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Abstract
A symmetric Lorenz map is obtained by ‘flipping’ one of the two branches of a symmetric unimodal map. We use this to derive a Sharkovsky-like theorem for symmetric Lorenz maps, and also to find cases where the unimodal map restricted to the critical omega-limit set is conjugate to a Sturmian shift. This has connections with properties of unimodal inverse limit spaces embedded as attractors of some planar homeomorphisms.
MATHEMATICS SUBJECT CLASSIFICATIONS 2010:
1. Introduction
Topological properties of a continuous dynamical system are, in general, easier to understand than those of discontinuous systems. For example, for continuous functions of the real line there is the celebrated Sharkovsky Theorem [Citation29], which says that if the map has a periodic point of prime period n, it also has a periodic point of prime period m for every in the Sharkovsky order
However, in general there is no analogue of the Sharkovsky theorem for discontinuous functions of the reals.
In this paper we study Lorenz maps, which are piecewise monotone interval maps with a single discontinuity point. Such Lorenz maps appear as Poincaré maps of geometric models of Lorenz attractors described independently by Guckenheimer [Citation20], Williams [Citation30] and Afraimovich, Bykov and Shil'nikov [Citation1]. For the class of ‘old’ maps (discontinuous degree one interval maps) which also include Lorenz maps, a characterization of periodic orbit forcing was given by Alsedá, Llibre, Misurewicz and Tresser in [Citation3]. Hofbauer in [Citation22] obtained a result similar as in [Citation3] using an oriented graph with infinitely many vertices whose closed paths represent the periodic orbits of the map except that he did not characterize completely the set of periodic points. The increasing Lorenz maps ϕ were studied earlier by Rand in [Citation28], where he noticed, based on observations from [Citation23], that periods follow Sharkovsky's order. In particular, [Citation28, Theorem 4] is an analogue of our Theorem 3.1. In [Citation2] the connection between β-expansions and Sharkovsky's orderi is given. Recently, Cosper [Citation18] proved a direct analogue of Sharkovsky's Theorem in special families of piecewise monotone maps (a truncated tent map family).
In the present paper we combine some old and more recent results on the relation between unimodal and Lorenz maps, including a version of Sharkovsky's Theorem. The basic idea is to explore the relation between a unimodal map f and symmetric Lorenz maps ϕ and ψ obtained by ‘flipping the right branch’ and ‘flipping the left branch’ of the graph of f respectively, see Figure .
For increasing Lorenz maps ϕ we prove in Theorem 3.1 that Sharkovsky's Theorem holds with the exception of the fixed points, and for decreasing Lorenz maps ψ we prove in Theorem 3.2 that Sharkovsky's Theorem holds possibly except for periods .
We can turn ϕ into a proper circle endomorphism (with unique rotation number independent of ) by setting (see also Figure ):
In Proposition 5.1 we calculate the rotation number of the family of such maps, and prove that in the irrational rotation number case the restriction to omega limit set is a minimal homeomorphism. We use techniques developed primarily for unimodal interval maps.
Next, we also give an implementation of Sturmian shifts in interval maps. For every Sturmian shift we assign a unimodal map (basically a kneading sequence) so that the unimodal map restricted to its omega limit set is conjugate to that Sturmian shift.
Maps , besides being interesting on their own, prove also to be very useful in surface dynamics. Namely, knowledge of their dynamics can be related to special orientation preserving planar embeddings of inverse limit spaces with bonding maps being f. In the last section of the paper we connect the map
to the study of unimodal inverse limit spaces represented as attractors of some planar homeomorphisms (this was initially done in [Citation9] using a map conjugated to
). In Theorem 6.1 we give a compete characterization of accessible points of tent inverse limit spaces embedded in such a way. Then Corollary 6.1 gives a partial answer to Problem 1 in [Citation4] by giving an example of tent inverse limit space which has uncountably many inhomogeneities with only countably infinitely many of them not being endpoints.
2. Preliminaries
Let be the unit interval, and
a symmetric unimodal map, i.e. given the involution
, we assume that
for every x. This means that the critical point
, and by an appropriate scaling, we can assume that
. For example,
with
is the logistic family in this scaling.
