This paper was converted on www.awesomepapers.org from LaTeX by an anonymous user.
Want to know more? Visit the Converter page.

A note on affinely regular polygons

Christian Huck Department of Mathematics and Statistics
The Open University
Walton Hall
Milton Keynes
MK7 6AA
United Kingdom
c.huck@open.ac.uk
Abstract.

The affinely regular polygons in certain planar sets are characterized. It is also shown that the obtained results apply to cyclotomic model sets and, additionally, have consequences in the discrete tomography of these sets.

The author was supported by the German Research Council (Deutsche Forschungsgemeinschaft), within the CRC 701, and by EPSRC via Grant EP/D058465/1.

1. Introduction

Chrestenson [6] has shown that any (planar) regular polygon whose vertices are contained in d\mathbbm{Z}^{d} for some d2d\geq 2 must have 3,43,4 or 66 vertices. More generally, Gardner and Gritzmann [9] have characterized the numbers of vertices of affinely regular lattice polygons, i.e., images of non-degenerate regular polygons under a non-singular affine transformation of the plane whose vertices are contained in the square lattice 2\mathbbm{Z}^{2} or, equivalently, in some arbitrary planar lattice LL. It turned out that the affinely regular lattice polygons are precisely the affinely regular triangles, parallelograms and hexagons. As a first step beyond the case of planar lattices, this short text provides a generalization of this result to planar sets Λ\varLambda that are non-degenerate in some sense and satisfy a certain affinity condition on finite scales (Theorem 3.3). The obtained characterization can be expressed in terms of a simple inclusion of real field extensions of \mathbbm{Q} and particularly applies to algebraic Delone sets, thus including cyclotomic model sets. These cyclotomic model sets range from periodic examples, given by the vertex sets of the square tiling and the triangular tiling, to aperiodic examples like the vertices of the Ammann-Beenker tiling, of the Tübingen triangle tiling and of the shield tiling, respectively. I turns out that, for cyclotomic model sets Λ\varLambda, the numbers of vertices of affinely regular polygons in Λ\varLambda can be characterized by a simple divisibility condition (Corollary 4.1). In particular, the result on affinely regular lattice polygons is contained as a special case (Corollary 4.2(a)). Additionally, it is shown that the obtained divisibility condition implies a weak estimate in the discrete tomography of cyclotomic model sets (Corollary 5.5).

2. Preliminaries and notation

Natural numbers are always assumed to be positive, i.e., ={1,2,3,}\mathbbm{N}\,=\,\{1,2,3,\dots\} and we denote by 𝒫\mathcal{P} the set of rational primes. If k,lk,l\in\mathbbm{N}, then gcd(k,l)\operatorname{gcd}(k,l) and lcm(k,l)\operatorname{lcm}(k,l) denote their greatest common divisor and least common multiple, respectively. The group of units of a given ring RR is denoted by R×R^{\times}. As usual, for a complex number zz\in\mathbbm{C}, |z||z| denotes the complex absolute value, i.e., |z|=zz¯|z|=\sqrt{z\bar{z}}, where .¯\bar{.} denotes the complex conjugation. The unit circle in 2\mathbbm{R}^{2} is denoted by 𝕊1\mathbb{S}^{1}, i.e., 𝕊1={x2||x|=1}\mathbb{S}^{1}=\{x\in\mathbbm{R}^{2}\,|\,|x|=1\}. Moreover, the elements of 𝕊1\mathbb{S}^{1} are also called directions. For r>0r>0 and x2x\in\mathbbm{R}^{2}, Br(x)B_{r}(x) denotes the open ball of radius rr about xx. A subset Λ\varLambda of the plane is called uniformly discrete if there is a radius r>0r>0 such that every ball Br(x)B_{r}(x) with x2x\in\mathbbm{R}^{2} contains at most one point of Λ\varLambda. Further, Λ\varLambda is called relatively dense if there is a radius R>0R>0 such that every ball BR(x)B_{R}(x) with x2x\in\mathbbm{R}^{2} contains at least one point of Λ\varLambda. Λ\varLambda is called a Delone set (or Delaunay set) if it is both uniformly discrete and relatively dense. For a subset SS of the plane, we denote by card(S)\operatorname{card}(S), (S)\mathcal{F}(S), conv(S)\operatorname{conv}(S) and 𝟙S\mathbbm{1}_{S} the cardinality, set of finite subsets, convex hull and characteristic function of SS, respectively. A direction u𝕊1u\in\mathbb{S}^{1} is called an SS-direction if it is parallel to a non-zero element of the difference set SS:={ss|s,sS}S-S:=\{s-s^{\prime}\,|\,s,s^{\prime}\in S\} of SS. Further, a finite subset CC of SS is called a convex subset of SS if its convex hull contains no new points of SS, i.e., if C=conv(C)SC=\operatorname{conv}(C)\cap S holds. Moreover, the set of all convex subsets of SS is denoted by 𝒞(S)\mathcal{C}(S). Recall that a linear transformation (resp., affine transformation) Ψ:22\Psi\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} of the Euclidean plane is given by zAzz\mapsto Az (resp., zAz+tz\mapsto Az+t), where AA is a real 2×22\times 2 matrix and t2t\in\mathbbm{R}^{2}. In both cases, Ψ\Psi is called singular when det(A)=0\operatorname{det}(A)=0; otherwise, it is non-singular. A homothety h:22h\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} is given by zλz+tz\mapsto\lambda z+t, where λ\lambda\in\mathbbm{R} is positive and t2t\in\mathbbm{R}^{2}. A convex polygon is the convex hull of a finite set of points in 2\mathbbm{R}^{2}. For a subset S2S\subset\mathbbm{R}^{2}, a polygon in SS is a convex polygon with all vertices in SS. A regular polygon is always assumed to be planar, non-degenerate and convex. An affinely regular polygon is a non-singular affine image of a regular polygon. In particular, it must have at least 33 vertices. Let U𝕊1U\subset\mathbb{S}^{1} be a finite set of directions. A non-degenerate convex polygon PP is called a UU-polygon if it has the property that whenever vv is a vertex of PP and uUu\in U, the line uv\ell_{u}^{v} in the plane in direction uu which passes through vv also meets another vertex vv^{\prime} of PP. For a subset Λ\varLambda\subset\mathbbm{C}, we denote by 𝕂Λ\mathbbm{K}_{\varLambda} the intermediate field of /\mathbbm{C}/\mathbbm{Q} that is given by

𝕂Λ:=((ΛΛ)(ΛΛ¯)),\mathbbm{K}_{\varLambda}\,\,:=\,\,\mathbbm{Q}\left(\big{(}\varLambda-\varLambda\big{)}\cup\big{(}\overline{\varLambda-\varLambda}\big{)}\right)\,,

where ΛΛ\varLambda-\varLambda denotes the difference set of Λ\varLambda. Further, we set 𝕜Λ:=𝕂Λ\mathbbm{k}_{\varLambda}:=\mathbbm{K}_{\varLambda}\cap\mathbbm{R}, the maximal real subfield of 𝕂Λ\mathbbm{K}_{\varLambda}.

