Abstract

AbstractWe present a single, connected tile which can tile the plane but only nonperiodically. The tile is hexagonal with edge markings, which impose simple rules as to how adjacent tiles are allowed to meet across edges. The first of these rules is a standard matching rule, that certain decorations match across edges. The second condition is a new type of matching rule, which allows tiles to meet only when certain decorations in a particular orientation are given the opposite charge. This forces the tiles to form a hierarchy of triangles, following a central idea of the Socolar–Taylor tilings. However, the new edge-to-edge orientational matching rule forces this structure in a very different way, which allows for a surprisingly simple proof of aperiodicity. We show that the hull of all tilings satisfying our rules is uniquely ergodic and that almost all tilings in the hull belong to a minimal core of tilings generated by substitution. Identifying tilings which are charge-flips of each other, these tilings are shown to have pure point dynamical spectrum and a regular model set structure.

Highlights

  • The fact that periodically arranged structures can be enforced by local rules is familiar to everyone

  • It was a great surprise to crystallographers in the 1980s when Dan Shechtman discovered a metal alloy whose diffraction pattern implied a great deal of structural order but had rotational symmetry precluding periodicity [20]

  • (1) We denote the collection of standard R1-tilings by Ωa because these tilings are seen to be mutually local derivable (MLD; see [2]) to the arrowed hex tilings [1]

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Summary

Introduction

The fact that periodically arranged structures can be enforced by local rules is familiar to everyone. The patterns of tile parities (given by labeling hexagons only with the information of whether the tile of Figure 1 or its mirror image is used) are very different, and closely follow the structure of the R1-edges, which are forced to carry the same parities across them. This observation leads to a remarkably simple proof of aperiodicity, presented in full detail in §2 and which we briefly outline now. The substitutional hull (modulo charge-flip) factors almost everywhere 1-to-1 to its maximal equicontinuous factor and so has pure point dynamical spectrum and the structure of a regular model set

R1-triangles
Charges of triangle edges
Finding edges of increasing length
Standard R1-tilings
R1-edge graphs
The hull of tilings
Generating valid tilings by substitution
MLD triangle tilings
Supertile decompositions of valid tilings
Unique ergodicity
Topological factors and spectral properties
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