In geometry, the Dehn invariant of a polyhedron is a value used to determine whether polyhedra can be dissected into each other or whether they can tile space. It is named after Max Dehn, who used it to solve Hilbert's third problem on whether all polyhedra with equal volume could be dissected into each other.
Two polyhedra have a dissection into polyhedral pieces that can be reassembled into either one, if and only if their volumes and Dehn invariants are equal. A polyhedron can be cut up and reassembled to tile space if and only if its Dehn invariant is zero, so having Dehn invariant zero is a necessary condition for being a space-filling polyhedron. It is also conjectured that the Dehn invariant of a flexible polyhedron must stay invariant as it flexes.
The Dehn invariant is zero for the cube but nonzero for the other Platonic solids, implying that the other solids cannot tile space and that they cannot be dissected into a cube. All of the Archimedean solids have Dehn invariants that are rational combinations of the invariants for the Platonic solids.
The Dehn invariants of polyhedra are elements of an infinite-dimensional vector space. As an abelian group, this space is part of an exact sequence involving group homology. Similar invariants can also be defined for some other dissection puzzles, including as the problem of dissecting rectilinear polygons into each other by axis-parallel cuts and translations.
In two dimensions, the Wallace–Bolyai–Gerwien theorem states that any two polygons of equal area can be cut up into polygonal pieces and reassembled into each other. David Hilbert became interested in this result as a way to axiomatize area, in connection with Hilbert's axioms for Euclidean geometry. In Hilbert's third problem, he posed the question of whether two polyhedra of equal volumes can always be cut into polyhedral pieces and reassembled into each other. Hilbert's student Max Dehn, in his 1900 habilitation thesis, invented the Dehn invariant in order to provide a negative solution to Hilbert's problem. Although Dehn formulated his invariant differently, the modern approach is to describe it as a value in a tensor product, following Jessen (1968).
The definition of the Dehn invariant requires a notion of a polyhedron for which the lengths and dihedral angles are well defined. Most commonly, it applies to the polyhedra whose boundaries are manifolds, embedded on a finite number of planes in Euclidean space. However, the Dehn invariant has also been considered for polyhedra spherical geometry or in hyperbolic space, and for certain self-crossing polyhedra in Euclidean space.
The left factor of this tensor product is the set of real numbers (in this case representing lengths of edges of polyhedra) and the right factor represents dihedral angles in radians, given as numbers modulo 2π. (Some sources take the angles modulo π instead of modulo 2π, or divide the angles by π and use in place of  but this makes no difference to the resulting tensor product, as any rational multiple of π in the right factor becomes zero in the product.)
The Dehn invariant of a polyhedron with edge lengths and edge dihedral angles is the sum
An alternative but equivalent description of the Dehn invariant involves the choice of a Hamel basis, an infinite subset of the real numbers such that every real number can be expressed uniquely as a sum of finitely many rational multiples of . Thus, as an additive group, is isomorphic to . If is chosen carefully so that π (or a rational multiple of π) is one of its elements, and is the rest of the basis with this element excluded, then the tensor product is the (infinite dimensional) real vector space . The Dehn invariant can be expressed by decomposing each dihedral angle into a finite sum of basis elements
where is rational, is one of the real numbers in the Hamel basis, and these basis elements are numbered so that is the rational multiple of π that belongs to but not . With this decomposition, the Dehn invariant is
where each is a unit vector in corresponding to the basis element . Although the Hamel basis formulation appears to involve the axiom of choice, this can be avoided (when considering any specific finite set of polyhedra) by restricting attention to the finite-dimensional vector space generated over by the dihedral angles of the polyhedra. This alternative formulation shows that the values of the Dehn invariant can be given the additional structure of a real vector space.
The Platonic solids each have uniform edge lengths and dihedral angles, none of which are rational multiples of each other. The dihedral angle of a cube, π/2, is a rational multiple of π, but the rest are not. The dihedral angles of the regular tetrahedron and regular octahedron are supplementary: they sum to π.