Remark 2.1.

Note that UU-polygons have an even number of vertices. Moreover, an affinely regular polygon with an even number of vertices is a UU-polygon if and only if each direction of UU is parallel to one of its edges.

For nn\in\mathbbm{N}, we always let ζn:=e2πi/n\zeta_{n}:=e^{2\pi i/n}, as a specific choice for a primitive nnth root of unity in \mathbbm{C}. Let (ζn)\mathbbm{Q}(\zeta_{n}) be the corresponding cyclotomic field. It is well known that (ζn+ζ¯n)\mathbbm{Q}(\zeta_{n}+\bar{\zeta}_{n}) is the maximal real subfield of (ζn)\mathbbm{Q}(\zeta_{n}); see [17]. Throughout this text, we shall use the notation

𝕂n=(ζn),𝕜n=(ζn+ζ¯n),𝒪n=[ζn],𝒪=n[ζn+ζ¯n].\mathbbm{K}_{n}=\mathbbm{Q}(\zeta_{n}),\;\mathbbm{k}_{n}=\mathbbm{Q}(\zeta_{n}+\bar{\zeta}_{n}),\;\mathcal{O}_{n}=\mathbbm{Z}[\zeta_{n}],\;\thinspace\scriptstyle{\mathcal{O}}{}_{n}=\mathbbm{Z}[\zeta_{n}+\bar{\zeta}_{n}]\,.

Except for the one-dimensional cases 𝕂1=𝕂2=\mathbbm{K}_{1}=\mathbbm{K}_{2}=\mathbbm{Q}, 𝕂n\mathbbm{K}_{n} is an imaginary extension of \mathbbm{Q}. Further, ϕ\phi will always denote Euler’s phi-function, i.e.,

ϕ(n)=card({k| 1kn and gcd(k,n)=1}).\phi(n)=\operatorname{card}\left(\big{\{}k\in\mathbbm{N}\,|\,1\leq k\leq n\textnormal{ and }\operatorname{gcd}(k,n)=1\big{\}}\right)\,.

Occasionally, we identify \mathbbm{C} with 2\mathbbm{R}^{2}. Primes p𝒫p\in\mathcal{P} for which the number 2p+12p+1 is prime as well are called Sophie Germain prime numbers. We denote by 𝒫SG\mathcal{P}_{\rm SG} the set of Sophie Germain prime numbers. They are the primes pp such that the equation ϕ(n)=2p\phi(n)=2p has solutions. It is not known whether there are infinitely many Sophie Germain primes. The first few are

{2,3,5,11,23,29,41,53,83,89,113,131,173,\displaystyle\{2,3,5,11,23,29,41,53,83,89,113,131,173,
179,191,233,239,251,281,293,359,419,},\displaystyle\hphantom{\{}179,191,233,239,251,281,293,359,419,\dots\}\,,

see entry A005384 of [16] for further details. We need the following facts from the theory of cyclotomic fields.

Fact 2.2 (Gauß).

[17, Theorem 2.5] [𝕂n:]=ϕ(n)[\mathbbm{K}_{n}:\mathbbm{Q}]=\phi(n). The field extension 𝕂n/\mathbbm{K}_{n}/\mathbbm{Q} is a Galois extension with Abelian Galois group G(𝕂n/)(/n)×G(\mathbbm{K}_{n}/\mathbbm{Q})\simeq(\mathbbm{Z}/n\mathbbm{Z})^{\times}, where a(modn)a\,(\textnormal{mod}\,n) corresponds to the automorphism given by ζnζna\zeta_{n}\mapsto\zeta_{n}^{a}.

Since 𝕜n\mathbbm{k}_{n} is the maximal real subfield of the nnth cyclotomic field 𝕂n\mathbbm{K}_{n}, Fact 2.2 immediately gives the following result.

Corollary 2.3.

If n3n\geq 3, one has [𝕂n:𝕜n]=2[\mathbbm{K}_{n}:\mathbbm{k}_{n}]=2. Thus, a 𝕜n\mathbbm{k}_{n}-basis of 𝕂n\mathbbm{K}_{n} is given by {1,ζn}\{1,\zeta_{n}\}. The field extension 𝕜n/\mathbbm{k}_{n}/\mathbbm{Q} is a Galois extension with Abelian Galois group G(𝕜n/)(/n)×/{±1(modn)}G(\mathbbm{k}_{n}/\mathbbm{Q})\simeq(\mathbbm{Z}/n\mathbbm{Z})^{\times}/\{\pm 1\,(\textnormal{mod}\,n)\} of order [𝕜n:]=ϕ(n)/2[\mathbbm{k}_{n}:\mathbbm{Q}]=\phi(n)/2.

Consider an algebraic number field 𝕂\mathbbm{K}, i.e., a finite extension of \mathbbm{Q}. A full \mathbbm{Z}-module 𝒪\mathcal{O} in 𝕂\mathbbm{K} (i.e., a free \mathbbm{Z}-module of rank [𝕂:][\mathbbm{K}:\mathbbm{Q}]) which contains the number 11 and is a ring is called an order of 𝕂\mathbbm{K}. Note that every \mathbbm{Z}-basis of 𝒪\mathcal{O} is simultaneously a \mathbbm{Q}-basis of 𝕂\mathbbm{K}, whence 𝒪=𝕂\mathbbm{Q}\mathcal{O}=\mathbbm{K} in particular. It turns out that among the various orders of 𝕂\mathbbm{K} there is one maximal order which contains all the other orders, namely the ring of integers 𝒪𝕂\mathcal{O}_{\mathbbm{K}} in 𝕂\mathbbm{K}; see [5, Chapter 2, Section 2]. For cyclotomic fields, one has the following well-known result.

Fact 2.4.

[17, Theorem 2.6 and Proposition 2.16] For nn\in\mathbbm{N}, one has:

  • (a)

    𝒪n\mathcal{O}_{n} is the ring of cyclotomic integers in 𝕂n\mathbbm{K}_{n}, and hence its maximal order.

  • (b)

    𝒪n\thinspace\scriptstyle{\mathcal{O}}{}_{n} is the ring of integers in 𝕜n\mathbbm{k}_{n}, and hence its maximal order.

