Víctor F. Sirvent 1 Departamento de Matemáticas, Universidad Simón Bolívar, Caracas, Venezuela
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1 # A5 INTEGERS B (2) SYMMETRIES IN K-BONACCI ADIC SYSTEMS Víctor F. Sirvent Departamento de Matemáticas, Universidad Simón Bolívar, Caracas, Venezuela vsirvent@usb.ve Received: 9/2/, Revised: 3/7/, Accepted: 7/5/, Published: 2/2/ Abstract In this paper we study the symmetries of the k-bonacci adic systems and their geometrical realizations known as Rauzy fractals. We consider the maximal invariant subset under the involution or mirror image in {, } N that exchanges with. We explore the dynamical properties of the induced dynamical system on this set and their geometrical realizations as subsets of Rauzy fractals.. Introduction In this paper we explore some symmetries of the k-bonacci adic systems, (R(k), T k ), and their geometric realizations known as Rauzy fractals. These adic systems are symbolic dynamical systems with symbols in the alphabet {, }. The adic map T k is given by addition by in R(k); it will be defined in Section 2. We consider the maximal subsystems invariant under the involution or mirror image Ψ : {, } N {, } N, which consists of mapping each into and vice versa. Let P(k) be the maximal subset of R(k) invariant under Ψ. We obtain this set using the concept of the product automaton; see Section 3. We show in Theorem there is a continuous map S k on P(k) such that the dynamical system (P(k), S k ) is semi-conjugated to (R(k ), T k ), and the semi-conjugacy is 2 to. So we can interpret P(k) as a double cover of R(k ), and the sucessor map in R(k ), i.e., T k, is lifted continuously to a map S k on P(k). We explore how the symmetries in the symbolic systems are reflected in their geometrical representations; we also show that Theorem does not have a geometric counterpart. However, the dynamical system (P(k), S k ) can be realized in R k as a permutation in k pieces; see Propositions 6 and 7. The systems (P(k), S k ) were first introduced by the author in [22], where their metrical properties were studied. Unlike there, in the present paper we use the language of automata theory and in particular the notion of the product automaton vsirvent
2 INTEGERS: B (2) 2 in order to introduce and study these systems. The properties of the geometrical realizations, and the symmetries involved, were not addressed before. Here we do not consider the relation of the dynamical systems studied with substitution dynamical systems [7, 8]. 2. Adic Systems Let A = {,..., k} be a finite alphabet and W A = i A i a set of finite words on A. An automaton over A, A = (Q, W, E, I), is a direct graph labelled by elements of A. We let Q be the set of states, I Q is the set of initial states, W is the set of labels and E Q W Q is the set of labelled edges or transitions. If (p, w, q) E we say that w is a transition between p and q. Here we will consider W a finite set, Q = A and I = {}. A finite path in the automaton A is a word in E; that is, it is a sequence of transitions: (p n, a n, q n )(p n, a n, q n ) (p, a, q ) such that q i = p i for i n and p n I; however, we usually denote the paths using only the labels, i.e., a n a. The automaton reads words from left to right. See [8] for more on automata theory. The transition matrix of an automaton is the matrix M whose m ij entry is defined as the number of different transitions from i to j. We shall assume that the automaton is primitive, i.e., for some integer m > each entry of M m is positive. Let R = { a = a a... W N : a n... a is a path in A for all n N }, where A is an automaton. We consider in R the topology induced from the product topology of W N, i.e., the usual metric topology on -sided infinite sequences over a finite alphabet. We can order lexicographically all the finite paths in A, so the addition by of a given element in W is its consecutive element. Due to the definition of R, addition by is well-defined in R, and we will denote this map by T. There are only a finite number of maximal elements of R. If a is a maximal element of R, then T (a) is the minimal element of R. Here we suppose that there is only one minimal element in R. Hence we have the dynamical system (R, T ), which is called the adic system. If the transition matrix is primitive then the dynamical systems (R, T ) is primitive, i.e., every orbit is dense. We note that an adic system is sometimes also called stationary Markov compactum or stationary Bratteli-Vershik system; see [3, 27, 7, 3, 7, 3] for further details. These dynamical systems are related to general numeration systems; for details see [2, 6,, ]. Let A = {,..., k}, W = {, } where denotes the empty word, Q = A, E = {(,, ), (,, 2), (j,, j + ), (j,, ), (k,, ) : 2 j k }
