Dynamics of 2-interval piecewise affine maps and Hecke-Mahler series
Michel Laurent, Arnaldo Nogueira

TL;DR
This paper explicitly characterizes the dynamics of a specific class of 2-interval piecewise affine maps using functions related to Hecke-Mahler series, revealing rational rotation numbers for algebraic parameters.
Contribution
It provides an explicit description of the dynamics of 2-interval piecewise affine maps via functions involving Hecke-Mahler series, linking algebraic parameters to rational rotation numbers.
Findings
Explicit formulas for the dynamics using functions δ and φ
Rotation number is rational for algebraic parameters
Connections between dynamics and Hecke-Mahler series
Abstract
Let be a -interval piecewise affine increasing map which is injective but not surjective. Such a map has a rotation number and can be parametrized by three real numbers. We make fully explicit the dynamics of thanks to two specific functions and depending on these parameters whose definitions involve Hecke-Mahler series. As an application, we show that the rotation number of is rational, when the three parameters are algebraic numbers.
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Dynamics of 2-interval piecewise affine maps and Hecke-Mahler series
Abstract.
Let be a -interval piecewise affine increasing map which is injective but not surjective (see Figure 1). Such a map has a rotation number and can be parametrized by three real numbers. We make fully explicit the dynamics of thanks to two specific functions and depending on these parameters whose definitions involve Hecke-Mahler series. As an application, we show that the rotation number of is rational, whenever the three parameters are all algebraic numbers, extending thus the main result of [16] dealing with the particular case of -interval piecewise affine contractions with constant slope.
Michel Laurent and Arnaldo Nogueira
2010 Mathematics Subject Classification: 11J91, 37E05.
\marginsize
2.5cm2.5cm1cm2cm
1. Introduction
Definition 1**.**
Let be the unit interval. Let be three real numbers. Assume
[TABLE]
Set and define a map by the splited formula
[TABLE]
The restrictions of to the intervals and are increasing affine functions with slopes and , respectively. The symmetry on exchanges the two slopes. Our assumption that the first segment of the graph has a slope less than is thus unrestrictive. Observe that and that the bound yields the injectivity of . Indeed the inequality
[TABLE]
holds true for any in the interval when ( is then a piecewise contracting map) and is equivalent to
[TABLE]
when (see Figure 1). Notice that in the limit case with , becomes a bijection which was studied in [3].
We are concerned with the dynamics of the family of interval maps . We plan to relate their dynamics to the so-called Hecke-Mahler series in two variables and (see Section 2 for definitions). The paper [16] deals with the case where the slope is constant. Although the map is not necessarily a piecewise contraction, we extend part of the results established in [16] to a -slope setting.
The dynamics of interval piecewise affine contractions has been studied by many authors, amongst others [6, 7, 8, 9, 11, 12, 13, 19, 22, 23]. According to [24], every map has a rotation number , . Although is not necessarily a piecewise contraction, we will prove that if takes an irrational value, then the closure of the limit set of is a Cantor set and is topologically conjugated to the rotation map on C. When the rotation number is rational, the map has at most one periodic orbit (exactly one in most cases) and the limit set equals the periodic orbit when it does exist. More precisely, either or (a slight modification of the map whose definition is postponed to Section 8) has a periodic cycle.
We make the above mentioned qualitative results fully explicit thanks to formulae involving Hecke-Mahler series. Our approach is based on the study of a conjugation function which may be written down in terms of Hecke-Mahler series. The method was already performed in the special case where the two slopes are equal. It is motivated by Coutinho’s thesis [9] and has been recently reworked in [4, 14, 16]. The general case involving two different slopes is quite similar. Theorem 1 gives the value of the rotation number in terms of the values of the three parameters , while Theorem 3 describes the behaviour of the orbits of and their relations with the conjugation .
