k1,…,ks. Then there exists
ks+1∈{1,…,s+1},
and As has a subsequence
As+1={mis+1}i≥0 such that for all i≥0,
mis+1≡ks+1(mods+1). Let f:N→N
with f(i)=ki (i≥1) and subsequence {ni}i≥0 of A with
n0=m01 and ni=mii for i≥1, then the map f:N→N
and subsequence {ni}i≥0 of A satisfies (1).
2. We construct {mi}i≥0 inductively. Let m0:=m01, for
i≥0 suppose we have chosen mi=mni1 let mi+1:=mni+2i+11.
The the subsequence {mi}i≥0 of A satisfies (2).
∎
Lemma 4.3**.**
If all points of Γ are periodic points of φ:Γ→Γ,
then (XΓ,σφ) has uniform stroboscopical property.
Proof.
Let A be a strictly increasing sequence in N.
By Lemma 4.2 there exists a map f:N→N
and A has a subsequence
{ni}i≥0
such that for all m≥1 and i≥m, ni≡f(m)(modm)
and f(m)≤m. For all
α∈Γ let kα=min{n≥1:φn(α)=α}.
For z=(zα)α∈Γ∈XΓ define z∗=(zα∗)α∈Γ∈XΓ
with:
[TABLE]
Then for all
α∈Γ and i≥f(kα), kα−f(kα)+ni≡0(modkα), so
[TABLE]
For D∈U there exists finite subset H={β1,…,βs} of Γ with αH⊆D.
For all i≥max{f(kβ1),…,f(kβm)} and for all z=(zα)α∈Γ∈XΓ
we have (z,σφni(z∗))∈αH⊆D.
Thus for z↦z∗ϱ:XΓ→XΓ the sequence
{σφni∘ϱ}i≥1 converges uniformly to idXΓ.
∎
Remark 4.4**.**
If φ:Γ→Γ is one–to–one, then each D∈∼φΓ(={∼φα:α∈Γ}) satisfies exactly one of the
following conditions:
D has finite elements like m and for all α∈D, D={φi(α):1≤i≤m},
D is infinite and there exists α∈Γ with D={φn(α):n≥0},
D is infinite and we may suppose that D={βn:n∈Z} with φ(βn)=βn+1 for all n∈Z.
Lemma 4.5**.**
If φ:Γ→Γ is one–to–one and does not have any periodic point,
then (XΓ,σφ) has uniform stroboscopical property.
Proof.
Suppose φ:Γ→Γ is a one–to–one map without any periodic point.
Using axiom of choice there exists a subset of Γ like Λ such that
⋃{∼φα:α∈Λ}=Γ and for all
distinct α,β∈Λ, ∼φα∩∼φβ=∅, also we may suppose each α∈Λ
provides exactly one of the following conditions (use Remark 4.4 too):
∼φα={φn(α):n≥0},
∀n≥0∃β∈Γ(φn(β))=α).
Let
[TABLE]
and
[TABLE]
Moreover for all α∈Γ, choose
λα∈Λ∩∼φα.
Suppose A is a strictly increasing sequence in N.
By Lemma 4.2, A has a subsequence
like {ni}i≥0 such that
ni+1−ni>2i for all i≥0. Consider p∈X and for
z=(zα)α∈Γ∈XΓ define z∗=(zα∗)α∈Γ∈XΓ with:
[TABLE]
Note that using 0<n1<n2<n3<⋯, for k≥n1 there exists unique i≥1 and j∈{0,…,ni+1−ni−1}
with k=ni+j thus for μ∈Λ1 and
α∈{φn(μ):n≥n1}, zα∗ is well-defined.
Moreover for μ∈Λ2 if there exist
i1,i2≥1, j1∈{−(i1−1),…,i1−1} and j2∈{−(i2−1),…,i2−1} with
φni1+j1(μ)=φni2+j2(μ) we have ni1+j1=ni2+j2.
If i1=i2 we may suppose i1<i2 thus 2(i2−1)<ni2−ni2−1≤ni2−ni1=j1−j2≤i1−1+i2−1
which leads to contradiction i2<i1, thus i2=i1 and j2=j1. Therefore zα∗s are
well-defined. We have:
[TABLE]
since for μ∈Λ1, j≥0 and i≥j+2 the relation λφni+j(μ)=μ
and inequalities 0≤j<2(j+2)≤2i<ni+1−ni lead to
zφni+j(μ)∗=zφj(μ).
Also
[TABLE]
For D∈U there exists finite subset H={β1,…,βs} of Γ with αH⊆D.
There exists N≥1, finite subset H1 of Λ1 and finite subset H2 of Λ2 with
H⊆⋃{φt(H1∪H2):∣t∣≤N}(=(⋃{φt(H1):0≤t≤N})∪(⋃{φt(H2):−t≤t≤N})).
Using (i) and (ii) for all z=(zα)α∈Γ∈XΓ we have:
[TABLE]
thus (z,σφni(z∗))∈αH⊆D for all z=(zα)α∈Γ∈XΓ
and i≥N+2.
Hence for z↦z∗ϱ:XΓ→XΓ the sequence
{σφni∘ϱ}i≥1 converges uniformly to idXΓ.
∎
Theorem 4.6**.**
The dynamical system
(XΓ,σφ) has uniform stroboscopical property if and only if
φ:Γ→Γ is one-to-one.
Proof.
If (XΓ,σφ) has uniform stroboscopical property, then it has stroboscopical property and by Lemma 4.1
the map φ:Γ→Γ is one–to–one.