3 INTEGERS: B (2) 3 2 Figure : The Fibonacci automaton k Figure 2: The k-bonacci automaton. and I = {}; see Figure 2. This is known as the k-bonacci automaton; we shall denote it by A(k). For k = 2 it is called the Fibonacci or golden mean automaton; see Figure. The corresponding adic system is denoted by (R(k), T k ), in order to emphasize the dependency on k. It is easy to check that the automaton A(k) is symmetrical in the sense that a n... a is a path in A(k) if and only if a... a n is a path in A(k). Then R(k) := { a = a a... {, } N : a n... a is a path in A(k) for all n N } = { a = a a... {, } N : a... a n is a path in A(k) for all n N } = { a = a a... {, } N : a i a i+ a i+k a i+k =, i }, where a i a j denotes the usual product of natural numbers, i.e., the space R(k) consists of all one-sided infinite sequences of and such that there are no k consecutive s. For an automaton A = (Q, W, E, I) whose set of labels W is {, } we define its dual automaton as the automaton  = (Q, W, Ê, I) where Ê = {(p, ŵ, q) : (p, w, q) E} where ŵ = { if w = if w =.
4 INTEGERS: B (2) 4 For an adic system (R, T ) whose set of labels is W = {, }, we define its dual adic system ( R, T ) using the dual automaton. Since taking the dual reverses the ordering in W, we have the relation T ( T (â)) = a, or equivalently T ( T (a)) = â for any a R. We remark that T is still adding by, but on R. 3. Product Automaton Let A and A 2 be two automata on the alphabets A and A 2 respectively. The product automaton A A 2 is defined as the automaton satisfying: set of states: A A 2. labels: w is a label of A A 2 if and only if w is a label of A and A 2. transitions: w is a transition between (p, q ) and (p 2, q 2 ) if and only if w is a transition between p i and q i, for i = and 2. initial states: the product of the initial states of A and A 2. And finally the connected component containing the initial state is taken. The paths in A A 2 are paths in A and A 2, so it is said that the paths in the product automaton are the common paths in each of the factors. The product automaton was used in [25, 2] in the study of adic systems. Let A be an automaton with labels in {, }. The product automaton A Â is called the canonical product of A. Let } P = {a = a a... W N : a n... a is a path in A Â for all n N. Let Ψ : {, } N {, } N be the involution Ψ(a) = â = â â.... By definition, P is the maximal subset of R invariant under Ψ. Here we shall consider A(k) Â(k); see Figure 3. Let B(k) be the automaton of Figure 4. It can be easily checked that A(k) Â(k) and B(k) are equivalent, i.e., both automata recognize the same finite paths. Observe that B(k) is also symmetrical, i.e., a n... a is a path in B(k) if and only if a... a n is also a path in B(k). Let P(k) be the set of infinite paths on B(k), for k 3. The set P(2) consists of only two points, namely () =... and () =.... Since P(k) is invariant under the involution Ψ, } P(k) := {a = a a... {, } N : a n... a is a path in A(k) Â(k) for all n N } = {a = a a... {, } N : a... a n is a path in A(k) Â(k) for all n N = a = a i+k a... {, } N : < a j < k, i, j=i
5 INTEGERS: B (2) 5,, 2, 3, 4..., k 2, 3, 4,... k, Figure 3: The canonical product of k-bonacci automaton, i.e., A(k) Â(k)., 2, 3, 4..., k 2, 3, 4,... k, Figure 4: The automaton B(k) is equivalent to A(k) Â(k). i.e., the space P(k) consists of all one-sided infinite sequences of and such that there are no k consecutive s nor k consecutive s. Theorem. Let (R(k ), T k ) be the (k )-bonacci adic system and P(k) as before. For k 3, there exist continuous maps φ k : P(k) R(k ) and S k : P(k) P(k) such that φ k is 2 to and semi-conjugates the dynamical system (P(k), S k ) with (R(k ), T k ), i.e., the following diagram commutes P(k) φ k S k P(k) φ k R(k ) T k R(k ).