Next we introduce some standard notations. For any real function of the real variable , we denote by
[TABLE]
respectively, the left limit and the right limit of at , whenever these limits do exist. As usual and stand, respectively, for the integer floor and the integer ceiling of the real number . In particular, we have for any real number and when . We denote by the fractional part of . The length of an interval is denoted by .
We first define a real function as follows.
Definition 2**.**
For positive real numbers and such that , set
[TABLE]
and
[TABLE]
For real numbers and with and , set
[TABLE]
The series converges when . For fixed and with , the map is increasing in the interval and it has a left discontinuity at each rational value (see Figure 2). It is continuous for any irrational and right continuous everywhere. The function enables us to compute the rotation number of thanks to the
Theorem 1**.**
*Let and be real numbers with and . Then the application is a continuous non decreasing function sending the interval onto the interval and satisfying the following properties:
(i) Let be a rational number with where and are relatively prime integers. Then takes the value if, and only if, is located in the interval*
[TABLE]
with the explicit formulae
[TABLE]
where
[TABLE]
*and the sum equals [math] when .
(ii) For every irrational number with , there exists one and only one real number such that and which is given by*
[TABLE]
Roughly speaking, the two maps and are “inverse” from each other, meaning that their graphs are symmetric with respect to the main diagonal. In the special case , we recover the formulae obtained in [16] for the map , which coincides with the contracted rotation . Notice that the formulae of our Theorem 1 are consistent with those of Theorem 4.15 in [6], dealing with the subfamily of contractions with , although the formulations greatly differ.
Applying now a classical transcendence result, which is stated as Theorem 4 below, to the number , we deduce from the assertion (ii) of Theorem 1 the following:
Theorem 2**.**
Let be algebraic real numbers with and . Then, the rotation number takes a rational value.
Notice that Theorem 2 no longer holds for the value when . Indeed, is an algebraic number when and are algebraic, while has rotation number by [3]. This ratio is a transcendental number when and are non-zero algebraic numbers, unless and are multiplicatively dependent.
We now investigate the behaviour of the iterates of thanks to an explicit conjugation map .
Definition 3**.**
Let be three positive real numbers such that , and let be an arbitrary real number. Let be the real function defined by the convergent series
[TABLE]
Theorem 3**.**
*Let be three real numbers with , and . Set and .
(i) Assume that is irrational. Then and the restriction of to the invariant set is conjugate by to the rotation . In other words, we have the commutative diagramm:*
[TABLE]
Moreover is a Cantor set and for every , the -limit set
[TABLE]
*equals .
(ii) Assume that is rational, where and are relatively prime, and that*
[TABLE]
Then
[TABLE]
is a cycle of order and we have the commutative diagramm:
where denotes the rotation . Moreover, for every , the -limit set equals .
(iii) When , the limit set is empty and is a finite set with elements containing . For every , the -limit set coincides with .
The paper is organized as follows. In Section 2, we introduce Hecke-Mahler series and relate them to our functions and . Then, Theorem 2 easily follows from Theorem 1. The purpose of Sections 3 and 4 is to establish the basic conjugation equations (1) and (3). This goal is achieved thanks to Lemma 4.2 where some relations connecting the parameter with values of the function are needed, as for instance the inequalities (2) in the case (3). It turns out that these constraints characterize the rotation number . As a consequence of the method, we establish Theorem 1 in Section 5. The next two sections provide additional information on the dynamics of in the case of an irrational rotation number (Proposition 5 in Section 6), or a rational one (Proposition 6 of Section 7). In both cases, we explicitly describe the iterated images . Finally Section 8 deals with the exceptional values of the form for which no periodic cycle exists.
2. Hecke-Mahler series and transcendental numbers
2.1. On Hecke-Mahler series.
We introduce the following sums:
Definition 4**.**
Let , and be positive real numbers such that . We set, for every real number ,
[TABLE]
with the convention that a sum indexed by an empty set equals zero.