We can turn f into an (increasing) symmetric Lorenz map by flipping the right half of the graph vertically around
, see Figure , giving the following result:
The choice
is arbitrary, only made to be definite.
Then, ϕ is semi-conjugate to f: . In fact
(1)
(1) We can also flip the left branch of f and obtain
which is called a decreasing symmetric Lorenz map. Then
for all x, and by induction
Suppose then
is continuous at x. Then (Equation1
(1)
(1) ) implies that
and
otherwise.
3. Sharkovsky's Theorem for Lorenz maps
We can describe the dynamics of f using the standard symbolic dynamics with the alphabet , where the symbols stand for the sets
and
respectively. It is also enough to restrict the study to the dynamical core
, since points from
will be mapped to the core under f. The kneading invariant
is the itinerary of the point
. Since the itinerary map
is monotone in the parity-lexicographical order on
, the kneading invariant is maximal admissible sequence, i.e.
for all
. Also,
for all
. It can be shown that every itinerary for which every shift is in parity-lexicographical ordering between
and ν can be realized by a point in the dynamical core (see e.g. [Citation25]).
Also, if an m-periodic point y is closest to c from all the points in its orbit, and , then
for all
. As a corollary,
(if admissible) is periodic of period k = m or
, which we prove in the rest of this paragraph. To prove that, assume that there is
such that for
we can write
. Then,since
is maximal among its shifts,
, and thus
is odd. But then
, so
, violating the parity-lexicographical shift-maximality of
.
Lemma 3.1
Let f be a unimodal map with a periodic point x of period n. Then for every there are periodic points y and
of f such that
y has prime period m and
is decreasing at y, and
has prime period m and
is increasing at
or
has prime period m/2 and
is decreasing at
.
If is decreasing at x, then the statement holds for m = n as well.
Proof.
By Sharkovsky's Theorem, f has at least one periodic orbit of period m. Take the m-periodic point y closest to c, so the itinerary is maximal (w.r.t. the party-lexicographical order
) among all admissible m-periodic itineraries. Find
by setting
if
and
. Otherwise we set
. Let us first show that
is admissible. Let
be the smallest integer such that
. If j<m, then both
. If
and
is odd, then
. The remaining case is
is even and
.
Assume that m = j. Thus . To show that
is admissible, assume that
. Since
is odd, we have
, which contradicts shift-maximality of ν. Thus,
is admissible in this case. Also,
cannot be periodic of period m/2 since
has an odd number of ones. It follows that
, which contradicts the assumption that e is the closest to ν among m-periodic itineraries, so this case is not possible.
Assume that m<j. Then but since the first symbol at which
and
differ is j−m, the parity argument and m-periodicity of e imply that
, which contradicts the shift-maximality of ν. So this case cannot occur either.
We conclude that , and since it is shift-maximal,
for every
. We still have to argue that
for every
. Assume there is
such that
and take the smallest such n. Since
starts with 1, and thus n>0. Also, since n is the smallest such integer,
. Then
implies that
, which is a contradiction. We conclude that
is admissible, i.e. realized by a point
in
.
Moreover, we also conclude that is decreasing in y and increasing in
. From the discussion preceding the statement of the lemma, we conclude that the prime period of
is m or m/2.
If has prime period
, then
and
. Since
, we conclude that
is odd, from which is follows that
is decreasing in
.
For discontinuous interval maps, there are previous results regarding the forcing relation between periods, see e.g. [Citation3] which however do not give the following result.
Theorem 3.1
Symmetric increasing Lorenz maps ϕ satisfy Sharkovsky's Theorem, except for the fixed points.
Proof.
We start the proof for the symmetric Lorenz map ϕ with two claims.
We first show that if ϕ has a periodic point of prime period
, then f also has a periodic point of prime period n, unless, possibly, n is a power of 2, and then f has a periodic point of prime period n or
.
