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 [itex]SO(n)[/itex]. 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 [itex]R^n[/itex] 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 [itex]SO(3)[/itex] will usually have "rotation axes" pointing in different directions. However, the elements of [itex]SO(n)[/itex] 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 [itex]R^n[/itex].
Once this theorem is established, it is easy to see how to modify it to obtain a similar decomposition for any element of [itex]O(n)[/itex].
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 [itex]O(n)[/itex] look like and how they act on [itex]R^n[/itex]
(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 [itex]R^5[/itex]. Geometrically speaking, the effect of this element of [itex]SO(5)[/itex] 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 [itex]R^5[/itex]. Senechal cites P. Engel,
Geometric Crystallography, Reidel, 1986.)