6 INTEGERS: B (2) 6 Moreover, let σ(a a a 2 ) = a a 2 be the shift map. Then the dynamical system (P(k), σ) is semi-conjugate to (R(k ), σ), by the semi-conjugacy φ k. Proof. Let A(k) Â(k) be the canonical product of the k-bonacci automaton; see Figure 3. If in this automaton we identify the state (, m ) with (m, ) for 2 m k, we get the automaton seen in Figure 5. If we erase the state (, ) and define (2, ) as the initial state, we get the (k )-bonacci automaton; see Figure 6. More precisely, let π be the map from the set of edges of the automaton A(k) Â(k) to the set of edges of the automaton of Figure 6 defined as follows: ((, 2 ),, (2, )) (,, ), ((2, ),, (, 2 )) (,, ), ((, j ),, (, j + )) (j,, j), ((j, ),, (j +, )) (j,, j), ((, j ),, (2, )) (j,, ), ((j, ),, (, 2 )) (j,, ), ((, ),, (, 2 )) (,, ), ((, ),, (2, )) (,, ); where 2 j k. The map φ k is the resulting map on P(k) after the identification described on the automaton A(k) Â(k). Let a P(k). Due to the symmetry of P(k) pointed out before, we can write it as: a = (p, a, p )(p, a, p 2 ) where p i are the states and a i the labels in A(k). Since π(p, a, p ) = (,, ), we define φ k (a) := π((p, a, p 2 ))π((p 2, a 2, p 3 )). Since φ k is continuous and bijective on each P(k) i := {a = a a... P(k) : a = i}, for i = and, the map T k lifts continuously to Sk : P(k) P(k) and Sk : P(k) P(k), where Sk i = φ k T k φ k for i =,, i.e., each Sk i is topologically conjugated to T k. We define S k : P(k) P(k) a Sk i (a); if a P(k) i. Since P(k) and P(k) are disjoint, the map S k is well-defined and the continuity follows from the continuity of Sk i. By construction we get φ k (S k (a)) = T k (φ k (a)). On the other hand, from the definition of φ k, the spaces P(k) and R(k) are σ-invariant and it also follows that for a P(k): φ k (σ(a)) = π((p 2, a 2, a 3 ))π((p 3, a 3, a 4 ))... = σ(φ k (a)).
7 INTEGERS: B (2) k Figure 5: The automaton π(a(k) Â(k)) k Figure 6: The automaton obtained from the automaton of Figure 5 after removing the state. This automaton is equivalent to the (k )-bonacci automaton.