Lemma 2.5.

If m,nm,n\in\mathbbm{N}, then 𝕂m𝕂n=𝕂gcd(m,n)\mathbbm{K}_{m}\cap\mathbbm{K}_{n}=\mathbbm{K}_{\operatorname{gcd}(m,n)}.

Proof.

The assertion follows from similar arguments as in the proof of the special case (m,n)=1(m,n)=1; compare [15, Ch. VI.3, Corollary 3.2]. Here, one has to observe (ζm,ζn)=𝕂m𝕂n=𝕂lcm(m,n)\mathbbm{Q}(\zeta_{m},\zeta_{n})=\mathbbm{K}_{m}\mathbbm{K}_{n}=\mathbbm{K}_{\operatorname{lcm}(m,n)} and then to employ the identity

(1) ϕ(m)ϕ(n)=ϕ(lcm(m,n))ϕ(gcd(m,n))\phi(m)\phi(n)=\phi(\operatorname{lcm}(m,n))\phi(\operatorname{gcd}(m,n))

instead of merely using the multiplicativity of the arithmetic function ϕ\phi. ∎

Lemma 2.6.

Let m,nm,n\in\mathbbm{N}. The following statements are equivalent:

  • (i)

    𝕂m𝕂n\mathbbm{K}_{m}\subset\mathbbm{K}_{n}.

  • (ii)

    m|nm|n, or m 2(mod4)m\;\equiv\;2\;(\operatorname{mod}4) and m|2nm|2n.

Proof.

For direction (ii) \Rightarrow (i), the assertion is clear if m|nm|n. Further, if m 2(mod4)m\;\equiv\;2\;(\operatorname{mod}4), say m=2om=2o for a suitable odd number oo, and m|2nm|2n, then 𝕂o𝕂n\mathbbm{K}_{o}\subset\mathbbm{K}_{n} (due to o|no|n). However, Fact 2.2 shows that the inclusion of fields 𝕂o𝕂2o=𝕂m\mathbbm{K}_{o}\subset\mathbbm{K}_{2o}=\mathbbm{K}_{m} cannot be proper since we have, by means of the multiplicativity of ϕ\phi, the equation ϕ(m)=ϕ(2o)=ϕ(o)\phi(m)=\phi(2o)=\phi(o). This gives 𝕂m𝕂n\mathbbm{K}_{m}\subset\mathbbm{K}_{n}.

For direction (i) \Rightarrow (ii), suppose 𝕂m𝕂n\mathbbm{K}_{m}\subset\mathbbm{K}_{n}. Then, Lemma 2.5 implies 𝕂m=𝕂gcd(m,n)\mathbbm{K}_{m}=\mathbbm{K}_{\operatorname{gcd}(m,n)}, whence

(2) ϕ(m)=ϕ(gcd(m,n))\phi(m)=\phi(\operatorname{gcd}(m,n))\,

by Fact 2.2 again. Using the multiplicativity of ϕ\phi together with ϕ(pj)=pj1(p1)\phi(p^{j})\,=\,p^{j-1}\,(p-1) for p𝒫p\in\mathcal{P} and jj\in\mathbbm{N}, we see that, given the case gcd(m,n)<m\operatorname{gcd}(m,n)<m, Equation (2) can only be fulfilled if m 2(mod4)m\;\equiv\;2\;(\operatorname{mod}4) and m|2nm|2n. The remaining case gcd(m,n)=m\operatorname{gcd}(m,n)=m is equivalent to the relation m|nm|n. ∎

Corollary 2.7.

Let m,nm,n\in\mathbbm{N}. The following statements are equivalent:

  • (i)

    𝕂m=𝕂n\mathbbm{K}_{m}=\mathbbm{K}_{n}.

  • (ii)

    m=nm=n, or mm is odd and n=2mn=2m, or nn is odd and m=2nm=2n.

Remark 2.8.

Corollary 2.7 implies that, for m,n 2(mod4)m,n\;\not\equiv\;2\;(\operatorname{mod}4), one has the identity 𝕂m=𝕂n\mathbbm{K}_{m}=\mathbbm{K}_{n} if and only if m=nm=n.

Lemma 2.9.

Let m,nm,n\in\mathbbm{N} with m,n3m,n\geq 3. Then, one has:

  • (a)

    𝕜m=𝕜n𝕂m=𝕂n or m,n{3,4,6}.\mathbbm{k}_{m}=\mathbbm{k}_{n}\;\Leftrightarrow\;\mathbbm{K}_{m}=\mathbbm{K}_{n}\mbox{ or\, }m,n\in\{3,4,6\}.

  • (b)

    𝕜m𝕜n𝕂m𝕂n or m{3,4,6}.\mathbbm{k}_{m}\subset\mathbbm{k}_{n}\;\Leftrightarrow\;\mathbbm{K}_{m}\subset\mathbbm{K}_{n}\mbox{ or\, }m\in\{3,4,6\}.

Proof.

For claim (a), let us suppose 𝕜m=𝕜n=:𝕜\mathbbm{k}_{m}=\mathbbm{k}_{n}=:\mathbbm{k} first. Then, Fact 2.2 and Corollary 2.3 imply that [𝕂m:𝕜]=[𝕂n:𝕜]=2[\mathbbm{K}_{m}:\mathbbm{k}]=[\mathbbm{K}_{n}:\mathbbm{k}]=2. Note that 𝕂m𝕂n=𝕂gcd(m,n)\mathbbm{K}_{m}\cap\mathbbm{K}_{n}=\mathbbm{K}_{\operatorname{gcd}(m,n)} is a cyclotomic field containing 𝕜\mathbbm{k}. It follows that either 𝕂m𝕂n=𝕂gcd(m,n)=𝕂m=𝕂n\mathbbm{K}_{m}\cap\mathbbm{K}_{n}=\mathbbm{K}_{\operatorname{gcd}(m,n)}=\mathbbm{K}_{m}=\mathbbm{K}_{n} or 𝕂m𝕂n=𝕂gcd(m,n)=𝕜\mathbbm{K}_{m}\cap\mathbbm{K}_{n}=\mathbbm{K}_{\operatorname{gcd}(m,n)}=\mathbbm{k} and hence 𝕜m=𝕜n=𝕜=\mathbbm{k}_{m}=\mathbbm{k}_{n}=\mathbbm{k}=\mathbbm{Q}, since the latter is the only real cyclotomic field. Now, this implies m,n{3,4,6}m,n\in\{3,4,6\}; see also Lemma 2.10(a) below. The other direction is obvious. Claim (b) follows immediately from the part (a). ∎

Lemma 2.10.

