The one theorem everyone should know concerning orthogonal matrices
Everyone knows that a surprising fact about three dimensional special orthogonal matrices is that they fix
pointwise a one-dimensional subspace and act in the orthogonal two-dimensional subspace just like a two-dimensional rotation. But what is the n-dimensional generalization?
Consider a block diagonal matrix with one two by two block, which is an ordinary two-dimensional rotation matrix, plus ones down the diagonal. Call this a "rotation matrix"; it is a special case of a "special orthogonal matrix", i.e. an element of SO(n). Geometrically, it fixes
pointwise a codimension two subspace orthogonal to the two-plane, and acts like a two-dimensional rotation orthogonal to this "axis". It is possible to decompose a special orthogonal matrix as a product of "rotation matrices" all respecting a particular orthogonal direct sum decomposition of the vector space R^n into two-dimensional subspaces (with a one-dimensional pointwise fixed subspace left over in case of odd dimension). In general, two distinct special orthogonal matrices will require two distinct orthogonal direct sum decompositions; this observation generalizes the fact that two elements of SO(3) will usually have "rotation axes" pointing in different directions. However, the elements of SO(n) which do share such a decomposition form an abelian subgroup. This in fact gives a large conjugacy class of abelian subgroups
An interesting example: apply this idea to the permutation matrix corresponding to an n-cycle in R^n.
Once this theorem is established, it is easy to see how to modify it to obtain a similar decomposition for any element of O(n).
I just checked two dozen books which discuss the orthogonal group, including Birkhoff and Mac Lane,
A Survey of Modern Algebra (chapter 9), Armstrong,
Groups and Symmetry (chapters 9 and 19), Neumann, Stoy and Thompson,
Groups and Geometry (chapters 14,15), Jacobson,
Basic Algebra I (chapter 9), and Artin,
Geometric Algebra (chapter III) and unfortunately was unable to find any mention of this. Wikipedia doesn't mention anything like this either. Yet it is a quite well known nineteenth century theorem. Go figure...
This is perhaps the most elementary thing one can say in discussing what elements of the orthogonal group O(n) look like and how they act on R^n
(Edit: finally found a citation for you. The theorem is stated without proof in Senechal,
Quasicrystals and Geometry, Prop 2.12, p. 47; see p. 63 for the decomposition of a five-cycle in R^5. Geometrically speaking, the effect of this element of SO(5) respects an orthogonal direct sum decomposition into one pointwise fixed line plus two two-dimensional subspaces; it acts like a one-fifth turn in one of these, and like a two-fifth turn in the other. By linearity this description extends to all of R^5. Senechal cites P. Engel,
Geometric Crystallography, Reidel, 1986.)