8 INTEGERS: B (2) 8 Corollary 2. Let Ψ be the involution defined before. Let S k/ Ψ : P(k) / Ψ P(k) / Ψ be the map corresponding to S k under the projection which maps P(k) into P(k) / Ψ. Then the dynamical systems ( P(k) / Ψ, S k/ Ψ ) and (R(k ), T k ) are topologically conjugated. Proof. By the definition of the map φ k, we get φ k (Ψ(a)) = φ k (a). Since Ψ is a homeomorphism between P(k) and P(k), we have P(k) / Ψ is homeomorphic to P(k) and P(k). According to Theorem, φ k/ Ψ : P(k) j R(k ) is continuous and bijective for j =,. Since both spaces are compact, this map is a homeomorphism. Therefore ( P(k) / Ψ, S k/ Ψ ) and (R(k ), T k ) are topologically conjugated. This Corollary shows that we can interpret P(k) as the double cover of R(k ) with the successor map on R(k ) and the corresponding lifted map on P(k). We point out that the map S k, i.e., lifted map on P(k), is not the adic map on this space. 4. Rauzy Fractals The eigenvalues of the transition matrix of the k-bonacci automaton (i.e., the roots of the polynomial x k x k x ) are of the form γ, γ,..., γ s γ s, γ s+, ρ where γ j <, γ,..., γ s are non-real complex, γ s+ is real, this eigenvalue only exists if k is even; and ρ is real and bigger than ; see [4]. Let R(k) := ( a i γ i,..., a i γs i, a i γs+ i ) Rk : a = a a... R i i i if k = 2s + 2, and R(k) := ( a i γ, i..., a i γs) i R k : a = a a... R i i if k = 2s +. Here we identify C s with R 2s. This set is known as the Rauzy fractal of the k-bonacci automaton, first introduced by G. Rauzy for k = 3 in 982 [9]; see Figure 7. In [9] it was proved, for k = 3, that it is compact, convex and simply connected. The geometrical and dynamical properties of this set have been studied extensively; see for instance [, 2, 5, 2, 6, 7, 29, 24, 26].
9 INTEGERS: B (2) 9 The set R(k) admits a natural partition {R(k),... R(k) k }, which is also called the natural decomposition, where R(k) j := ξ k(a) : a = } {{ }. () j In Figure 7, R(3) and its natural decomposition can be seen. Figure 7: The Rauzy fractal R(3) and its natural decomposition. We define the map ξ k : R(k) R k, a ( i a iγ i,..., i a iγ i s, i a iγ i s+), if k = 2s + 2; a ( i a iγ i,..., i a iγ i s), if k = 2s +. By construction R(k) = ξ k (R(k)). The adic dynamical system (R(k), T k ) allows us to define a dynamical system in
10 INTEGERS: B (2) the Rauzy fractal (R(k), F k ) such that the following diagram commutes: T k R(k) R(k) ξ k ξ k R(k) Fk R(k). (2) The map F k is defined by F k (x) = x + v i if x R(k) i, where γ v = v 2 =,, v k =.. γ s+ γ k γ k 2 γ. γs+ k γk 2 s+ γ s+ Here v j R k, and we identify C s with R 2s. We suppose for notational purposes that k = 2s + 2, with s. We say that the dynamical system (X, H) is a piece exchange or domain exchange if X R k and there exists a partition {X,..., X m } of X, i.e., X = m i= X i and their interiors in the relative topology are disjoint pairwise, such that H exchanges the elements of the partition by translations. So (R(k), F k ) is a domain exchange transformation. See [, 5, 7] for details of domain exchange transformations. Theorem 3. Let ξ k : R(k) R(k) as before. Then ξ k ( R(k)) = R(k) = ξ k (R(k)). Proof. Let us introduce some definitions and notation. Let R(k) := ξ k ( R(k)). Let R (k) be the set of finite paths on the automaton A(k), i.e., R (k) := {a a... a n W : a n... a is a path in A(k) for all n N} and R (k) is its dual. Let us remark that the map ξ k is well-defined on elements of R (k) and R (k). We give the proof for k = 3 in order to simplify the notation. But the ideas of the proof are the same for any k. Let a = a... a n R. We shall associate an element b R such that ξ(a) = ξ(b). If a R then b = a. If a / R, without loss of generality we can assume that a n =. Let So we define l := max j n {j : a j =, a j =, a j 2 =, a j 3 = }. b l 3 =, b l 2 =, b l 2 =, b l =, b l+i = a l+i, for i n l. Now we repeat this process with the word a... a l 4, until l 4. By construction b R..
