Affine involution

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In Euclidean geometry, of special interest are involutions which are linear or affine transformations over the Euclidean space Template:Tmath Such involutions are easy to characterize and they can be described geometrically.[1]

Linear involutions

To give a linear involution is the same as giving an involutory matrix, a square matrix Template:Math such that 𝐀2=𝐈(1) where Template:Math is the identity matrix.

It is a quick check that a square matrix Template:Math whose elements are all zero off the main diagonal and ±1 on the diagonal, that is, a signature matrix of the form

𝐃=(±10000±10000±10000±1)

satisfies (1), i.e. is the matrix of a linear involution. It turns out that all the matrices satisfying (1) are of the form 𝐀=𝐔1𝐃𝐔, where Template:Math is invertible and Template:Math is as above. That is to say, the matrix of any linear involution is of the form Template:Math 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 Template:Mvar hyperplanes going through the origin. (The term oblique reflection as used here includes ordinary reflections.)

One can easily verify that Template:Math represents a linear involution if and only if Template:Math has the form 𝐀=±(2𝐏𝐈) for a linear projection Template:Math.

Affine involutions

If A represents a linear involution, then xA(xb)+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 (see above), 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.[2]

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 (in 2D, 3D, and up; this is in 2D a reflection, and in 3D a rotation about the line by 180°), inversion in a plane (in 3D and up; in 3D this is a reflection in a plane), inversion in a 3D space (in 3D: the identity), etc.

References

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