Let
and assume
for all k<n. Then the same holds for
. At exactly one of x and
, say at
is increasing, so
. Assume k<n is such that
and take the smallest such (so that x has prime period k). If k is not a power of two, then, since k divides n, Sharkovsky's Theorem gives the existence of a periodic point of prime period n as well. So we only have to consider the case that
.
If
is increasing at x, then
, a contradiction. Thus
must be decreasing at x. In that case
is increasing at x, and thus
, from which we conclude that
and x is a periodic point of f of prime period
.
Next we show that if m>1 is such that f has an m-periodic point, then there exists an m-periodic point of ϕ. Assume
and
for all k<m. If
is increasing at x, then
. Assume that there is k<m such that
. Then
must be decreasing at x, and we get
, thus m = 2k. Now
, so
, but on the other hand
, which gives a contradiction.
The remaining case is when
is decreasing at x. By Lemma 3.1 and its proof, we find a point
such that
and
is increasing at
. If m is indeed the prime period of
, then we can use the above argument to conclude that
is m-periodic point of ϕ. Otherwise, the prime period of
is m/2 and
is decreasing in
. But then
and
, so
is periodic for ϕ with prime period m.
However, if m = 1, then
and
lies in general outside the core (and in fact outside I), so it is lost in the construction of ϕ. Indeed, ϕ has a fixed point only if it comes from a ‘full’ unimodal map f (i.e. a unimodal map that exhibits all possible itineraries of points, such as e.g. the quadratic Chebyshev polynomial
).
To finish the proof, assume that ϕ has an n-periodic point. By the first part of the proof, there exists an n-periodic point for f (or possibly an n/2-periodic point if n is a power of 2). Sharkovsky's Theorem implies that f has an m-periodic point for every . The second part of the proof implies that there exists an m-periodic point of ϕ provided
.
There are maps f with periodic points of period and no other periods. If r is maximal with this property, we say that f is of type
. If f has periodic points of all periods of the form
we say that f is of type
. The union of these two is called type
. If x is a
-periodic point of a unimodal map f of type
, then we say that x has the pattern from the first period doubling cascade; itinerary of such point is the (shift of the)
-periodic continuation of the Feigenbaum itinerary
which equals
(2)
(2) where the dots indicate the powers of 2.
Studying the decreasing symmetric Lorenz maps ψ we can obtain a theorem similar to Theorem 3.1.
Theorem 3.2
Decreasing symmetric Lorenz maps ψ satisfy Sharkovsky's Theorem, possibly except for periods .
Proof.
The proof for a decreasing symmetric Lorenz map ψ is similar as for increasing Lorenz maps. We only need to repeat the two claims.
Let
and assume
for all k<n. Then the same holds for
. For even n the proof is the same as for ϕ in Theorem 3.1, so assume that n is odd. At exactly one of x and
, say at
is decreasing, so
. Assume k is a divisor of n is such that
. Then k and n/k are odd and
is decreasing as well, so
, which is a contradiction.
Assume that f has a n-periodic point and take
. (We note that the claim does not hold for m = n. Indeed, if n = m = 3 and the 3-periodic point is emerging in a saddle node bifurcation, then ψ does not yet have a 3-periodic point.) By Lemma 3.1, f has periodic points x of prime period m, and if m is not a power of two, then we can take x orientation preserving as well as orientation reversing. Assume that
for all proper divisors k of m.
If m is odd, we take x orientation reversing, so that
. Suppose that j is a proper divisor of m such that
. Then
because
by assumption. Also,
so we also conclude that
. But then
, a contradiction. Therefore m is the prime period of x for ψ.
If m is even, we take x orientation preserving, so that
. Analogously as above we prove that m is the prime period of x for ψ.
This shows that ψ satisfies Sharkovsky's Theorem with the potential exception of periodic points in the first period doubling cascade. For instance, if with
(where
is the Feigenbaum parameter, then ψ does not have a point of prime period 2, despite the fact that it has periods
. More generally, if
is r−1 renormalizable of period 2 (so in contrast with Theorem 3.1 the final renormalization has period
), then ψ has no periodic point of period
. The map ψ always has a fixed point, so we don't need to make exceptions for fixed points.