11 INTEGERS: B (2) Denote by γ any root of the polynomial x 3 x 2 x. Since + γ + γ 2 = γ 3, we get ξ(a) = ξ(b). Furthermore, since + j= γ3j+ +γ 3j+2 =, we have ξ(a() ) = ξ(b() ) and a R, b() R. The elements a, b() are dense in R and R, respectively. Therefore R R, the reverse inclusion is proved in a similar manner. Figure 8: The set F(3). Let F(k) := ξ k (P(k)). Figure 8 shows the set F(3) and its partition {F(3), F(3), F(3), F(3) }, where F(3) bb := ξ 3 (P(3) bb ) and P(3) bb := {a = a a... P(3) : a = b, a = b }. Corollary 4. The sets R(k) and F(k) have the same center of symmetry. Proof. For notational purposes, let k = 2s + 2, with s. Let a R(k) or
12 INTEGERS: B (2) 2 a P(k). Then ξ k (a) + ξ k (â) = ( a i γ, i..., a i γs, i a i γs+) i i i i +( i â i γ i,..., i â i γ i s, i â i γ i s+) = ( i a i γ i,..., i a i γ i s, i a i γ i s+) +( ( a i )γ i,..., i i = ( γ i,..., i i = (,..., γ γ i s, i γ i s+ ) γ s, γ s+ ). ( a i )γ i s, i ( a i )γ i s+ ) Since ξ k (a), and ξ k (â) are in R(k), or in F(k), then the center of symmetry of these sets is (/2( γ ),..., /2( γ s+ )) if k = 2s + 2 or (/2( γ ),..., /2( γ s )) if k = 2s +. Corollary 5. The center of symmetry of R(k) and F(k) is in R(k), but not in F(k). Proof. By Proposition 4, the center of symmetry of R(k) and F(k) is (/2( γ ),..., /2( γ s+ )) if k = 2s + 2 or (/2( γ ),..., /2( γ s )) if k = 2s +. Since + γ i + + γ k i = γi k, we have: = γ j i 2( γ i ) 2 = 2 (2γk i + 2γ2k+ i + 2γi 3k+2 + ) = γ (k+)j+k i. j= So the center of symmetry of R(k) is ξ k (b), where b = ( }. {{.. } ). Clearly b is in k R(k), so ξ k (b) R(k). It is clear that b is not in P(k). In order to prove that ξ k (b) / F(k), we shall show that the image under ξ k of a neighbourhood of the point b is disjoint from F(k). For simplicity we assume that k = 3. Let j= U b := {a R(3) : a 3 =, a i = for i =,, 2, 4, 5, 6} and U := ξ 3 (U b ), so U = γ 3 + γ 7 (R(3)). We have i a iγ i = i a i γi for a, a R(3) if and only if we can pass from one expression to the other using the relation + γ + γ 2 = γ 3. Considering the elements of U are of the form i a iγ i with a 3 = and a i = for i =,, 2, 4, 5, 6, it is not possible to rewrite them in any of the following forms: + γ + γ 4 (x), + γ 2 + γ 4 (x), γ + γ 4 (x), γ 2 + γ 4 (x),
13 INTEGERS: B (2) 3 where x is an element of R(3), which are the allowed expressions for the elements of F(3). Therefore U and F(3) are disjoint. 4.. Some Remarks (i) From Theorem 3 and Corollary 4 it follows that the duality on the Rauzy fractal, R(k) and on the subset F(k), acts as a reflection in the center of symmetry. (ii) In the special case of k = 3, the boundary of the set R(3) is contained in the F(3), since the characterization of the boundary of R(3) given in [6] does not admit points whose symbolic representation has more than three consecutives s. However, the inclusion is proper since the Hausdorff dimension of F(3) is 2 log ρ(2)/ log ρ(3).579, where ρ(k) is the root outside the unit circle of the the polynomial x k x k x for k = 2, 3 [23]; and the Hausdorff dimension of the boundary of R(3) is 2 log θ/ log ρ(3).93 where θ is the root outside the