The Hexagonal Tiling Honeycomb
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arXiv
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| Format: | Preprint |
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2024
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| _version_ | 1866909410136162304 |
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| author | Baez, John C. |
| author_facet | Baez, John C. |
| contents | The hexagonal tiling honeycomb is a beautiful structure in 3-dimensional hyperbolic space. It is called {6,3,3} because each hexagon has 6 edges, 3 hexagons meet at each vertex in a Euclidean plane tiled by regular hexagons, and 3 such planes meet along each edge of this honeycomb. It also appears naturally in algebraic geometry. If $\mathbb{E}$ denotes the Eisenstein integers, the Néron-Severi group of the abelian surface $\mathbb{C}^2/\mathbb{E}^2$ is isomorphic to the lattice $\mathfrak{h}_2(\mathbb{E})$ consisting of $2 \times 2$ hermitian matrices with Eisenstein integer entries. The points $A \in \mathfrak{h}_2(\mathbb{E})$ with $\mathrm{tr}(A) \gt 0$ and $\det(A) \gt 0$ come from ample line bundles on $\mathbb{C}^2/\mathbb{E}^2$, and among these points, those with $\det(A) = 1$ correspond to principal polarizations. But these points are precisely the centers of the hexagons in the hexagonal tiling honeycomb! |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2412_00048 |
| institution | arXiv |
| publishDate | 2024 |
| record_format | arxiv |
| spellingShingle | The Hexagonal Tiling Honeycomb Baez, John C. History and Overview Algebraic Geometry Metric Geometry The hexagonal tiling honeycomb is a beautiful structure in 3-dimensional hyperbolic space. It is called {6,3,3} because each hexagon has 6 edges, 3 hexagons meet at each vertex in a Euclidean plane tiled by regular hexagons, and 3 such planes meet along each edge of this honeycomb. It also appears naturally in algebraic geometry. If $\mathbb{E}$ denotes the Eisenstein integers, the Néron-Severi group of the abelian surface $\mathbb{C}^2/\mathbb{E}^2$ is isomorphic to the lattice $\mathfrak{h}_2(\mathbb{E})$ consisting of $2 \times 2$ hermitian matrices with Eisenstein integer entries. The points $A \in \mathfrak{h}_2(\mathbb{E})$ with $\mathrm{tr}(A) \gt 0$ and $\det(A) \gt 0$ come from ample line bundles on $\mathbb{C}^2/\mathbb{E}^2$, and among these points, those with $\det(A) = 1$ correspond to principal polarizations. But these points are precisely the centers of the hexagons in the hexagonal tiling honeycomb! |
| title | The Hexagonal Tiling Honeycomb |
| topic | History and Overview Algebraic Geometry Metric Geometry |
| url | https://arxiv.org/abs/2412.00048 |