On the topology of discrete hyperplanes∗ D. Jamet [email protected] We deal with the connectedness of discrete hyperplanes H(v, µ, ω) = {x ∈ Zn | 0 ≤ hv, x < ωi} with v ∈ Rn , µ ∈ R and ω ∈ R. Given a vector v and an intersect µ ∈ R, the question we investigate is how to calculate Ω(v, µ) = inf {ω ∈ R | H(v, µ, ω) is connected} of R Let S be a subset of Z, let us recall that a path in S is a finite sequence π = (x1 , . . . , xk ) such that xi ∈ S for every i ∈ {1, . . . , k} and d (xi , xi+1 ) = 1, for every i ∈ {1, . . . , k}, where d denotes Euclidean distance. One says that the path π = (x1 , . . . , xk ) links x1 to xk . The set S is connected if, for each pair (x, y), there exists a path π = (x1 , . . . , xk ) in S linking x to y. The first result we present is an algorithm allowing us to compute Ω(v, µ). This algorithm is already known as the fully subtractive algorithm [5] and has already been studied in [3, 4] in case of percolations models defined by rotations. It has been proved that the convergence set of the fully subtractive algorithm has Lebesgue-measure zero [3, 4, 2]. A direct consequence is the almost sure finiteness of the algorithm computing Ω(v, µ). A natural question follows : what about the connectdness of H (v, µ, ω) at the critical value ω = Ω(v, µ)? Since H (v, µ, Ω(v, µ)) is connected only if the fully subtractive algorithm is convergent on the entry v, it becomes natural to consider such a vector. Let α be the unique real eigenvalue of the matrix   −1 1 0 M3 = −1 0 1 1 0 0 and let v = αe1 + (α + α2 )e2 + e3 be the associated eigenvector. Then one computes, for each µ ∈ R, 1+α Ω(v, µ) = . α Let (tn )n∈N be a sequence of integer vectors satisfying htn , vi = αn and let Pn be a sequence of subsets of Z3 defined as follows (see Figure 1):  3 P : Z −→ P Z P = {(0, 0, 0)} if n = 0, n 7−→ n Pn = Pn−1 ∪ (Pn−1 + tn ) if n > 0

−→

−→

−→

−→

−→

−→

Figure 1: Step by step construction of Pn It follows that, for all n ≥ 0, the set Pn is connected and is a tree. Moreover, the set Pn \ {0} has exactly 3 connected components (see Figure 2) ∗ Joint work with J.-L. Toutant (ISIT, Clermont-Ferrand), E. Domenjoud (Loria, Nancy), V. Berthé (Liafa, Paris 7) and X. Provençal (Lama, Chambéry)

1

Figure 2: The three connected components of P14 \ {0} in three different colors   1+α It is easy to see that, for all n ∈ N, Pn ⊆ H v, 0, . The other inclusion is a consequence of [1] α   1+α −1 −3 −2 −1 which states that Fin(α ) = Z[α], since α − α − α − 1 = 0. It follows that the set H v, 0, α   1+α is a connected, is a tree and the set H v, 0, \ {0} has exactly 3 connected components. α   1+α The last problem we investigate is the role of µ in the connectedness of H v, µ, and we show that α     1+α 1+α 1+α the discrete plane H v, , is not connected since it is a symmetric of the set H v, µ, \ α α α {0}.

References [1] Christiane Frougny and Boris Solomyak. Finite beta-expansions. Ergodic Theory Dynam. Systems, 12(4):713–723, 1992. [2] Cor Kraaikamp and Ronald Meester. Ergodic properties of a dynamical system arising from percolation theory. Ergodic Theory Dynam. Systems, 15(4):653–661, 1995. [3] Ronald W. J. Meester. An algorithm for calculating critical probabilities and percolation functions in percolation models defined by rotations. Ergodic Theory Dynam. Systems, 9(3):495–509, 1989. [4] Ronald W. J. Meester and Tomasz Nowicki. Infinite clusters and critical values in two-dimensional circle percolation. Israel J. Math., 68(1):63–81, 1989. [5] F. Schweiger. Multidimensional Continued Fractions. Oxford Science Publications. Oxford University Press, 2000.

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On the topology of discrete hyperplanes

[1] Christiane Frougny and Boris Solomyak. Finite beta-expansions. Ergodic Theory Dynam. Systems,. 12(4):713–723, 1992. [2] Cor Kraaikamp and Ronald Meester. Ergodic properties of a dynamical system arising from percolation theory. Ergodic Theory Dynam. Systems, 15(4):653–661, 1995. [3] Ronald W. J. Meester.

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