unit circle of the polynomial x 4 2x [4, 24]. We conjecture that for k 4, the boundary of R(k) is properly contained in F(k). (iii) The map F k : R(k) R(k), was defined on each element of the natural decomposition of R(k). In a similar way, we will use the symbolic dynamics to define a map S k : F(k) F(k), such that it makes commutative the diagram: P(k) ξ k S k P(k) ξ k F(k) Sk F(k). The set P(k) admits the natural decomposition P(k), P(k),, P(k) } {{, P ( k), P(k),, P(k) } } {{ }, k k where P(k) b b m := {a = a a P(k) : a i = b i, for i m}, so the natural partition of F(k) is given by the image under the map ξ k of the elements of the natural decomposition of P(k). From Theorem we would expect that the dynamical system (F(3), S 3 ) is semiconjugate to (R(2), F 2 ); however, this is not true, since the map φ 3 does not preserves the identification of points under the map ξ 2. For example, consider a = and a = ; they are mapped
14 INTEGERS: B (2) 4 Figure 9: At the left the set F(3) and its partition; at the right the image of the partition under S 3. to the same point in F(3), ξ 3 (a) = ξ 3 (a ); cf. [24] or [6]. However φ 3 (a) = and φ 3 (a ) =, and their images under ξ 2 are different points in R(2), since a necessary condition for points in R(2) to be mapped to the same point under ξ 2 is that their sequences are eventually periodic of the form. (iv) The involution Ψ allows us to define an equivalent relation in F(3). In Theorem 2 of [6], necessary and sufficient conditions are given when two points of R(3) are mapped to the same point in R(3) under the map ξ 3. These conditions are invariant under the involution Ψ, so if a and a P(3), such that ξ 3 (a) = ξ 3 (a ), then ξ 3 (Ψ(a)) = ξ 3 (Ψ(a )). So the set F(3) := ξ 3 ( P(3) / Ψ ) and the map S 3 := S 3/ Ψ are well-defined. The natural decomposition of F(3) induces a natural decomposition on the set F(3): { F(3), F(3) } where F(3) = ξ 3 ( P(3) / Ψ ) = ξ 3 ( P(3) / Ψ ) and F(3) = ξ 3 ( P(3) / Ψ ) = ξ 3 ( P(3) / Ψ ). (v) The set P(3) / Ψ admits the partition {( P(3) / Ψ ), ( P(3) / Ψ ) }, where ( P(3) / Ψ ) = P(3) / Ψ = P(3) / Ψ, ( P(3) / Ψ ) = P(3) / Ψ = P(3) / Ψ. These sets can be obtained as images of the maps H j : P(3) P(3), for j =,, where Ψ(a) if a = Ψ(a) if a = H (a) :=, H (a) := Ψ(a) if a = Ψ(a) if a =. These maps are well-defined since H j (a) is a path in the automaton A(3) Â(3), for a P(3). It can be easily checked that φ 3 (H (a)) = φ 3 (a) and
15 INTEGERS: B (2) 5 φ 3 (H (a)) = φ 3 (a). So the maps {φ 3 H, φ 3 H } define the iterated function system (IFS) [9], whose fixed point is R(2) [23]. This construction generalizes in a straightforward manner to P(k), for k 3. The partition { F(3), F(3) } of the set F(3) given in remark (iv) can be obtained as follows: F(3)j = G j (P(3)), where G j = ξ 3 H j, for j =,. Using techniques of fractal geometry it can be proved that M s ( F(3) )/M s ( F(3) ) = ( 5 )/2, where M s is the s-dimensional Hausdorff measure and s is the Hausdorff measure of F(3); for more details see [23]. Hence the ratio M s ( F(3) )/M s ( F(3) ) is equal to m(r(2) )/m(r(2) ), where m is the - dimensional