The Hexagonal Cell: Symmetry Beyond the Frame

geometrysymmetrymirrors

An exact symmetry can belong to something larger. Begin with a hexagonal mirror room: its reflections fill space without an angular gap. Then unfold the room into the chambers that generate it, or follow the same six vertices into higher dimensions.

Stand inside the reflections
Lighting the mirrors…
Six chambers in one room120° between walls · 90° at the caps

Drag to orbit · right-drag to look · scroll or pinch to move · WASD to fly · double-tap to enter

Light and mirrors
Light and line
The room and the chamber

Three regular hexagons meet at a point: 3×120°=360°3\times120°=360°. Their prisms also meet four at a time along the horizontal edges, where the dihedral angle is 90°90°. The geometry closes in both directions. This gives the Infinity Cell a new exact Euclidean home.

There is another structure inside the frame. Join the hexagon’s center to its six vertices and it becomes six equilateral triangles. Each triangle has 60°60° corners, and reflections in its sides generate the triangular tiling. These are the fundamental chambers of the affine reflection group A~2\widetilde{A}_2.

The hexagonal room contains six chambers. Several reflection sequences can reach the same geometric room with different internal orientations. The wireframe still agrees; an asymmetric object or colored pattern can appear in several orientations. Exact room geometry does not require every colored reflection to look identical.

The triangular prism in Mirrors has the proportions of one of these six chambers. Each cell is framed independently by the camera. Unfold shows their actual relationship, then extends the rooms through the plane and into three layers of space.

The hexagonal mirror-room construction appears in Miles Reid and Balázs Szendrői’s Geometry and Topology, §6.6.

Six vertices, then twelve, then twenty-four

The Lift view follows an exact inclusion of three root systems:

A2⊂D3⊂D4.A_2 \subset D_3 \subset D_4.

The six roots of A2A_2 form a regular hexagon. Six more vertices complete the cuboctahedron, the twelve-neighbor arrangement in a face-centered cubic lattice. Twelve more complete the regular four-dimensional 24-cell. The same original hexagon belongs to every stage.

One coordinate rule produces the whole structure. In four dimensions take every vector with two nonzero coordinates, each equal to +1+1 or −1-1. These are the twenty-four roots of D4D_4. Keep only those with fourth coordinate zero to obtain D3D_3. Also require the first three coordinates to sum to zero to obtain A2A_2. Joining pairs at distance 2\sqrt{2} gives, respectively, 96, 24, and 6 edges.

The 4D rotation turns the two directions perpendicular to the original hexagon. Its six vertices therefore stay fixed while the surrounding structure moves. The drawing is a projection: apparent edge lengths vary, but the lengths in the original geometry remain equal. The transition reveals additional vertices at their exact positions.

The 24-cell is a regular four-dimensional polytope made of twenty-four octahedral cells. This dimensional extension is a separate construction from the Euclidean mirror room. Both begin with an exact hexagon and expose a larger order in which it participates.

John Baez’s Lie Theory Through Examples develops the connections between these root systems, lattices, and regular polytopes.

Where diamond enters the picture

Ordinary diamond has cubic crystal symmetry and a tetrahedral bonding network. Its structure includes puckered six-membered rings. Cubic and hexagonal diamond retain tetrahedral coordination while arranging related layers differently.

A regular hexagon can be folded into a chair-shaped ring while keeping every edge the same length. At a particular fold, its bond angles become the tetrahedral angle arccos⁡(−1/3)≈109.47°\arccos(-1/3)\approx109.47°. The top view remains hexagonal while a tilted view reveals the alternating heights. This is a physical branch of the same geometric question: how can one exact arrangement belong to a larger structure?

Diamond’s hardness reflects its bonding framework; it does not rank the crystal’s symmetry above other shapes. The crystal structure is also distinct from the close-packed lattice associated with the cuboctahedron in Lift.

See Murri and colleagues, Quantifying hexagonal stacking in diamond.