Consider ϕ\phi on {n|n 2(mod4)}\{n\in\mathbbm{N}\,|\,n\;\not\equiv\;2\;(\operatorname{mod}4)\}. Then, one has:

  • (a)

    ϕ(n)/2=1\phi(n)/2=1 if and only if n{3,4}n\in\{3,4\}.

  • (b)

    ϕ(n)/2𝒫\phi(n)/2\in\mathcal{P} if and only if n𝒮:={8,9,12}{2p+1|p𝒫SG}n\in\mathcal{S}:=\{8,9,12\}\cup\{2p+1\,|\,p\in\mathcal{P}_{\rm SG}\}.

Proof.

The equivalences follow from the multiplicativity of ϕ\phi in conjunction with the identity ϕ(pj)=pj1(p1)\phi(p^{j})\,=\,p^{j-1}\,(p-1) for p𝒫p\in\mathcal{P} and jj\in\mathbbm{N}. ∎

Remark 2.11.

Let n 2(mod4)n\;\not\equiv\;2\;(\operatorname{mod}4). By Corollary 2.3, for n3n\geq 3, the field extension 𝕜n/\mathbbm{k}_{n}/\mathbbm{Q} is a Galois extension with Abelian Galois group G(𝕜n/)G(\mathbbm{k}_{n}/\mathbbm{Q}) of order ϕ(n)/2\phi(n)/2. Using Lemma 2.10, one sees that G(𝕜n/)G(\mathbbm{k}_{n}/\mathbbm{Q}) is trivial if and only if n{1,3,4}n\in\{1,3,4\}, and simple if and only if n𝒮n\in\mathcal{S}, with 𝒮\mathcal{S} as defined in Lemma 2.10(b).

3. The characterization

The following notions will be of crucial importance.

Definition 3.1.

For a set Λ2\varLambda\subset\mathbbm{R}^{2}, we define the following properties:

  • (Alg)

    [𝕂Λ:]<\left[\mathbbm{K}_{\varLambda}:\mathbbm{Q}\right]<\infty.

  • (Aff)

    For all F(𝕂Λ)F\in\mathcal{F}(\mathbbm{K}_{\varLambda}), there is a non-singular affine transformation Ψ:22\Psi\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} such that h(F)Λh(F)\subset\varLambda.

Moreover, Λ\varLambda is called degenerate when 𝕂Λ\mathbbm{K}_{\varLambda}\subset\mathbbm{R}; otherwise, Λ\varLambda is non-degenerate.

Remark 3.2.

If Λ2\varLambda\subset\mathbbm{R}^{2} satisfies property (Alg), then one has [𝕜Λ:]<\left[\mathbbm{k}_{\varLambda}:\mathbbm{Q}\right]<\infty, i.e., 𝕜Λ\mathbbm{k}_{\varLambda} is a real algebraic number field.

Before we turn to examples of planar sets Λ\varLambda having properties (Alg) and (Aff), let us prove the central result of this text, where we use arguments similar to the ones used by Gardner and Gritzmann in the proof of [9, Theorem 4.1].

Theorem 3.3.

Let Λ2\varLambda\subset\mathbbm{R}^{2} be non-degenerate with property (Aff). Further, let mm\in\mathbbm{N} with m3m\geq 3. The following statements are equivalent:

  • (i)

    There is an affinely regular mm-gon in Λ\varLambda.

  • (ii)

    𝕜m𝕜Λ\mathbbm{k}_{m}\subset\mathbbm{k}_{\varLambda}.

If Λ\varLambda additionally fulfils property (Alg), then it only contains affinely regular mm-gons for finitely many values of mm.

Proof.

For (i) \Rightarrow (ii), let PP be an affinely regular mm-gon in Λ\varLambda. There is then a non-singular affine transformation Ψ:22\Psi\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} with Ψ(Rm)=P\Psi(R_{m})=P, where RmR_{m} is the regular mm-gon with vertices given in complex form by 1,ζm,,ζmm11,\zeta_{m},\dots,\zeta_{m}^{m-1}. If m{3,4,6}m\in\{3,4,6\}, condition (ii) holds trivially. Suppose 6m56\neq m\geq 5. The pairs {1,ζm}\{1,\zeta_{m}\}, {ζm1,ζm2}\{\zeta_{m}^{-1},\zeta_{m}^{2}\} lie on parallel lines and so do their images under Ψ\Psi. Therefore,

|ζm2ζm1||ζm1|=|Ψ(ζm2)Ψ(ζm1)||Ψ(ζm)Ψ(1)|.\frac{|\zeta_{m}^{2}-\zeta_{m}^{-1}|}{|\zeta_{m}-1|}=\frac{|\Psi(\zeta_{m}^{2})-\Psi(\zeta_{m}^{-1})|}{|\Psi(\zeta_{m})-\Psi(1)|}\,.

Moreover, since Ψ(ζm2)Ψ(ζm1)\Psi(\zeta_{m}^{2})-\Psi(\zeta_{m}^{-1}) and Ψ(ζm)Ψ(1)\Psi(\zeta_{m})-\Psi(1) are elements of ΛΛ\varLambda-\varLambda and since |z|2=zz¯|z|^{2}=z\bar{z} for zz\in\mathbbm{C}, we get the relation

(1+ζm+ζ¯m)2=(1+ζm+ζm1)2=|ζm2ζm1|2|ζm1|2=|Ψ(ζm2)Ψ(ζm1)|2|Ψ(ζm)Ψ(1)|2𝕜Λ.(1+\zeta_{m}+\bar{\zeta}_{m})^{2}=(1+\zeta_{m}+\zeta_{m}^{-1})^{2}=\frac{|\zeta_{m}^{2}-\zeta_{m}^{-1}|^{2}}{|\zeta_{m}-1|^{2}}=\frac{|\Psi(\zeta_{m}^{2})-\Psi(\zeta_{m}^{-1})|^{2}}{|\Psi(\zeta_{m})-\Psi(1)|^{2}}\in\mathbbm{k}_{\varLambda}\,.

The pairs {ζm1,ζm}\{\zeta_{m}^{-1},\zeta_{m}\}, {ζm2,ζm2}\{\zeta_{m}^{-2},\zeta_{m}^{2}\} also lie on parallel lines. An argument similar to that above yields

(ζm+ζ¯m)2=(ζm+ζm1)2=|ζm2ζm2|2|ζmζm1|2𝕜Λ.(\zeta_{m}+\bar{\zeta}_{m})^{2}=(\zeta_{m}+\zeta_{m}^{-1})^{2}=\frac{|\zeta_{m}^{2}-\zeta_{m}^{-2}|^{2}}{|\zeta_{m}-\zeta_{m}^{-1}|^{2}}\in\mathbbm{k}_{\varLambda}\,.