Lebesgue measure. Proposition 6. The dynamical system ( F(3), S 3 ) exchanges the elements of the partition { F(3), F(3) }. Proof. Let F(3) := ξ 3 ( P(3) / Ψ ) = ξ 3 ( P(3) / Ψ ) F(3) := ξ 3 ( P(3) / Ψ ) = ξ 3 ( P(3) / Ψ ). and So { F(3), F(3) } is a partition of F(3). follows that By the symbolic dynamics, it S 3 ( F(3) ) = F(3), S3 ( F(3) ) F(3) and S3 ( F(3) ) F(3). So the action of S 3 on the natural decomposition of F(3) is a permutation of its elements. Using the same ideas we can generalize the previous result to F(k), for k 3. So in a similar manner we define the dynamical system ( F(k), S k ). Proposition 7. Let k 3. The dynamical system ( F(k), S k ) acts as a permutation on the k pieces of the natural partition of F(k). While we have shown that (F(3), S 3 ) is not semi-conjugate to the dynamical system (R(2), F 2 ); hence ( F(3), S 3 ) is not conjugate to (R(2), F 2 ). We pointed out the behaviour of the system ( F(3), S 3 ) resembles the system (R(2), F 2 ), from the metrical and dynamical point of view. (vi) We would like to remark that if we consider the automaton of paths of length l, with l >, of the k-bonacci system, we obtain the same set P(k) as the maximal invariant subset of R(k) under the mirror involution. In fact: Let
16 INTEGERS: B (2) 6 C(l, k) be the automaton of paths of length l from A(k), the k-bonacci automaton. The set of infinite paths on C(l, k) is the same set as the set of infinite paths on A(k), i.e., R(k). The transition matrix of the automaton C(k, k) is calculated in [22]. The labels of C(l, k) are words of length l in W = {, }. So we can consider the dual automaton of C(l, k) and get its canonical product. Let P(l, k) be the set of infinite paths on the canonical product of C(l, k). Since P(l, k) and P(k) are, by construction, the maximal invariant set of R(k) under the the mirror involution, we get P(l, k) = P(k). (vii) Here we shall consider the domain exchange transformation on R(k) and its relation on the domain exchange transformation on R(k). Let {R(k),..., R(k) k } be the natural decomposition of R(k) defined in (), i.e., R(k) j = ξ k (R(k) j ), where R(k) j := a R(k) : a = } {{ }. j Let R(k) j := ξ k ( R(k) j ), so the natural decomposition of R(k) is { R(k),..., R(k) k }. Let ψ k : R k R k be the reflection map by the center of symmetry of R(k), mentioned in Remark (i), i.e., ψ k (x) = 2ω k x, where ω k is the center of symmetry of R(k) described in Corollary 4. According to the proof of this corollary, ξ k (â) = 2ω k ξ k (a) = ψ k (ξ x (a)), so R(k) j = ψ k (R(k) j ). In Section 4 we introduced F k, the piece exchange map on R(k), so that the diagram (2) commutes. Since in R(k) there is an adic map T k, it induces a map on R(k) so that the following diagram is commutative: R(k) ξ k T k R(k) F k R(k) ξ k R(k). In Section 2 we pointed out that the dual adic map relates to the adic map, so that T ( T (â)) = a, or equivalently T ( T (a)) = â. Hence, Fk (ψ k ( F k (ψ k (x)))) = x for any x R(k). Therefore F k ( R(k) j ) = ψ k (F k (R(k) j). We can conclude that the map F k is a piece exchange on the decomposition { R(k),..., R(k) k } of R(k).
