How big is a tiling’s return module?

Abstract The rank of a tiling’s return module depends on the geometry of its tiles and is not a topological invariant. However, the rank of the first Čech cohomology $\check H^1(\Omega )$ gives upper and lower bounds for the rank of the return module. For all sufficiently large patches, the rank of the return module is at most the rank of $\check H^1(\Omega )$ . For a generic choice of tile shapes and an arbitrary reference patch, the rank of the return module is at least the rank of $\check H^1(\Omega )$ . Therefore, for generic tile shapes and all sufficiently large patches, the rank of the return module is equal to the rank of $\check H^1(\Omega )$ .

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Publication Details

Journal
Ergodic Theory and Dynamical Systems
Published
2025-01-22
DOI
https://doi.org/10.1017/etds.2024.137
Primary Topic
Quasicrystal Structures and Properties
Type
article
Field-Weighted Citation Impact
0.00

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article

How big is a tiling’s return module?

Lorenzo Sadun, Abigail Perryman
Ergodic Theory and Dynamical Systems
Quasicrystal Structures and Properties
article

How big is a tiling’s return module?

Lorenzo Sadun, Abigail Perryman
article en

Abstract

Abstract The rank of a tiling’s return module depends on the geometry of its tiles and is not a topological invariant. However, the rank of the first Čech cohomology $\check H^1(\Omega )$ gives upper and lower bounds for the rank of the return module. For all sufficiently large patches, the rank of the return module is at most the rank of $\check H^1(\Omega )$ . For a generic choice of tile shapes and an arbitrary reference patch, the rank of the return module is at least the rank of $\check H^1(\Omega )$ . Therefore, for generic tile shapes and all sufficiently large patches, the rank of the return module is equal to the rank of $\check H^1(\Omega )$ .

Ergodic Theory and Dynamical SystemsVol. 45(8)
The University of Texas at Austin (US)
National Science Foundation
Openalex Percentile: Top 99%
Quasicrystal Structures and Properties
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