By subtracting these equations, one gets the relation

2(ζm+ζ¯m)+1𝕜Λ,2(\zeta_{m}+\bar{\zeta}_{m})+1\in\mathbbm{k}_{\varLambda}\,,

whence ζm+ζ¯m𝕜Λ\zeta_{m}+\bar{\zeta}_{m}\in\mathbbm{k}_{\varLambda}, the latter being equivalent to the inclusion of the fields 𝕜m𝕜Λ\mathbbm{k}_{m}\subset\mathbbm{k}_{\varLambda}.

For (ii) \Rightarrow (i), let RmR_{m} again be the regular mm-gon as defined in step (i) \Rightarrow (ii). Since m3m\geq 3, the set {1,ζm}\{1,\zeta_{m}\} is an \mathbbm{R}-basis of \mathbbm{C}. Since Λ\varLambda is non-degenerate, there is an element τ𝕂Λ\tau\in\mathbbm{K}_{\varLambda} with non-zero imaginary part. Hence, one can define an \mathbbm{R}-linear map L:22L\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} as the linear extension of 111\mapsto 1 and ζmτ\zeta_{m}\mapsto\tau. Since {1,τ}\{1,\tau\} is an \mathbbm{R}-basis of \mathbbm{C} as well, this map is non-singular. Since 𝕜m𝕜Λ\mathbbm{k}_{m}\subset\mathbbm{k}_{\varLambda} and since {1,ζm}\{1,\zeta_{m}\} is a 𝕜m\mathbbm{k}_{m}-basis of 𝕂m\mathbbm{K}_{m} (cf. Corollary 2.3), the vertices of L(Rm)L(R_{m}), i.e., L(1),L(ζm),,L(ζmm1)L(1),L(\zeta_{m}),\dots,L(\zeta_{m}^{m-1}), lie in 𝕂Λ\mathbbm{K}_{\varLambda}, whence L(Rm)L(R_{m}) is a polygon in 𝕂Λ\mathbbm{K}_{\varLambda}. By property (Aff), there is a non-singular affine transformation Ψ:22\Psi\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} such that Ψ(L(Rm))\Psi(L(R_{m})) is a polygon in Λ\varLambda. Since compositions of non-singular affine transformations are non-singular affine transformations again, Ψ(L(Rm))\Psi(L(R_{m})) is an affinely regular mm-gon in Λ\varLambda.

For the additional statement, note that, since Λ\varLambda has property (Alg), one has [𝕜Λ:]<[\mathbbm{k}_{\varLambda}:\mathbbm{Q}]<\infty by Remark 3.2. Thus, 𝕜Λ/\mathbbm{k}_{\varLambda}/\mathbbm{Q} has only finitely many intermediate fields. The assertion now follows immediately from condition (ii) in conjunction with Corollary 2.7, Remark 2.8 and Lemma 2.9. ∎

Let 𝕃\mathbbm{L} be an imaginary algebraic number field with 𝕃¯=𝕃\overline{\mathbbm{L}}=\mathbbm{L} and let 𝒪𝕃\mathcal{O}_{\mathbbm{L}} be the ring of integers in 𝕃\mathbbm{L}. Then, every translate Λ\varLambda of 𝕃\mathbbm{L} or 𝒪𝕃\mathcal{O}_{\mathbbm{L}} is non-degenerate and satisfies the properties (Alg) and (Aff). To this end, we first show that in both cases one has 𝕂Λ=𝕃\mathbbm{K}_{\varLambda}=\mathbbm{L}. If Λ\varLambda is a translate of 𝕃\mathbbm{L}, this follows immediately from the calculation

𝕂Λ=𝕂𝕃=(𝕃𝕃¯)=𝕃.\mathbbm{K}_{\varLambda}=\mathbbm{K}_{\mathbbm{L}}=\mathbbm{Q}(\mathbbm{L}\cup\overline{\mathbbm{L}})=\mathbbm{L}\,.

If Λ\varLambda is a translate of 𝒪𝕃\mathcal{O}_{\mathbbm{L}}, one has to observe that

𝕂Λ=𝕂𝒪𝕃=(𝒪𝕃𝒪𝕃¯)=𝕃,\mathbbm{K}_{\varLambda}=\mathbbm{K}_{\mathcal{O}_{\mathbbm{L}}}=\mathbbm{Q}(\mathcal{O}_{\mathbbm{L}}\cup\overline{\mathcal{O}_{\mathbbm{L}}})=\mathbbm{L}\,,

since 𝕃¯=𝕃\overline{\mathbbm{L}}=\mathbbm{L} implies 𝒪𝕃¯=𝒪𝕃\overline{\mathcal{O}_{\mathbbm{L}}}=\mathcal{O}_{\mathbbm{L}}. In the first case, property (Aff) is evident, whereas, if Λ\varLambda is a translate of 𝒪𝕃\mathcal{O}_{\mathbbm{L}}, property (Aff) follows from the fact that there is always a \mathbbm{Z}-basis of 𝒪𝕃\mathcal{O}_{\mathbbm{L}} that is simultaneously a \mathbbm{Q}-basis of 𝕃\mathbbm{L}. Thus, if F𝕃F\subset\mathbbm{L} is a finite set, then a suitable translate of aFaF is contained in Λ\varLambda, where aa is defined as the least common multiple of the denominators of the \mathbbm{Q}-coordinates of the elements of FF with respect to a \mathbbm{Q}-basis of 𝕃\mathbbm{L} that is simultaneously a \mathbbm{Z}-basis of 𝒪𝕃\mathcal{O}_{\mathbbm{L}}. Hence, for these two examples, property (Aff) may be replaced by the stronger property

  • (Hom)

    For all F(𝕂Λ)F\in\mathcal{F}(\mathbbm{K}_{\varLambda}), there is a homothety h:22h\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} such that h(F)Λh(F)\subset\varLambda .

Thus, we have obtained the following consequence of Theorem 3.3.

Corollary 3.4.

Let 𝕃\mathbbm{L} be an imaginary algebraic number field with 𝕃¯=𝕃\overline{\mathbbm{L}}=\mathbbm{L} and let 𝒪𝕃\mathcal{O}_{\mathbbm{L}} be the ring of integers in 𝕃\mathbbm{L}. Let Λ\varLambda be a translate of 𝕃\mathbbm{L} or a translate of 𝒪𝕃\mathcal{O}_{\mathbbm{L}}. Further, let mm\in\mathbbm{N} with m3m\geq 3. Denoting the maximal real subfield of 𝕃\mathbbm{L} by 𝕝\mathbbm{l}, the following statements are equivalent:

  • (i)

    There is an affinely regular mm-gon in Λ\varLambda.