In the Hamel basis formulation of the Dehn invariant, one can choose four of these dihedral angles as part of the Hamel basis. The angle of the cube, π/2, is the basis element that is discarded in the formula for the Dehn invariant, so the Dehn invariant of the cube is zero. More generally, the Dehn invariant of any parallelepiped is also zero. Only one of the two angles of the tetrahedron and octahedron can be included, as the other one is a rational combination of the one that is included and the angle of the cube. The Dehn invariants of each of the other Platonic solids will be a vector in formed by multiplying the unit vector for that solid's angle by the length and number of edges of the solid. No matter how they are scaled by different edge lengths, the tetrahedron, icosahedron, and dodecahedron all have Dehn invariants that form vectors pointing in different directions, and therefore are unequal and nonzero.
The negated dihedral angle of the octahedron differs from the angle of a tetrahedron by an integer multiple of pi, and in addition the octahedron has two times as many edges as the tetrahedron (twelve instead of six). Therefore, the Dehn invariant of the octahedron is −2 times the Dehn invariant of a tetrahedron of the same edge length. The Dehn invariants of the other Archimedean solids can also be expressed as rational combinations of the invariants of the Platonic solids.
|Unsolved problem in mathematics:
Is there a dissection between every pair of spherical or hyperbolic polyhedra with the same volume and Dehn invariant as each other?
(more unsolved problems in mathematics)
As Dehn (1901) observed, the Dehn invariant is an invariant for the dissection of polyhedra, in the sense that cutting up a polyhedron into smaller polyhedral pieces and then reassembling them into a different polyhedron does not change the Dehn invariant of the result. Another such invariant is the volume of the polyhedron. Therefore, if it is possible to dissect one polyhedron P into a different polyhedron Q, then both P and Q must have the same Dehn invariant as well as the same volume. Sydler (1965) extended this result by proving that the volume and the Dehn invariant are the only invariants for this problem. If P and Q both have the same volume and the same Dehn invariant, it is always possible to dissect one into the other.
Dehn's result continues to be valid for spherical geometry and hyperbolic geometry. In both of those geometries, two polyhedra that can be cut and reassembled into each other must have the same Dehn invariant. However, as Jessen observed, the extension of Sydler's result to spherical or hyperbolic geometry remains open: it is not known whether two spherical or hyperbolic polyhedra with the same volume and the same Dehn invariant can always be cut and reassembled into each other. Every hyperbolic manifold with finite volume can be cut along geodesic surfaces into a hyperbolic polyhedron, which necessarily has zero Dehn invariant.
The Dehn invariant also controls the ability of a polyhedron to tile space (part of the subject of Hilbert's eighteenth problem). Every space-filling tile has Dehn invariant zero, like the cube. The reverse of this is not true – there exist polyhedra with Dehn invariant zero that do not tile space, but they can always be dissected into another shape (the cube) that does tile space.
More generally, if some combination of polyhedra jointly tiles space, then the sum of their Dehn invariants (taken in the same proportion) must be zero. For instance, the tetrahedral-octahedral honeycomb is a tiling of space by tetrahedra and octahedra (with twice as many tetrahedra as octahedra), corresponding to the fact that the sum of the Dehn invariants of an octahedron and two tetrahedra (with the same side lengths) is zero.
Although the Dehn invariant takes values in not all of the elements in this space can be realized as the Dehn invariants of polyhedra. The Dehn invariants of Euclidean polyhedra form a linear subspace of : one can add the Dehn invariants of polyhedra by taking the disjoint union of the polyhedra (or gluing them together on a face), negate Dehn invariants by making holes in the shape of the polyhedron into large cubes, and multiply the Dehn invariant by any scalar by scaling the polyhedron by the same number. The question of which elements of (or, equivalently, ) are realizable was clarified by the work of Dupont and Sah, who showed the existence of the following short exact sequence of abelian groups (not vector spaces) involving group homology:
Here, the notation represents the free abelian group over Euclidean polyhedra modulo certain relations derived from pairs of polyhedra that can be dissected into each other. is the subgroup generated in this group by the triangular prisms, and is used here to represent volume (as each real number is the volume of exactly one element of this group). The map from the group of polyhedra to is the Dehn invariant. is the Euclidean point rotation group, and is the group homology. Sydler's theorem that volume and the Dehn invariant are the only invariants for Euclidean dissection is represented homologically by the statement that the group appearing in this sequence is actually zero. If it were nonzero, its image in the group of polyhedra would give a family of polyhedra that are not dissectable to a cube of the same volume but that have zero Dehn invariant. By Sydler's theorem, such polyhedra do not exist.