Notice that is a right continuous function in the variable , while the function is left continuous in both variables and . Viewed as power series in the two variables and , these two functions are called Hecke-Mahler series which have been studied especially from a diophantine point of view [1, 2, 5, 10, 15, 17, 18, 20, 21]. We relate our functions and respectively to and .
Lemma 2.1**.**
Let be real numbers with and , then the following equality holds
[TABLE]
Proof.
Reverting the summation order for the indices involved in , we obtain
[TABLE]
A positive integer is of the form for some some positive integer if and only if , or equivalently . There exists at most one integer in the interval whose length is . The integer does exist exactly when and then . Otherwise, . Thus
[TABLE]
since . ∎
We deduce
Corollary**.**
Let and , then the map is increasing on the interval and sends the interval into the interval . Moreover, it is right continuous everywhere and continuous at any irrational point .
Proof.
Using Lemma 2.1, we can rewrite in the form
[TABLE]
We distinguish two cases whether or not. When , we have . The series converges for any and the map is obviously increasing, since is a sum of powers of and and that the set of summation indices enlarges when grows. We easily compute that
[TABLE]
It follows that
[TABLE]
for any . Since differs from [math] and , the homographic function
[TABLE]
is increasing on the interval , and sends this interval onto . By composition, we obtain that the image of by the map is contained in the interval . When , we have and the series tends to when tends to from below. Thus, we obtain in this case,
[TABLE]
For the continuity’s property, observe that the floor function is right continuous on and continuous on . ∎
We now give an alternative formula for the function in terms of the Hecke-Mahler series .
Lemma 2.2**.**
Let , and , then, for any real number , we have the equalities
[TABLE]
where the indeterminate ratio equals when . Moreover, the formula
[TABLE]
holds for any real number .
Proof.
From Definition 4, we can write
[TABLE]
which implies (5). For equation (6), multiplying (5) by , we find
[TABLE]
Observe that, for any integer , takes only the value 0 or 1. Therefore
[TABLE]
We obtain the equality
[TABLE]
from which formula (6) follows. The map has period 1 for any integer . We can thus replace by its fractional part in the sum over occurring in the definition 3 giving . Observe also that for any real number . We can therefore rewrite in the form
[TABLE]
Using (5) and (6) for and noting that , we obtain
[TABLE]
∎
Corollary**.**
*Let , , and , then the function is right continuous and non-decreasing on the interval . Moreover,
(i) is strictly increasing on , if is irrational.
(ii) If is rational, the function is constant on each interval .
(iii) In any case, the relation holds for any real number .*
Proof.
The function is clearly non-decreasing and strictly increasing when is irrational. By Lemma 2.2, we have
[TABLE]
when . Notice that, by the assumption, the coefficient is negative which yields that is non-decreasing. The other assertions are straightforward. ∎
2.2. Proof of Theorem 2
Let us begin with the following result on the transcendency of values of the Hecke-Mahler function, due to Loxton and Van der Poorten [17]. See also Sections 2.9 and 2.10 of the monograph [20] and the survey article [18].
Theorem 4**.**
Let and be non-zero algebraic numbers and let be an irrational real number. Assume that and . Then is a transcendental number.
Using the homographic relations (4), both numbers and are simultaneously either algebraic or transcendental. Then, it follows from Theorem 4 that is a transcendental number for any irrational real number . As a consequence of the assertion (ii) of Theorem 1, the rotation number cannot be an irrational number when are algebraic numbers. It is therefore a rational number. Theorem 2 is established.
3. Properties of the function
Let be four real numbers satisfying the inequalities
[TABLE]
We estimate in this technical section the value of the function at the points [math] and according to the values of . We stress that is not assumed here to be the rotation number of the map . On the opposite, we shall make use of our results to identify this rotation number in the subsequent Section 5, and thus proving Theorem 1. Our estimates are based on numerical relations betweeen some special values of the Hecke-Mahler series and the function , as for instance the formulae (9) to (12) below.