  • (ii)

    𝕜m𝕝\mathbbm{k}_{m}\subset\mathbbm{l}.

Further, Λ\varLambda only contains affinely regular mm-gons for finitely many values of mm.

Remark 3.5.

In particular, Corollary 3.4 applies to translates of imaginary cyclotomic fields and their rings of integers, with 𝕝=𝕜n\mathbbm{l}=\mathbbm{k}_{n} for a suitable n3n\geq 3; cf. Facts 2.2 and 2.4 and also compare the equivalences of Corollary 4.1 below.

4. Application to cyclotomic model sets

Remarkably, there are Delone subsets of the plane satisfying properties (Alg) and (Hom). These sets were introduced as algebraic Delone sets in [13, Definition 4.2]. Note that algebraic Delone sets are always non-degenerate, since this is true for all relatively dense subsets of the plane. It was shown in [13, Proposition 4.15] that the so-called cyclotomic model sets Λ\varLambda are examples of algebraic Delone sets; cf. Section 4 of [13] and [13, Definition 4.6] in particular for the definition of cyclotomic model sets. Any cyclotomic model set Λ\varLambda is contained in a translate of 𝒪n\mathcal{O}_{n}, where n3n\geq 3, in which case the \mathbbm{Z}-module 𝒪n\mathcal{O}_{n} is called the underlying \mathbbm{Z}-module of Λ\varLambda. With the exception of the crystallographic cases of translates of the square lattice 𝒪4\mathcal{O}_{4} and translates of the triangular lattice 𝒪3\mathcal{O}_{3}, cyclotomic model sets are aperiodic (i.e., they have no translational symmetries) and have long-range order; cf. [13, Remarks 4.9 and 4.10]. Well-known examples of cyclotomic model sets with underlying \mathbbm{Z}-module 𝒪n\mathcal{O}_{n} are the vertex sets of aperiodic tilings of the plane like the Ammann-Beenker tiling [1, 2, 11] (n=8n=8), the Tübingen triangle tiling [3, 4] (n=5n=5) and the shield tiling [11] (n=12n=12); cf. [13, Example 4.11] for a definition of the vertex set of the Ammann-Beenker tiling and see Figure 1 and [13, Figure 1] for illustrations. For further details and illustrations of the examples of cyclotomic model sets mentioned above, we refer the reader to [14, Section 1.2.3.2]. Clearly, any cyclotomic model set Λ\varLambda with underlying \mathbbm{Z}-module 𝒪n\mathcal{O}_{n} satisfies

(3) 𝕂Λ(𝒪n𝒪n¯)=𝕂n,\mathbbm{K}_{\varLambda}\subset\mathbbm{Q}(\mathcal{O}_{n}\cup\overline{\mathcal{O}_{n}})=\mathbbm{K}_{n}\,,

whence 𝕜Λ𝕜n\mathbbm{k}_{\varLambda}\subset\mathbbm{k}_{n}. It was shown in  [13, Lemma 4.14] that cyclotomic model sets Λ\varLambda with underlying \mathbbm{Z}-module 𝒪n\mathcal{O}_{n} even satisfy the following stronger version of property (Hom) above:

  • (Hom)

    For all F(𝕂n)F\in\mathcal{F}(\mathbbm{K}_{n}), there is a homothety h:22h\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} such that h(F)Λh(F)\subset\varLambda .

This property enables us to prove the following characterization.

Refer to caption

Figure 1. A central patch of the eightfold symmetric Ammann-Beenker tiling of the plane with squares and rhombi, both having edge length 11. Therein, an affinely regular 66-gon is marked.
Corollary 4.1.

Let m,nm,n\in\mathbbm{N} with m,n3m,n\geq 3. Further, let Λ\varLambda be a cyclotomic model set with underlying \mathbbm{Z}-module 𝒪n\mathcal{O}_{n}. The following statements are equivalent:

  • (i)

    There is an affinely regular mm-gon in Λ\varLambda.

  • (ii)

    𝕜m𝕜n\mathbbm{k}_{m}\subset\mathbbm{k}_{n}.

  • (iii)

    m{3,4,6}m\in\{3,4,6\}, or 𝕂m𝕂n\mathbbm{K}_{m}\subset\mathbbm{K}_{n}.

  • (iv)

    m{3,4,6}m\in\{3,4,6\}, or m|nm|n, or m=2dm=2d with dd an odd divisor of nn.

  • (v)

    m{3,4,6}m\in\{3,4,6\}, or 𝒪m𝒪n\mathcal{O}_{m}\subset\mathcal{O}_{n}.

  • (vi)

    𝒪m𝒪n\thinspace\scriptstyle{\mathcal{O}}{}_{m}\subset\thinspace\scriptstyle{\mathcal{O}}{}_{n}.

Proof.

Direction (i) \Rightarrow (ii) is an immediate consequence of Theorem 3.3 in conjunction with Relation (3). For direction (ii) \Rightarrow (i), let RmR_{m} again be the regular mm-gon as defined in step (i) \Rightarrow (ii) of Theorem 3.3. Since m,n3m,n\geq 3, the sets {1,ζm}\{1,\zeta_{m}\} and {1,ζn}\{1,\zeta_{n}\} are \mathbbm{R}-bases of \mathbbm{C}. Hence, one can define an \mathbbm{R}-linear map L:22L\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} as the linear extension of 111\mapsto 1 and ζmζn\zeta_{m}\mapsto\zeta_{n}. Clearly, this map is non-singular. Since 𝕜m𝕜n\mathbbm{k}_{m}\subset\mathbbm{k}_{n} and since {1,ζm}\{1,\zeta_{m}\} is a 𝕜m\mathbbm{k}_{m}-basis of 𝕂m\mathbbm{K}_{m} (cf. Corollary 2.3), the vertices of L(Rm)L(R_{m}), i.e., L(1),L(ζm),,L(ζmm1)L(1),L(\zeta_{m}),\dots,L(\zeta_{m}^{m-1}), lie in 𝕂n\mathbbm{K}_{n}, whence L(Rm)L(R_{m}) is a polygon in 𝕂n\mathbbm{K}_{n}. Because Λ\varLambda has property (Hom), there is a homothety h:22h\!:\,\mathbbm{R}^{2}\rightarrow\mathbbm{R}^{2} such that h(L(Rm))h(L(R_{m})) is a polygon in Λ\varLambda. Since homotheties are non-singular affine transformations, h(L(Rm))h(L(R_{m})) is an affinely regular mm-gon in Λ\varLambda. As an immediate consequence of Lemma 2.9(b), we get the equivalence (ii) \Leftrightarrow (iii). Conditions (iii) and (iv) are equivalent by Lemma 2.6. Finally, the equivalences (iii) \Leftrightarrow (v) and (ii) \Leftrightarrow (vi) follow immediately from Fact 2.4. ∎

Although the equivalence (i) \Leftrightarrow (iv) in Corollary 4.1 is fully satisfactory, the following consequence deals with the two cases where condition (ii) can be used more effectively.