The group appearing towards the right of the exact sequence is isomorphic to the group of Kähler differentials, and the map from tensor products of lengths and angles to Kähler differentials is given by
where is the universal derivation of . This group is an obstacle to realizability: its nonzero elements come from elements of that cannot be realized as Dehn invariants.
Analogously, in hyperbolic or spherical space, the realizable Dehn invariants do not necessarily form a vector space, because scalar multiplication is no longer possible, but they still form a subgroup. Dupont and Sah prove the existence of the exact sequences
Here denotes the special linear group, and is the group of Möbius transformations; the superscript minus-sign "indicates the (−1)-eigenspace for the involution induced by complex conjugation". denotes the special unitary group. The subgroup in is the group generated by the whole sphere. Again, the rightmost nonzero group in these sequences is the obstacle to realizability of a value in as a Dehn invariant.
An approach very similar to the Dehn invariant can be used to determine whether two rectilinear polygons can be dissected into each other only using axis-parallel cuts and translations (rather than cuts at arbitrary angles and rotations). An invariant for this kind of dissection uses the the tensor product where the left and right terms in the product represent height and width of rectangles. The invariant for any given polygon is calculated by cutting the polygon into rectangles, taking the tensor product of the height and width of each rectangle, and adding the results. Again, a dissection is possible if and only if two polygons have the same area and the same invariant.
|Unsolved problem in mathematics:
Must the Dehn invariant of a flexible polyhedron stay invariant as it flexes?
(more unsolved problems in mathematics)
Flexible polyhedra are a class of polyhedra that can undergo a continuous motion that preserves the shape of their faces. By Cauchy's rigidity theorem, they must be non-convex, and it is known (the "bellows theorem") that the volume of the polyhedron must stay constant throughout this motion. A stronger version of this theorem is conjectured, stating that the Dehn invariant of such a polyhedron must also remain invariant throughout any continuous motion. This conjecture is called the "strong bellows conjecture". It is known to be true for the first known flexible polyhedra, the (self-intersecting) Bricard octahedra, and for a non-self-intersecting flexible polyhedron derived from them, Steffen's polyhedron. However, it remains an open problem for flexible polyhedra more generally.
The total mean curvature of a polyhedral surface has been defined as the sum over the edges of the edge lengths multiplied by the exterior dihedral angles. Thus (for polyhedra without rational angles) it is a linear function of the Dehn invariant, although it does not provide full information about the Dehn invariant. It has been proven to remain constant for any flexing polyhedron.
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- Essentially the same formula, but with tensor notation used for the unit vectors, appears in Fuchs, Dmitry; Tabachnikov, Serge (2007), Mathematical Omnibus: Thirty lectures on classic mathematics, Providence, RI: American Mathematical Society, p. 312, doi:10.1090/mbk/046, ISBN 978-0-8218-4316-1, MR 2350979. As that source notes, the fact that the second sum is indexed starting from 1 instead of 0 is not a mistake; this indexing is used deliberately, to omit the term corresponding to the rational multiples of π.
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- See Table of polyhedron dihedral angles.
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- Dupont (2001), p. 6.
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- This argument applies whenever the proportions of the tiles can be defined as a limit point of the numbers of tiles within larger polyhedra; see Lagarias & Moews (1995), Equation (4.2), and the surrounding discussion.
- Dupont (2001), p. 7.
- Dupont (2001), Theorem 6.2(a), p. 35. Dupont states that this is "a reformulation of a result of Jessen (1968)".
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