Affine involution
In Euclidean geometry, of special interest are involutions which are linear or affine transformations over the Euclidean space. Such involutions are easy to characterize and they can be described geometrically.
Linear involutions
To give a linear involution is the same as giving an involutory matrix, a square matrix such thatwhere is the identity matrix.
It is a quick check that a square matrix whose elements are all zero off the main diagonal and ±1 on the diagonal, that is, a signature matrix of the form
satisfies, i.e. is the matrix of a linear involution. It turns out that all the matrices satisfying are of the form
where is invertible and is as above. That is to say, the matrix of any linear involution is of the form up to a matrix similarity. Geometrically this means that any linear involution can be obtained by taking oblique reflections against any number from 0 through hyperplanes going through the origin.
One can easily verify that represents a linear involution if and only if has the form
for a linear projection.
Affine involutions
If A represents a linear involution, then x→''A+b'' is an affine involution. One can check that any affine involution in fact has this form. Geometrically this means that any affine involution can be obtained by taking oblique reflections against any number from 0 through n hyperplanes going through a point b.Affine involutions can be categorized by the dimension of the affine space of fixed points; this corresponds to the number of values 1 on the diagonal of the similar matrix D, i.e., the dimension of the eigenspace for eigenvalue 1.
The affine involutions in 3D are:
- the identity
- the oblique reflection in respect to a plane
- the oblique reflection in respect to a line
- the reflection in respect to a point.
Isometric involutions
In the case that the eigenspace for eigenvalue 1 is the orthogonal complement of that for eigenvalue −1, i.e., every eigenvector with eigenvalue 1 is orthogonal to every eigenvector with eigenvalue −1, such an affine involution is an isometry. The two extreme cases for which this always applies are the identity function and inversion in a point.The other involutive isometries are inversion in a line, inversion in a plane, inversion in a 3D space, etc.