In mathematics, the Dehn–Sommerville equations are a complete set of linear relations between the numbers of faces of different dimension of a simplicial polytope. For polytopes of dimension 4and 5, they were found by Max Dehn in 1905. Their general form was established by Duncan Sommerville in 1927. The Dehn–Sommerville equations can be restated as a symmetrycondition for the h-vector'' of the simplicial polytope and this has become the standard formulation in recent combinatorics literature. By duality, analogous equations hold for simple polytopes.
Statement
Let P be a d-dimensional simplicial polytope. For i = 0, 1,..., d−1, letfidenote the number of i-dimensional faces of P. The sequence is called the f-vector of the polytope P. Additionally, set Then for any k = −1, 0,..., d−2, the following Dehn–Sommerville equation holds: When k = −1, it expresses the fact that Euler characteristic of a -dimensional simplicial sphere is equal to 1 + d−1. Dehn–Sommerville equations with different k are not independent. There are several ways to choose a maximal independent subsetconsisting of equations. If d is even then the equations with k = 0, 2, 4,..., d−2 are independent. Another independent set consists of the equations with k = −1, 1, 3,..., d−3. If d is odd then the equations with k = −1, 1, 3,..., d−2 form one independent set and the equations with k = −1, 0, 2, 4,..., d−3 form another.
Equivalent formulations
Sommerville found a different way to state these equations: where 0 ≤ k ≤. This can be further facilitated introducing the notion of h-vector of P. For k = 0, 1,..., d, let The sequence is called the h-vector of P. The f-vector and the h-vector uniquely determine each other through the relation Then the Dehn–Sommerville equations can be restated simply as The equations with 0 ≤ k ≤ are independent, and the others are manifestly equivalent to them. Richard Stanley gave an interpretation of the components of the h-vector of a simplicial convex polytopeP in terms of the projectivetoric varietyX associated with P. Namely, they are the dimensions of the even intersectioncohomology groups of X: . In this language, the last form of the Dehn–Sommerville equations, the symmetry of the h-vector, is a manifestation of the Poincaré duality in the intersection cohomology of X.