Now suppose φ:Γ→Γ is one–to–one. If either all points
of Γ are periodic points of φ or φ does not have any periodic
point, then we are done by Lemmas 4.3 and 4.5. Otherwise
Per(φ) (the collection of all periodic points of φ) and
Γ∖Per(φ) are two nonempty subsets of Γ.
By Lemmas 4.3 and 4.5 both dynamical systems
(XPer(φ),σφ↾Per(φ)) and
(XΓ∖Per(φ),σφ↾Γ∖Per(φ)) have
uniform stroboscopical property. In order to complete the proof use the fact that if both
dynamical systems (Z,f) and (Y,h) have uniform stroboscopical property, then
(Z×Y,f×h) (where (f×h)(u,v)=(f(u),h(v)) for (u,v)∈Z×Y)
has uniform stroboscopical property.
∎
Note 4.7**.**
Using Lemmas 4.1 and Theorem 4.6,
for finite discrete topological space X with at least two elements,
nonempty set Γ, and arbitrary map φ:Γ→Γ the following
statements are equivalent:
(XΓ,σφ) has uniform stroboscopical property,
(XΓ,σφ) has stroboscopical property,
φ:Γ→Γ is one–to–one.
Note 4.8**.**
For countable Γ, by [8, Proposition 5] and [3],
(XΓ,σφ) has the strong stroboscopical property
if and only if φ:Γ→Γ is one–to–one without periodic points.
Theorem 4.9**.**
The following statements are equivalent:
(F,h) has uniform stroboscopical property,
(F,h) has stroboscopical property,
Per(h)=F.
Proof.
(b) ⇒ (c).
Suppose (F,h) has stroboscopical property and z is an isolated point of F,
then there exists x∈F and {n}n≥0 has a subsequence like {nk}k≥0 such that
k→∞limhnk(x)=z, hence there exists N≥1 such that:
[TABLE]
in particular hnN(x)=z=hnN+1(x), thus hnN+1−nN(z)=z and z∈Per(h).
On the other hand, if z is limit point of F, then F is infinite and z=b. Since
F∖{b}⊆Per(h), h↾F∖{b}:F∖{b}→F
is one-to-one which leads to h(b)=b by Remark 2.5.
(c) ⇒ (a).
Suppose Per(h)=F and A is an arbitrary
increasing sequence in N. The subsequences A1,A2,… of
of A defined inductively as follows:
let A1:=A={nk1}k≥0
and r1=0,
suppose for
t≥1, At={nkt}k≥0 is a subsequence of A and rt∈{0,…,t−1} such that
for all k≥0, nkt≡modtrt;
then there exists rt+1∈{0,…,t} and subsequence
At+1={nkt+1}k≥0 of At such nkt+1≡modt+1rt+1.
Then B:={nkk}k≥1 is a subsequence of A with
[TABLE]
For z∈F let mz:=min{m≥1:hm(z)=z}. Consider
ϱ:F→F with ϱ(z)=hmz−rmz(z) (z∈F). Then for all
z∈Z and k≥mz, hnkk(ϱ(z))=z. For α∈K
there exists a finite subset A of F∖{b} with γA⊆α.
Let N=max({mz:z∈A}∪{mb}), for all k≥N and z∈F.
mz≤N: in this case hnkk(ϱ(z))=z, and (hnkk(ϱ(z)),z)=(z,z)∈α.
mz>N: note that for all i≥0, mz=mhi(z), thus for all
n≥N we have mhnkk(ϱ(z))=mhnkk+mz−rmz(z)=mz>N
therefore z,hnkk(ϱ(z))∈/A and (hnkk(ϱ(z)),z)∈γA⊆α.
Regarding the above two cases we have (hnkk(ϱ(z)),z)=(hnkk(ϱ(z)),idF(z))∈α for all k≥N. Thus {hnkk∘ϱ}k≥1 converges uniformly
to idF:F→F and (F,h) has uniform stroboscopical property.
∎
Theorem 4.10**.**
The dynamical system (F,h) has strongly stroboscopical property if and only if F={b}.
Proof.
Suppose (F,h) has strongly stroboscopical property, if F={b}, then F has at least two
(distinct) isolated points like x,y. There exists m≥1 with hm(x)=x, by
Theorem 4.9, since (F,h) has strongly stroboscopical property and x
is an isolated point of F, y∈ωh({mn}n≥0,x)={x} which is
in contradiction with y=x, thus F={b}.
∎
5. Two diagrams
Let’s recall that inthe paper, X is a finite discrete space with at least two
elements, Γ is nonempty, φ:Γ→Γ is an arbitrary map, F
is a Fort space with particular point b, and h:F→F is continuous. So according to the previous
sections, we get the following table:
[TABLE]
Table A
Where the dynamical system (Z,f) has ρ property if and only if it has the phrase
occurs in the corresponding case.
Using Table A, we have the following diagrams:
(XΓ,σφ)has (almost) weak specification property(XΓ,σφ)has (uniform) stroboscopical property(C3)(C1)(C2)(XΓ,σφ)has specification property(strongly stroboscopical property)
Where (Ci) denotes the counterexample (XZ,σφi) for:
φ1:Z→Z with φ1(n)=n2+1 (n∈Z),
φ2:Z→Z with φ2(n)=−n (n∈Z),
φ3:Z→Z with φ3(n)=n+1 (n∈Z).
And:
(F,h)has (almost) weak specification property(F,h)has (uniform) stroboscopical property(F,h)has specification property(strongly stroboscopical property)F={b}(D1)(D2)(D3)
Where (Di) denotes the counterexample ({n±1:n∈Z∖{0}}∪{0},hi) for (consider {n±1:n∈Z∖{0}}∪{0} with induced topology from Euclidean line R):
[TABLE]