Lemma 3.1**.**
Assume that is irrational. Let and . Then the following equalities hold
[TABLE]
Proof.
Recall the formula
[TABLE]
Notice first that we have the equalities
[TABLE]
the last one coming from Lemma 2.1 and noting that the strict inequality is equivalent to , when is irrational. It follows from Lemma 2.2 and (7) that
[TABLE]
For the value , we compute using (6). Noting that , we find
[TABLE]
since for any integer . Therefore
[TABLE]
since . ∎
When is a rational number , the function is constant on any interval of the form , and has a positive jump at the endpoints . In this case, we have the analogous
Lemma 3.2**.**
Assume that and Put . Then
[TABLE]
and
[TABLE]
Proof.
Set and . We first show that
[TABLE]
where we recall the notation
[TABLE]
from Theorem 1. By Definition 2, we have
[TABLE]
Observe that . Splitting the above sum over according to the various classes of modulo , we obtain the first formula
[TABLE]
Similarly, we have
[TABLE]
Now, we establish the formulae
[TABLE]
To that purpose, we observe that the function is constant on each interval , and we use formula (6). Gathering as above the various classes of modulo , we obtain the sums
[TABLE]
since for and . Similarly, we have the equalities
[TABLE]
since for . For the value , we find
[TABLE]
taking again the computations used for . Finally, we get
[TABLE]
by the above computation of . The formulae (9) to (12) are established. We now use Lemma 2.2 in order to estimate values of . We have
[TABLE]
Then (9) yields
[TABLE]
since . Observe now that the factor is always positive. Indeed, we deduce from Lemma 2.1 and its corollary that
[TABLE]
Therefore is bounded from below by when and by when . It follows that is if and only if . For the value , observe that tends to from above when tends to 0. Lemma 2.2 provides now the formula
[TABLE]
Then (10) yields
[TABLE]
It follows that is negative if and only if . We now deal with the lower bound at the point . Using Lemma 2.2 and (11), we find
[TABLE]
since the expression
[TABLE]
appearing above in the numerator is . The computations are similar for the left limit at the point . Using (12), we find
[TABLE]
since
[TABLE]
∎
4. The lift
Let be the real function defined by
[TABLE]
Then is a lift of , meaning that satisfies the following properties:
(i) For every , we have
[TABLE]
(ii) , for every .
(iii) is an increasing function on which is continuous on each interval of and right continuous everywhere.
Let and let be the forward orbit of by , where stands for the -th iterate of the function . When belongs to , we denote moreover by the backward orbit of by , where is the -th preimage of by . This makes sense since is the -th preimage of by and is the inverse image of by the injective map , noting that for all . A fundamental property is that any forward orbit can be computed explicitely in terms of its initial point and of the associated *symbolic sequence *
[TABLE]
It turns out that, for any orbit, this symbolic sequence is either periodic when the rotation number is rational, or a sturmian sequence of slope in the irrational case. We have the following explicit recursion formulae which motivate our definition of the conjugation :
Lemma 4.1**.**
Let and let be the forward orbit of by . For any non-negative integers and , we have the relation
[TABLE]
Moreover, assume that . Let be the backward orbit of by and assume that there exist two real numbers and with such that for all integer . Then, we have the series expansion
[TABLE]
Proof.
Notice that for any integer . Put
[TABLE]
so that . Thus . Let be a positive integer. Composing these affine relations for , we obtain by induction on the formula
[TABLE]
where we have set
[TABLE]
We display the terms
[TABLE]
appearing in the above sum. Note that . Thus, by Abel’s summation, we find
[TABLE]
Replacing the index of summation by in the last sum, we find
[TABLE]
The first assertion is established. For the second one, observe that the first assertion remains valid for negative when belongs to , since then has a preimage and we apply the formula at this point. Choosing and letting tend to infinity, we get the stated series expansion. ∎
The next result is crucial in our approach. It shows that satisfies a functional equation as in Theorem 3.