4. Cutting times
We recall some notation from Hofbauer towers and kneading maps that we use later in the paper; for more information on these topics, see e.g. [Citation11, Chapter 6].
Recall that c denotes the critical point 1/2. For denote by
. We assume that
(otherwise the dynamics of f is trivial).
Define inductively , and
We say that n is a cutting time if
. The cutting times are denoted by
(where
and
). They were introduced in the late 1970s by Hofbauer [Citation21]. The difference between consecutive cutting times is again a cutting time (see e.g. Subsection 6.1 in [Citation11]), so we can define the kneading map
as
We call f long-branched if
, which is equivalent to
and also to
.
A purely symbolic way of obtaining the cutting times is the following. Recall that we use the itinerary map for f (and also for ϕ) with codes 0 for
and 1 for
. We will use the modified kneading sequence
, where we traditionally omit the zero-th symbol. Note that if c is not periodic,
and the modification is only made so that the itineraries do not contain symbol
(we take the smaller of the two sequences in parity-lexicographical ordering).
We can split any sequence into maximal pieces (up to the last symbol) that coincide with a prefix of ν. To this end, define
(3)
(3) That is, the function ρ depends on e and ν, but we will suppress this dependence. When we apply this for
, we obtain
or in other words
for
and
.
Define the closest precritical points as any point such that
for some
and
for all
and
. By symmetry, if ζ is a closest precritical point,
is also a closest precritical point. If
is a closest precritical point of the lowest
, then the itineraries of
and
coincide for exactly
entries, and differ at entry
. Hence
is a cutting time, say
for some
. We use the notation
if
. That is
(4)
(4) and
(5)
(5)
Applying this to , we obtain that
is a cutting time.
In particular,
(6)
(6) see Figure , and the larger
, the closer
is to c.
Let . Then we can define the co-cutting times as
The cutting and co-cutting times are always disjoint sequences (see [Citation13, Lemma 2]), and
if f is the full unimodal map (because then
and κ is not defined). Furthermore, there is a co-kneading map
such that
Proposition 4.1
Let f be a unimodal map with the kneading map Q. If then
and
is a minimal Cantor set.
Proof.
In [Citation12, Lemma 3.6 and Proposition 3.2] and [Citation13, Lemma 4 and Proposition 2] it was shown that implies
and that c is persistently recurrent. This property was introduced by Blokh and implies minimality of
, see [Citation7] and also [Citation14, Section 3].
In fact, implies that
, but not vice versa. If both
and
, then c is non-recurrent, but as we will see in Section 6, there are maps where
.
5. Sturmian shifts
There are multiple ways of defining Sturmian shifts and we take the one using the symbolic dynamics of circle rotations.
Definition 5.1
Let , be the rotation over an irrational angle α. Let
and build the itinerary
by
(7)
(7) Then u is called a rotational sequence. The minimal (and uniquely ergodic) shift space obtained as
is the Sturmian shift of frequency α, and each
is called a Sturmian sequence.
The purpose of this section is to describe cases when unimodal maps restricted to their critical omega-limit sets are conjugate to Sturmian shift. There are in fact multiple ways of choosing the kneading map Q so that
is Sturmian. The simplest way is by means of the Ostrowski numeration, see [Citation26]. Indeed, let
be some irrational number and let
be the convergent of its continued fraction expansion. Thus
and
. Take
and then cutting times as follows:
It is clear that
in this case, and the
interpolate between the numbers
, see also [Citation16]. However,
is in general not invertible, since c itself and/or other points in the backward orbit of c have two preimages in
, see also [Citation15]. As such
is conjugate to the one-sided Sturmian shift.
However, also when is bounded (in fact also when
) there are examples where
is Sturmian, see [Citation12, Chapter III, 3.6]. Let
be an increasing symmetric Lorenz map as in previous sections. In addition to
, another way of coding orbits of unimodal maps (used by Milnor & Thurston [Citation25], Collet & Eckmann [Citation17] and Derrida et al. [Citation19]) is as follows: set
and for
,
(8)
(8) It follows that
if
and
if
. For the itinerary
of
under the function ϕ this means that
and
In other words,
. This gives
. Also, if
with the first symbol neglected, and defined
, then we recover the cutting times as
. (The co-cutting times can be recovered as
and
.) See the example in the proof of Proposition 5.1.
