Definition 1.
An isometry of is a distance preserving map from to itself, a map such that, for all and in ,
Artin composes isometries from the right.
Lemma 2.
Let and be points in . If the three dot products , , and are equal, then .
Theorem 3.
The following conditions on a map are equivalent:
- is an isometry that fixes the origin:
- preserves dot products: for all and ,
- is an orthogonal linear operator.
Corollary
Every isometry of is the composition of an orthogonal linear operator and a translation.
More precisely, if is an isometry and if , then where is a translation and is an orthogonal linear operator. This expression for is unique.
Corollary
The set of all isometries of forms a group that we denote by , with the composition of functions as its law of composition
There is an important map , defined by dropping the translation part of an isometry .
Theorem 4(Proposition).
The map is a surjective homomorphism. Its kernel is the set of translations, which is a normal subgroup of .
Change of coordinates
Let denote an -dimensional space. To analyze the effect of such a change, we begin with an isometry , a point of , and its image , without reference to coordinates. Now, suppose we introduce a coordinate system of . The space becomes identified with , and the points and have coordinates and . The isometry will have a formula in terms of the coordinates; call it : . We want to determine what happens to the coordinate vectors and to the formula when we change coordinates by an isometry.
Say we change our coordinates by some isometry of , such that , where would be the new basis. Substituting for and in the old formula, we get
so .
Isometries of the plane
Theorem 5.
Every isometry of the plane has one of the following forms:
(a) Orientation preserving symmetries:
- Translation: A map that sends .
- Rotation: rotation of the plane through a nonzero angle about some point.
(b) orientation-reversing isometries:
3. Reflection: a bilateral symmetry about a line
4. glide reflection: a reflection about a line , followed by translation by a nonzero vector parallel to .