Lemma 4.2**.**
Let , , and be real numbers such that , . We assume that when is irrational, or that belongs to the interval (2) when is rational. Put and . Then, the relations
[TABLE]
hold for any real number . Thus, the -orbit of is given by the sequence
[TABLE]
Proof.
We first show that when . In the case irrational, Lemma 3.1 gives . Thus and the corollary of Lemma 2.2 asserts that the function is strictly increasing. Therefore
[TABLE]
In the rational case, the function is non-increasing and constant on each interval . Now, we know that and by Lemma 3.2. Therefore
[TABLE]
For any , we can write
[TABLE]
We have thus proved that and for all real number . We now prove the relation . By definition of , we have to deal with two expressions for the value of depending whether the fractional part is smaller than or not. But and Lemmae 3.1 and 3.2 yield that belongs the interval when , and to the other interval when , since is non-decreasing. The computation splits into two cases. Suppose first that . Then . Moreover, by Lemmae 3.1 and 3.2 and the increasing monotonicity of the function . Using the expression of in the intervals , we obtain the equalities:
[TABLE]
The case is similar. Then and by Lemmae 3.1 and 3.2. We now use the expression of in the intervals . We then obtain the equalities:
[TABLE]
∎
5. Proof of Theorem 1
Let and let be the forward orbit of by . It is known (see [24]) that the limit
[TABLE]
exists and does not depend on the initial point . The number is called the rotation number of the map . Fix and with , . Let be a real number in the interval . By the corollary of Lemma 2.1, the following alternative holds. Either belongs to the image of the interval by the function , or
[TABLE]
for some rational number with (these intervals are the jumps of the increasing function ). In the latter case, Lemma 4.2 yields that . Indeed, we select an initial point of the form for an arbitrary , so that for every integer . Then,
[TABLE]
It remains to deal with parameters in the image, in other words for some . When is irrational, Lemma 4.2 yields as well that . When is rational, we may use a general argument of continuity. Proposition 5.7 in [25] tells us that the rotation number is a continuous function of the parameter . Thus
[TABLE]
since we have already proved that is constant and equal to when is located in the right open interval
[TABLE]
We express now and in term of the finite sum . Recalling formula (8), we obtain
[TABLE]
and
[TABLE]
6. Irrational rotation number
We prove part (i) of Theorem 3 and we give furthermore a description of the iterated images when the rotation number is irrational. In this case, the function is strictly increasing on and jumps at the points . Put
[TABLE]
All the intervals , are pairwise disjoint and contained in .
Proposition 5**.**
For any integer , we have the decomposition into disjoint intervals
[TABLE]
and the formulae
[TABLE]
Moreover, the set equalities
[TABLE]
hold. The set is topologically homeomorphic to a Cantor set.
Proof.