To each we can assign a rotation number by first assigning a lift
to the Lorenz map ϕ:
Then
and the rotation number is defined as
(9)
(9) Since
if and only if
and
otherwise, we obtain
(10)
(10) Next we turn ϕ into a proper circle endomorphism (with unique rotation number independent of
) by setting:
Also let b>c be such that
, see Figure .
The circle endomorphism obtained from ϕ was already studied in the last section of [Citation12].
Proposition 5.1
Assume that f is a unimodal map with cutting times . Let b>c be such that
, see Figure . Then the rotation number of the corresponding
equals
In the latter case, the kneading map
for all
and if
then
is a minimal homeomorphism.
Proof.
Recall that and assume that there is a minimal integer
such that
. Then
and
is periodic with period n + 1.
Recall that b>c is such that , so
, and
. Therefore
for closest precritical points
, see (Equation4
(4)
(4) ), and
. There are two possibilities:
. In this case
is increasing at 1 and thus
is a cutting time.
. In this case
is decreasing at 1 and again
is a cutting time.
By minimality of for all j<k, and hence the kneading sequence ν of f consists of blocks 0 or 11. For example:
where dots indicate cutting times and the bold symbol the position
. Since n + 1 is the period of
, this shows that
, and in view of (Equation10
(10)
(10) ) we have
.
If there is no such minimal n, i.e. for all
, then
for all
(and in particular
) for all
. A counting argument similar to the above shows that
. It is possible that α is rational, e.g. for the logistic map
with a = 3.5097. In this case,
and
converges to an attracting orbit of period 3. Also for the tent map
with
, the critical orbit
has period three and avoids
.
If , then
is the Cantor set, disjoint from
and minimal w.r.t. the action of
. Under the semi-conjugacy f between f and ϕ (indeed
), this projects to a minimal map
. We will show that
is in fact a homeomorphism, from which it follows that
is also a homeomorphism. Assume by contradiction that
are points in
such that
. Then, since f is the semi-conjugacy between ϕ and f, we must have
for every
. Note that
for every
, and thus
, unless
, and thus
. Since c is not periodic, there exists
such that
for all
, and thus
has two f-preimages in
. Since
is minimal, for every
there exists infinitely many
which are ϵ-close to
. For sufficiently small ϵ, an f-preimage of a point ϵ-close to
will be contained in
. Since every point in
eventually has both f-preimages in
, we conclude that
, which is a contradiction.
We argued so far that there exist stunted Lorenz maps for which is a Cantor set with dynamics similar to circle rotations (in fact to Denjoy circle maps) with irrational rotation number, and that there are also unimodal maps with kneading map bounded by 1, such that
is semi-conjugate to a circle rotation, and in fact, the rotation number is
. Therefore
represents a Sturmian shift.
In fact, every irrational rotation number (hence every Sturmian shift) can be realized this way, as we can prove by studying this rotation number closer. Indeed, let be the continued fraction expansion of ρ, with convergents
. For the irrational rotation
, the denominators
are the times of closest returns of any point
to itself, and these returns occur alternatingly on the left and on the right. If we assume that
is to the right of x, and set
, then the first iterate k such that
is
and
is to the left of x.
For the map , the closest returns on the left indeed accumulate on c, but the right neighbourhood
is the preimage of the plateau
and no further iterates of c enter that region. Instead, returns on the left accumulate on b.
Translating this back to the unimodal map f with kneading sequence , the closest returns on the left correspond to closest returns at co-cutting times (recall that there are no cutting times
so that
). If
is such a co-cutting time, then (recalling the function ρ from (Equation3
(3)
(3) ) and using the above argument), the Farey convergents
are also the next co-cutting times for
, and in particular,
.
The closest returns on the right correspond to cutting times, but this time accumulate on b, and because
, the itinerary of b is
(11)
(11) Therefore we need to consider the analogous function
, and find that
for
, and in particular,
.