Corollary 4.2.

Let m,nm,n\in\mathbbm{N} with m,n3m,n\geq 3. Further, let Λ\varLambda be a cyclotomic model set with underlying \mathbbm{Z}-module 𝒪n\mathcal{O}_{n}. Consider ϕ\phi on {n|n 2(mod4)}\{n\in\mathbbm{N}\,|\,n\;\not\equiv\;2\;(\operatorname{mod}4)\}. Then, one has:

  • (a)

    If n{3,4}n\in\{3,4\}, there is an affinely regular mm-gon in Λ\varLambda if and only if m{3,4,6}m\in\{3,4,6\}.

  • (b)

    If n𝒮n\in\mathcal{S}, there is an affinely regular mm-gon in Λ\varLambda if and only if

    {m{3,4,6,n},if n=8 or n=12,m{3,4,6,n,2n},otherwise.\left\{\begin{array}[]{ll}m\in\{3,4,6,n\},&\mbox{if $n=8$ or $n=12$,}\\ m\in\{3,4,6,n,2n\},&\mbox{otherwise.}\end{array}\right.
Proof.

By Lemma 2.10(a), n{3,4}n\in\{3,4\} is equivalent to ϕ(n)/2=1\phi(n)/2=1, thus condition (ii) of Corollary 4.1 specializes to 𝕜m=\mathbbm{k}_{m}=\mathbbm{Q}, the latter being equivalent to ϕ(m)=2\phi(m)=2, which means m{3,4,6}m\in\{3,4,6\}; cf. Corollary 2.3. This proves the part (a).

By Lemma 2.10(b), n𝒮n\in\mathcal{S} is equivalent to ϕ(n)/2𝒫\phi(n)/2\in\mathcal{P}. By Corollary 2.3, this shows that [𝕜n:]=ϕ(n)/2𝒫[\mathbbm{k}_{n}:\mathbbm{Q}]=\phi(n)/2\in\mathcal{P}. Hence, by condition (ii) of Corollary 4.1, one either gets 𝕜m=\mathbbm{k}_{m}=\mathbbm{Q} or 𝕜m=𝕜n\mathbbm{k}_{m}=\mathbbm{k}_{n}. The former case implies m{3,4,6}m\in\{3,4,6\} as in the proof of the part (a), while the proof follows from Lemma 2.9(a) in conjunction with Corollary 2.7 in the latter case. ∎

Example 4.3.

As mentioned above, the vertex set ΛAB\varLambda_{\rm AB} of the Ammann-Beenker tiling is a cyclotomic model set with underlying \mathbbm{Z}-module 𝒪8\mathcal{O}_{8}. Since 8𝒮8\in\mathcal{S}, Corollary 4.2 now shows that there is an affinely regular mm-gon in ΛAB\varLambda_{\rm AB} if and only if m{3,4,6,8}m\in\{3,4,6,8\}; see Figure 1 for an affinely regular 66-gon in ΛAB\varLambda_{\rm AB}. The other solutions are rather obvious, in particular the patch shown also contains the regular 88-gon R8R_{8}, given by the 88th roots of unity.

For further illustrations and explanations of the above results, we refer the reader to [14, Section 2.3.4.1] or [12, Section 5]. This references also provide a detailed description of the construction of affinely regular mm-gons in cyclotomic model sets, given that they exist.

5. Application to discrete tomography of cyclotomic model sets

Discrete tomography is concerned with the inverse problem of retrieving information about some finite object from information about its slices; cf. [8, 9, 12, 13, 14] and also see the refences therein. A typical example is the reconstruction of a finite point set from its (discrete parallel) XX-rays in a small number of directions. In the following, we restrict ourselves to the planar case.

Definition 5.1.

Let F(2)F\in\mathcal{F}(\mathbbm{R}^{2}), let u𝕊1u\in\mathbb{S}^{1} be a direction and let u\mathcal{L}_{u} be the set of lines in direction uu in 2\mathbbm{R}^{2}. Then, the (discrete parallel) X-ray of FF in direction uu is the function XuF:u0:={0}X_{u}F:\mathcal{L}_{u}\rightarrow\mathbbm{N}_{0}:=\mathbbm{N}\cup\{0\}, defined by

XuF():=card(F)=x𝟙F(x).X_{u}F(\ell):=\operatorname{card}(F\cap\ell\,)=\sum_{x\in\ell}\mathbbm{1}_{F}(x)\,.

In [13], we studied the problem of determining convex subsets of algebraic Delone sets Λ\varLambda by XX-rays. Solving this problem amounts to find small sets UU of suitably prescribed Λ\varLambda-directions with the property that different convex subsets of Λ\varLambda cannot have the same XX-rays in the directions of UU. More generally, one defines as follows.

Definition 5.2.

Let (2)\mathcal{E}\subset\mathcal{F}(\mathbbm{R}^{2}), and let mm\in\mathbbm{N}. Further, let U𝕊1U\subset\mathbb{S}^{1} be a finite set of directions. We say that \mathcal{E} is determined by the XX-rays in the directions of UU if, for all F,FF,F^{\prime}\in\mathcal{E}, one has

(XuF=XuFuU)F=F.(X_{u}F=X_{u}F^{\prime}\;\,\forall u\in U)\;\Longrightarrow\;F=F^{\prime}\,.