Lemma 4.2 shows that for any and any , we have the equalities
[TABLE]
and
[TABLE]
where stands for the -th iterate of . Since is increasing and continuous on , it follows that
[TABLE]
so that any number has integer part . We first show that
[TABLE]
Since is right continuous and increasing, no point of is located in an interval of the form . Thus, we have the inclusion The reversed inclusion follows straightforwardly from the right continuity of . Indeed, let which is located outside the intervals . For every , define an index among the integers for which and is the closest to . It is readily seen that the decreasing sequence converges to a number and that by right continuity of . We know by Lemma 3.1 that the critical point is located in the image . In particular, this critical point does not belong to any interval . The function is thus continuous on each interval , so that we deduce from (15) that
[TABLE]
by reducing modulo 1. Now, Lemmae 3.1 and 4.2 yield the equalities
[TABLE]
Looking at Figure 1, we immediately observe that , as announced. Taking now the image by and using (16), we find
[TABLE]
Arguing by induction on , we thus deduce from (16) the required equality
[TABLE]
Letting tend to infinity, we finally obtain that
[TABLE]
It remains to establish the explicit formulae giving and . Lemma 4.1 delivers the expression
[TABLE]
since for every integer . Taking the fractional part, we obtain the formula
[TABLE]
The equality immediately follows from Lemmae 3.1 and 4.2. Similarly . We have and for any integer . Then, Lemma 4.1 gives
[TABLE]
As a corollary of the above formulae, let us briefly prove that is a Cantor set. The Lebesgue measure of is equal to
[TABLE]
Using (5) and (7), we easily compute the sum
[TABLE]
where . On the other hand, we have
[TABLE]
Therefore is a null set. Consequently, it has no inner point. Moreover, has no isolated point, since the function is strictly increasing and right continuous. It follows that the compact set is homeomorphic to a Cantor set. ∎
In order to complete the proof of the assertion (i) of Theorem 3, we now show that for any point , the -limit set coincides with . To that purpose, we consider the orbit , of . When belongs to , Lemma 4.2 shows that so that . The sequence of fractional parts is dense in , since is an irrational number. Thus the set of accumulation points of the orbit is equal to . It remains to deal with points not belonging to , it means for some . Observe first that
[TABLE]
since . In particular the symbolic sequence coincides with the sturmian sequence , where we have set . Then, Lemma 4.1, with and , provides us the formula
[TABLE]
Thus, the -orbit converges exponentially fast to the -orbit as tends to infinity. Reducing modulo 1, one obtains as well that .
7. Rational rotation number
We prove the statement (ii) of Theorem 3 and add a dynamical description of the iterated images of . We assume throughout this section that the inequalities (2) are fulfilled for some rational number . Then, Theorem 1 asserts that the rotation number of equals . Put and set
[TABLE]
It is convenient to extend the sequence by -periodicity setting for any integer , where is the remainder in the euclidean division of by . Then, Lemma 4.2 yields the formula
[TABLE]
As is nondecreasing , we claim that these numbers are distinct. If not, there exists such that . Iterating thus , , obtaining that the function is constant, in contradiction for instance with Lemma 3.2. Moreover, , again by Lemma 3.2. So, we have an increasing sequence
[TABLE]
in . It follows that the set is an -cycle of order , on which acts by the substitution modulo . Recall that and , where is the critical point of the map . Moreover, Lemma 3.2 shows that . If does not belong to , we have strict inequalities and . Otherwise and . The latter case occurs only when coincides with the left end point of the interval (2). Indeed (13) shows that vanishes if and only if . \marginsize2.5cm2.5cm1cm2cm
The next proposition provides a partition of the image , , into disjoint intervals. It is convenient to consider circular intervals (or circle arcs identifying with ). For any both belonging to , we set
[TABLE]
We write for instance .
Proposition 6**.**
For any integer , the circular interval \big{[}f^{l}(1^{-}),f^{l}(0)\big{)} is contained in \big{[}\zeta_{lp-1},\zeta_{lp}\big{)}=\big{[}f^{l}(\zeta_{q-1}),f^{l}(\zeta_{0})\big{)}. We have when is not divisible by and when is a multiple of . The decomposition into disjoint intervals
[TABLE]
and
[TABLE]
holds true. Moreover has Lebesgue measure .
Proof.