For example, if , so the
s are the Pell numbers
, then we obtain
where dots indicate cutting times and primes co-cutting times. The bold symbols indicate the positions
. In fact, for each i
and therefore c has two limit itineraries
and
, but c has only one preimage in
.
6. Outside maps and unimodal inverse limit spaces
Boyland, de Carvalho and Hall in [Citation9, Section 3] present a different way of creating a circle endomorphism from a unimodal map. They call this the outside map B, and use it to study the inverse limit space of the unimodal map as attractors of sphere homeomorphisms. Starting from a unimodal map such that the second branch is surjective (i.e.
), they double the interval to a circle
, and let B map the second branch onto
by flipping this branch, and then extend the definition of f on
for the unique point
for which
to cover the interval
. The remaining interval
is then mapped to the constant
. That is
see Figure . Let us carry this out for the family of cores of tent maps
,
for all
.
Then the map
(12)
(12) and the outside map
are conjugate with conjugacy
, i.e.
. But the conjugacy reverses orientation, so the rotation numbers are each others opposite, α for
versus
for B.
Outside map B was used in [Citation9] to give a complete description of the prime end and accessible points structure in unimodal inverse limits embedded in the plane as attractors of an orientation-preserving homeomorphism of the plane (or the two-dimensional sphere ).
In the rest of the section we restate some results from [Citation9] and relate them to the established conjugacy between maps B and .
Recall that I denotes the unit interval . The inverse limit space with the bonding map
is a subspace of the Hilbert cube
defined by
Equipped with the product topology, the space
is a continuum, i.e. compact and connected metric space. Define the shift homeomorphism
,
There is a natural way to make
an attractor of an orientation preserving sphere homeomorphism. Such embeddings are called Brown-Barge-Martin embeddings (abbreviated BBM embeddings), see [Citation6] for the original construction, [Citation8] for generalization of the construction to parametrized families and [Citation9] for the construction applied to unimodal inverse limits. As the outcome of the BBM embedding of
, one obtains an orientation-preserving homeomorphism
so that
is topologically conjugate to
and for every
, and
is contained in
.
In [Citation9] the authors study in detail BBM embeddings of inverse limits of unimodal maps satisfying certain (mild) conditions, which are in particular satisfied for the tent map family . For simplicity we state the following results for tent maps only, noting that they can be generalized to a much wider class of unimodal maps.
Fix the slope for the tent map
. Let B be the corresponding outside map. Denote by
. Theorem 4.28 from [Citation9] shows that there is a natural homeomorphism h between
and the circle P of prime ends of
. Then h conjugates the shift homeomorphism
of the outside map to the action of H on P, so that the prime end rotation number of
is equal to the rotation number (as defined in (Equation9
(9)
(9) )) of
, see [Citation9, Lemma 4.30]. Finally, Corollary 4.36 in [Citation9] gives that the prime end rotation number of
is equal to the rotation number of B. Since
and B are conjugate, the results above follow analogously and by Proposition 5.1 we obtain that the prime end rotation number of
equals
.
Proposition 6.1
Let be a tent map with slope
and let
be corresponding stunted Lorenz map with rotation number α. Let
be embedded in
by a BBM construction. Then the prime end rotation number of
on
equals
.
Remark 6.1
In [Citation9], the prime end rotation number is expressed in terms of the height of the kneading sequence of a unimodal map f (see the definition of height in e.g. [Citation9, Section 2.6]). Proposition 5.1 thus gives an algorithm to compute the height of the kneading sequence in the following way: find the smallest
such that
, and n is a cutting time
. Then the height equals
. If no such n exists, then the height equals
. Recall that b>c is such that
, so the itinerary of b is
, see (Equation11
(11)
(11) ), where
is the kneading sequence. Hence, the previous condition can be expressed with symbols as
, where ≺ denotes the parity-lexicographic ordering on symbolic sequences.
Furthermore, [Citation9] gives the complete characterization of accessible points the BBM embeddings of using the outside map. We emphasize it here and connect it to the stunted Lorenz map
.
