Emmanuel Amiot Modèles algébriques et algorithmes pour la ...
Emmanuel Amiot Modèles algébriques et algorithmes pour la ...
Emmanuel Amiot Modèles algébriques et algorithmes pour la ...
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12<br />
10<br />
8<br />
6<br />
4<br />
2<br />
4<br />
0<br />
ME7,3<br />
4<br />
alternative title 11<br />
2<br />
12<br />
10<br />
Figure 4. Maximizing for B is maximizing for A<br />
8<br />
6<br />
4<br />
2<br />
ME28,12<br />
(0 2 4)<br />
4 8 12 16 20 24<br />
From the equations (k + d ′ )c<br />
kc<br />
=<br />
d d + d′ c<br />
kc <br />
= + c ′ , we conclude first that A is a disjoint<br />
d d<br />
union of m trans<strong>la</strong>tes of the s<strong>et</strong> B = { kc <br />
, k = 0 . . . d ′ − 1}, with multiples of c ′ as disp<strong>la</strong>cements, i.e.<br />
d<br />
A = B ⊔ c ′ + B ⊔ ... ⊔ (m − 1)c ′ + B. Thus, each element in the multis<strong>et</strong> πd(A) has multiplicity m. It<br />
remains to be shown that πd(B) is a contiguous cluster.<br />
We will use the fact that the fractional parts of the rational numbers kc<br />
d<br />
= kc′<br />
d ′ take d′ different values<br />
when k runs from 0 to d ′ − 1. This is true because c ′ and d ′ are coprime. To see this choose 0 ≤ k, k ′ < d ′ :<br />
k ′ c ′ kc′<br />
−<br />
d ′ d ′ = n ∈ Z ⇒ (k′ − k)c ′ = d ′ n ⇒ d ′ | (k ′ − k) ⇒ k ′ = k as |k ′ − k| < d ′<br />
From the d ′ different fractional parts 0 ≤ kc′ ′<br />
−kc<br />
d ′ d ′<br />
kc ′<br />
< 1 we obtain d ′ different integers 0 ≤ kc ′ −d ′<br />
d ′<br />
<br />
≤<br />
d ′ − 1, which are in fact all the integers 0, ..., d ′ . Reduction of the elements kc ′ ′<br />
− d ′kc<br />
d ′<br />
<br />
modulo c ′ yields<br />
the s<strong>et</strong> −πd(B) = −d ′ B mod c ′ . Thus πd(B) is a cluster, namely πd(B) = {c ′ − d ′ + 1, c ′ − d ′ + 2, ..., c ′ }. <br />
3 Generated S<strong>et</strong>s and Groups Generated by a S<strong>et</strong><br />
The Fourier approach offers further directions of investigation. Here we restrict ourselves to maximality<br />
conditions for the absolute values for Fourier coefficients. As we have seen in Section 2 it is the index<br />
d ∈ Zc, i.e. the residue c<strong>la</strong>ss of the chords cardinality to which the maximality condition for maximal<br />
evenness is attached.