Let us consider the partition of
[TABLE]
into disjoint circular intervals. The action of on these intervals is drawn in Figure 6. The inclusions
[TABLE]
hold for and we have equality
[TABLE]
for . However, for , we have a strict inclusion:
[TABLE]
Thus (17) holds for . Applying to this decomposition, we observe the appearance of a second “hole” contained in the interval , just over the first hole dotted on Figure 6. Iterating again, we obtain (17) for (note that the formulae (17) and (18) coincide for ). At the -th iteration, each interval \big{[}\zeta_{lp-1},\zeta_{lp}\big{)},1\leq l\leq q, has been holed and does not belong to . Then, exchanges the intervals and contracts them. We thus obtain formula (18) for . We finally prove the bound for the Lebesgue measure of the iterated images . We claim that
[TABLE]
for every integer . Suppose for instance and rewrite (18) in the form
[TABLE]
Each interval or involved in the disjoint union (20) is contained either in or in . Keeping track of the iterated images
[TABLE]
for in the decomposition (20) at level (instead of ), we observe that is an interval contained in for values of and in for the remaining values of (see Figure 5). Notice that the image of any interval contained in (resp. ) is an interval whose lenght equals (resp. ). The length of equals the length of multiplied either by or by , according whether is contained in or in . It follows that
[TABLE]
Summing over the disjoint intervals occurring in (20), we obtain (19) for . The proof for is similar, now based on the decomposition (17). Using euclidean division, write , with . Equation (19) yields the required bound
[TABLE]
∎
We deduce from Proposition 6 the following explicit decomposition of the images .
Corollary**.**
Let . Denote by the multiplicative inverse of modulo . For every integer with , let be the unique integer in the interval which is congruent to modulo . Then, the decomposition into disjoint intervals
[TABLE]
holds true. For every integer with , the interval contains the point .
Proof.
Recall the decomposition (20) and observe that and that is a bijection of the set . Collecting the intervals involved in (20) by pairs , we find
[TABLE]
∎
It follows from the corollary that
[TABLE]
Indeed, is contained in , for every . The image , for , equals the union of intervals whose lengths shrink to [math], as , noting that Proposition 6 delivers the bound
[TABLE]
where in both upper bounds, the numbers and are less than . This proves (21). Since these disjoint intervals rotates under the action of , we obtain as well that the the -limit set equals , for any . The proof of the assertion (ii) of Theorem 3 is complete.
8. The right end point
We deal here with the exceptional value . Let us first explain the reasons why the arguments expanded in Section 7 do not apply to this value. Indeed, (14) shows that in this case. Then
[TABLE]
and the set cannot be of course an -cycle, since it contains the point which is outside the set of definition of the map . We slightly modify the map in order that the obstruction no longer holds. Put . As usual, let be three real numbers with
[TABLE]
and let be the rotation number of . Recall the associated lift and the conjugation . We introduce three functions and which are the left limit of and respectively.
Definition 5**.**
(i) Let be the map defined by
[TABLE]
(ii). Let be the map defined by
[TABLE]
(iii) Let be the map defined by
[TABLE]
The maps and share almost the same dynamical behaviour and we present the analogies, omitting the proofs which follow the lines of Sections 3 and 4. The two maps and coincide on and differ at the critical point where and . Thus, any -orbit contained in does not contain the point and is also an -orbit. The function turns out to be a lift for the circle map , identifying now the circle with the interval . It follows that both maps and have the same rotation number . One can show that when is irrational, or when is rational and
[TABLE]
the functional equation holds for any . Moreover, when is irrational, the closure is the Cantor set considered in Theorem 3 (i) and any -orbit approaches of this Cantor set. When (22) holds, every -orbit approaches cyclically of the periodic -cycle
[TABLE]
of order . From now, let us fix and put . Since belongs to the interval (22), is an -cycle of order containing the point . Let be an -orbit. If , then is also an -orbit which converges to . It follows in particular that there exists no finite -cycle. Indeed, arguing as in Section 7, this finite cycle should be an attractor for any -orbit , and it would be equal to , which is impossible since . Suppose now that . Then [math] appears only once in . If not, would contain a finite -cycle. Hence, some tail of does not contain [math] and converges as well to . Part (iii) of Theorem 3 is established. Acknowledgements. We graciously acknowledge the support of Région Provence-Alpes-Côte d’Azur through the project APEX Systèmes dynamiques: Probabilités et Approximation Diophantienne PAD, CEFIPRA through the project No. 5801-B and the program MATHAMSUD projet No. 38889TM DCS: Dynamics of Cantor systems.
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