Let be a circle parametrisation defined by
for
. Let
be the vertical projection, i.e.
for
. Furthermore, let
. As before, let
.
Proposition 6.2
Theorem 4.28(d), Remark 4.15, Definition 4.12, Corollary 4.14 in [Citation9]
Let be embedded in
by an orientation-preserving BBM embedding. Then
is accessible if and only if there exists
and
such that
for all i>N and such that
for all
.
Using the conjugacy of B and , we can state the previous theorem in terms of
directly. We parametrize the circle above as
as
and let
. The vertical projection onto a horizontal diameter is denoted by τ as above (that is actually
, where G is the conjugacy between
and B and it is equal to the vertical projection). In particular,
for all
.
Theorem 6.1
Let be a tent map with slope
and let
be corresponding stunted Lorenz map with rotation number α. Let
be embedded in
by an orientation-preserving BBM embedding. Let
. A point
is accessible if and only if there exists
and
such that
for all i>N and such that
for all
.
We say that a point is a folding point if
for every
. In the context of inverse limits on intervals this is equivalent to saying that x has no neighbourhood homeomorphic to the Cantor set times an open interval (see [Citation27]). In the case when rotation number of
is irrational, Proposition 5.1 and its proof imply that
is a homeomorphism (recall that orbits of c under ϕ and
are the same when the corresponding height of the tent map is irrational). From that and Theorem 6.1 we have the following:
Corollary 6.1
If and the rotation number of
is irrational (i.e. the height of the kneading sequence of
is irrational), then every folding point of
embedded in
by the orientation-preserving BBM embedding is accessible.
Proof.
We first note that is well defined and bijective. The first part follows since
, when
exists. Similar argument also shows that τ is surjective. For the proof of injectivity, it is enough to note that
implies that
or y = x and apply the fact that
is a homeomorphism.
Now let be such that
for every
. Then
for every i>0, so
. We apply Theorem 6.1 to conclude that
is accessible.
Remark 6.2
Given a continuum X, we say that point is an endpoint if for every subcontinua
such that
, we have
or
. In [Citation5] it was shown that if
is embedded in the plane by an orientation-preserving BBM embedding, and if
has irrational rotation number (i.e. the height of the kneading sequence of
is irrational), then all endpoints are accessible. Moreover, it was shown that there also exist countably many accessible non-end folding points. Corollary 6.1Footnote1 in particular implies that there are uncountably many endpoints and only countably many non-end folding point in
. This partially answers Problem 1 in [Citation4].
Let us discuss the irrational rotation number case in more details. If (and hence α) is irrational, then Proposition 5.1 gives that
for all j, and
is a Cantor minimal homeomorphism conjugate to a Sturmian shift. This implies that
induces Denjoy-like dynamics on the corresponding circle of prime ends P. In [Citation5], a detailed characterization of accessible points for BBM embeddings of tent inverse limit spaces is given (there, also accessible endpoints and non-end folding points are distinguished), based solely on symbolic dynamics techniques from kneading theory. It follows (see [Citation5, Theorem 11.20]) that there is a Cantor set
corresponding to accessible folding points in
uncountably many of which are endpoints and countably many are non-end folding points. Furthermore, all endpoints are accessible. The remaining countably infinitely many open arcs
correspond to countably infinitely many open arcs in different arc-components of
(unions of all arcs containing some point from
) that are accessible at more than one point. Thus this planar continua are interesting also from a topological perspective. A theorem of Mazurkiewicz [Citation24] shows that for every indecomposable planar continuum there are at most countably infinitely many arc-components accessible at more than one point. Our examples confirm that it is possible to find planar continua indeed having countably infinitely many arc-components accessible at more than one point. Furthermore,
is long-branched since
. Therefore, all proper subcontinua of
are arcs (see e.g. [Citation10, Proposition 3]).
Thus, from the discussion in this section we have a complete understanding of topology of as well as their orientation-preserving BBM planar embedding in the case when the rotation number of
is irrational (that is, the height of the kneading sequence of
is irrational).
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Notes
1 Its statement was suggested to us by Boyland, de Carvalho, Hall through personal communication.
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