17 INTEGERS: B (2) 7 By Theorem 3 we have that R(k) = R(k). We can conclude that there are two decompositions on this set, that define different piece exchange transformations. They are related by the symmetry map ψ k. Acknowledgement The author is grateful to the referee whose comments helped to improve the previous version of this paper. References [] P. Arnoux and S. Ito, Pisot substitutions and Rauzy fractals, Bull. Belg. Math. Soc. Simon Stevin 8 (2), [2] V. Berthé and A. Siegel, Tilings associated with beta-numeration and substitutions, Integers 5(3) (25), #A2. [3] S. Bezuglyi, J. Kwiatkowski, K. Medynets and B. Solomyak, Invariant measures on stationary Bratteli diagrams, Ergodic Theory and Dynam. Syst. 3 (2), [4] A. Brauer, On algebraic equations with all but one root in the interior of the unit circle, Math. Nachr. 4 (95), [5] V. Canterini and A. Siegel, Geometric representation of substitutions of Pisot type, Trans. Amer. Math. Soc. 353 (2), [6] J.M. Dumont and A. Thomas, Systèmes de numération et fonctions fractales relatifs aux substitutions, Theoret. Comput. Sci. 65 (989), [7] F. Durand, B. Host and C. Skau, Substitutional dynamical systems, Bratteli diagrams and dimension groups, Ergod. Th. Dynam. Systems 9 (999), [8] S. Eilenberg, Automata, languages and machines, Academic Press, New York, 974. [9] K. Falconer, Fractal Geometry. Mathematical Foundations and Applications, John Willey & Sons, Chichester, 99. [] C. Frougny, Representations of numbers and finite automata, Math. Systems Theory 25 (992), [] P.J. Grabner, P. Liardet and R. Tichy, Odometers and systems of numeration, Acta Arithmetica 7 (995), [2] C. Holton and L. Zamboni, Geometric realization of substitutions, Bull. Soc. Math. France 26 (998), [3] B. Host, Substitution subshifts and Bratteli diagrams, in: Topics in Symbolic Dynamics and Applications, London Mathematical Society Lecture Note Series 279, Cambridge University Press, Cambridge, 2, pp [4] S. Ito and M. Kimura, On the Rauzy fractal, Japan J. Indust. Appl. Math. 8 (99),
18 INTEGERS: B (2) 8 [5] D. Lind and B. Marcus, An Introduction to Symbolic Dynamics and Coding, Cambridge University Press, Cambridge, 995. [6] A. Messaoudi, Propriétés arithmétiques et dynamiques du fractal de Rauzy, J. Th. Nombres Bordeaux (998), [7] N. Pytheas Fogg, Substitutions in Dynamics, Arithmetics and Combinatorics, (edited by V. Berthé, S. Ferenczi, C. Mauduit, et al.), Lecture Notes in Mathematics 794, Springer, Berlin, 22. [8] M. Queffélec, Substitution Dynamical Systems Spectral Analysis, Lecture Notes in Mathematics 294, Springer, Berlin, 987. [9] G. Rauzy, Nombres algébriques et substitutions, Bull. Soc. Math. France (982), [2] G. Rauzy, Sequences defined by iterated morphisms, in: R.M. Capocelli (ed.), Sequences Springer, New York, 99, pp [2] B. Sing and V.F. Sirvent, Geometry of the common dynamics of flipped Pisot substitutions, Monatshefte für Mathematik 55 (28), [22] V.F. Sirvent, Relationships between the dynamical systems associated to the Rauzy substitutions, Theoretical Computer Science 64 (996), [23] V.F. Sirvent, On some dynamical subsets of the Rauzy Fractal, Theoretical Computer Science 8 (997), [24] V.F. Sirvent, Identifications and dimension of the Rauzy Fractal, Fractals 5 (997), [25] V.F. Sirvent, The common dynamics of the flipped tribonacci substitutions, Bull. Belg. Math. Soc. Simon Stevin 7 (2), [26] V.F. Sirvent and Y. Wang, Self-affine tilings via substitution dynamical systems and Rauzy fractals, Pacific Journal of Mathematics, 26 (22), [27] B. Solomyak, On the spectral theory of adic transformations, Advances in Soviet Mathematics, 9 (992), [28] B. Solomyak and A. Vershik, The adic realization of the Morse transformation and the extension of its action on the solenoid, Zapiski Nauchn. Semin. POMI 36 (28), 7-9. [29] J. Thuswaldner, Unimodular Pisot substitutions and their associated tiles, J. Th. Nombres Bordeaux 8 (26), [3] A.M. Vershik and A.N. Livshits, Adic models of ergodic transformations, spectral theory, substitutions, and related topics, in: Representation Theory and Dynamical Systems, Advances in Soviet Mathematics 9, American Mathematical Society, Providence, RI, 992, pp
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