Let Λ2\varLambda\subset\mathbbm{R}^{2} be a Delone set and let U𝕊1U\subset\mathbb{S}^{1} be a set of two or more pairwise non-parallel Λ\varLambda-directions. Suppose the existence of a UU-polygon PP in Λ\varLambda. Partition the vertices of PP into two disjoint sets V,VV,V^{\prime}, where the elements of these sets alternate round the boundary of PP. Since PP is a UU-polygon, each line in the plane parallel to some uUu\in U that contains a point in VV also contains a point in VV^{\prime}. In particular, one sees that card(V)=card(V)\operatorname{card}(V)=\operatorname{card}(V^{\prime}). Set

C:=(ΛP)(VV)C:=(\varLambda\cap P)\setminus(V\cup V^{\prime})

and, further, F:=CVF:=C\cup V and F:=CVF^{\prime}:=C\cup V^{\prime}. Then, FF and FF^{\prime} are different convex subsets of Λ\varLambda with the same XX-rays in the directions of UU. We have just proven direction (i) \Rightarrow (ii) of the following equivalence, which particularly applies to cyclotomic model sets, since any cyclotomic model set is an algebraic Delone set by [13, Proposition 4.15].

Theorem 5.3.

[13, Theorem 6.3] Let Λ\varLambda be an algebraic Delone set and let U𝕊1U\subset\mathbb{S}^{1} be a set of two or more pairwise non-parallel Λ\varLambda-directions. The following statements are equivalent:

  • (i)

    𝒞(Λ)\mathcal{C}(\varLambda) is determined by the XX-rays in the directions of UU.

  • (ii)

    There is no UU-polygon in Λ\varLambda.

Remark 5.4.

Trivially, any affinely regular mm-gon PP in Λ\varLambda with mm even is a UU-polygon in Λ\varLambda with respect to any set U𝕊1U\subset\mathbb{S}^{1} of pairwise non-parallel directions having the property that each element of UU is parallel to one of the edges of PP. The set UU then consists only of Λ\varLambda-directions and, moreover, satisfies card(U)m/2\operatorname{card}(U)\leq m/2.

By combining Corollary 4.1, direction (i) \Rightarrow (ii) of Theorem 5.3 and Remark 5.4, one immediately obtains the following consequence.

Corollary 5.5.

Let n3n\geq 3 and let Λ\varLambda be a cyclotomic model set with underlying \mathbbm{Z}-module 𝒪n\mathcal{O}_{n}. Suppose that there exists a natural number kk\in\mathbbm{N} such that, for any set UU of kk pairwise non-parallel Λ\varLambda-directions, the set 𝒞(Λ)\mathcal{C}(\varLambda) is determined by the XX-rays in the directions of UU. Then, one has

k>max{3,lcm(n,2)2}.k>\,\max\left\{3,\tfrac{\operatorname{lcm}(n,2)}{2}\right\}\,.
Remark 5.6.

In the situation of Corollary 5.5, the question of existence of a suitable number kk\in\mathbbm{N} is a much more intricate problem. So far, it has only been answered affirmatively by Gardner and Gritzmann in the case of translates of the square lattice (n=4n=4), whence corresponding results hold for all translates of planar lattices, in particular for translates of the triangular lattice (n=3n=3); cf. [9, Theorem 5.7(ii) and (iii)]. More precisely, it is shown there that, for these cases, the number k=7k=7 is the smallest among all possible values of kk. It would be interesting to know if suitable numbers kk\in\mathbbm{N} exist for all cyclotomic model sets.

Let us finally note the following relation between UU-polygons and affinely regular polygons. The proof uses a beautiful theorem of Darboux [7] on second midpoint polygons; cf. [10] or [8, Ch. 1].

Proposition 5.7.

[9, Proposition 4.2] If U𝕊1U\subset\mathbb{S}^{1} is a finite set of directions, there exists a UU-polygon if and only if there is an affinely regular polygon such that each direction of U\,U is parallel to one of its edges.

Remark 5.8.

A UU-polygon need not itself be an affinely regular polygon, even if it is a UU-polygon in a cyclotomic model set; cf. [9, Example 4.3] for the case of planar lattices and [14, Example 2.46] or [12, Example 1] for related examples in the case of aperiodic cyclotomic model sets.

Acknowledgements

I am indebted to Michael Baake, Richard J. Gardner, Uwe Grimm and Peter A. B. Pleasants for their cooperation and for useful hints on the manuscript. Interesting discussions with Peter Gritzmann and Barbara Langfeld are gratefully acknowledged.

References

  • [1] R. Ammann, B. Grünbaum G. C. Shephard, Aperiodic tiles, Discrete Comput. Geom. 8 (1992), 1–25.
  • [2] M. Baake D. Joseph, Ideal and defective vertex configurations in the planar octagonal quasilattice, Phys. Rev. B 42 (1990), 8091–8102.
  • [3] M. Baake, P. Kramer, M. Schlottmann D. Zeidler, The triangle pattern – a new quasiperiodic tiling with fivefold symmetry, Mod. Phys. Lett. B 4 (1990), 249–258.
  • [4] M. Baake, P. Kramer, M. Schlottmann D. Zeidler, Planar patterns with fivefold symmetry as sections of periodic structures in 4-space, Int. J. Mod. Phys. B 4 (1990), 2217–2268.
  • [5] Z. I. Borevich I. R. Shafarevich, Number Theory, Academic Press, New York, 1966.
  • [6] H. E. Chrestenson, Solution to problem 5014, Amer. Math. Monthly 70 (1963), 447–448.
  • [7] M. G. Darboux, Sur un problème de géométrie élémentaire, Bull. Sci. Math. 2 (1878), 298–304.
  • [8] R. J. Gardner, Geometric Tomography, 2nd ed., Cambridge University Press, New York, 2006.
  • [9] R. J. Gardner P. Gritzmann, Discrete tomography: determination of finite sets by X-rays, Trans. Amer. Math. Soc. 349 (1997), 2271–2295.
  • [10] R. J. Gardner P. McMullen, On Hammer’s X-ray problem, J. London Math. Soc. (2) 21 (1980), 171–175.
  • [11] F. Gähler, Matching rules for quasicrystals: the composition-decomposition method, J. Non-Cryst. Solids 153-154 (1993), 160–164.
  • [12] C. Huck, Uniqueness in discrete tomography of planar model sets, notes (2007); arXiv:math/0701141v2 [math.MG]
  • [13] C. Huck, Uniqueness in discrete tomography of Delone sets with long-range order, submitted; arXiv:0711.4525v1 [math.MG]
  • [14] C. Huck, Discrete Tomography of Delone Sets with Long-Range Order, Ph.D. thesis (Universität Bielefeld), Logos Verlag, Berlin, 2007.
  • [15] S. Lang, Algebra, 3rd ed., Addison-Wesley, Reading, MA, 1993.
  • [16] N. J. A. Sloane (ed.), The Online Encyclopedia of Integer Sequences, published electronically at http://www.research.att.com/~njas/sequences/
  • [17] L. C. Washington, Introduction to Cyclotomic Fields, 2nd ed., Springer, New York, 1997.