Affine group

Short description: Group of all affine transformations of an affine space

In mathematics, the affine group or general affine group of any affine space is the group of all invertible affine transformations from the space into itself. In the case of a Euclidean space (where the associated field of scalars is the real numbers), the affine group consists of those functions from the space to itself such that the image of every line is a line.

Over any field, the affine group may be viewed as a matrix group in a natural way. If the associated field of scalars the real or complex field, then the affine group is a Lie group.

Relation to general linear group

Construction from general linear group

Concretely, given a vector space V, it has an underlying affine space A obtained by "forgetting" the origin, with V acting by translations, and the affine group of A can be described concretely as the semidirect product of V by GL(V), the general linear group of V:

[math]\displaystyle{ \operatorname{Aff}(V) = V \rtimes \operatorname{GL}(V) }[/math]

The action of GL(V) on V is the natural one (linear transformations are automorphisms), so this defines a semidirect product.

In terms of matrices, one writes:

[math]\displaystyle{ \operatorname{Aff}(n,K) = K^n \rtimes \operatorname{GL}(n,K) }[/math]

where here the natural action of GL(n, K) on Kⁿ is matrix multiplication of a vector.

Stabilizer of a point

Given the affine group of an affine space A, the stabilizer of a point p is isomorphic to the general linear group of the same dimension (so the stabilizer of a point in Aff(2, R) is isomorphic to GL(2, R)); formally, it is the general linear group of the vector space (A, p): recall that if one fixes a point, an affine space becomes a vector space.

All these subgroups are conjugate, where conjugation is given by translation from p to q (which is uniquely defined), however, no particular subgroup is a natural choice, since no point is special – this corresponds to the multiple choices of transverse subgroup, or splitting of the short exact sequence

[math]\displaystyle{ 1 \to V \to V \rtimes \operatorname{GL}(V) \to \operatorname{GL}(V) \to 1\,. }[/math]

In the case that the affine group was constructed by starting with a vector space, the subgroup that stabilizes the origin (of the vector space) is the original GL(V).

Matrix representation

Representing the affine group as a semidirect product of V by GL(V), then by construction of the semidirect product, the elements are pairs (v, M), where v is a vector in V and M is a linear transform in GL(V), and multiplication is given by

[math]\displaystyle{ (v, M) \cdot (w, N) = (v+Mw, MN)\,. }[/math]

This can be represented as the (n + 1) × (n + 1) block matrix

[math]\displaystyle{ \left( \begin{array}{c|c} M & v\\ \hline 0 & 1 \end{array}\right) }[/math]

where M is an n × n matrix over K, v an n × 1 column vector, 0 is a 1 × n row of zeros, and 1 is the 1 × 1 identity block matrix.

Formally, Aff(V) is naturally isomorphic to a subgroup of GL(V ⊕ K), with V embedded as the affine plane {(v, 1) | v ∈ V}, namely the stabilizer of this affine plane; the above matrix formulation is the (transpose of) the realization of this, with the n × n and 1 × 1) blocks corresponding to the direct sum decomposition V ⊕ K.

A similar representation is any (n + 1) × (n + 1) matrix in which the entries in each column sum to 1. The similarity P for passing from the above kind to this kind is the (n + 1) × (n + 1) identity matrix with the bottom row replaced by a row of all ones.

Each of these two classes of matrices is closed under matrix multiplication.

The simplest paradigm may well be the case n = 1, that is, the upper triangular 2 × 2 matrices representing the affine group in one dimension. It is a two-parameter non-Abelian Lie group, so with merely two generators (Lie algebra elements), A and B, such that [A, B] = B, where

[math]\displaystyle{ A= \left( \begin{array}{cc} 1 & 0\\ 0 & 0 \end{array}\right), \qquad B= \left( \begin{array}{cc} 0 & 1\\ 0 & 0 \end{array}\right)\,, }[/math]

so that

[math]\displaystyle{ e^{aA+bB}= \left( \begin{array}{cc} e^a & \tfrac{b}{a}(e^a-1)\\ 0 & 1 \end{array}\right)\,. }[/math]

Character table of Aff(F_p)

Aff(F_p) has order p(p − 1). Since

[math]\displaystyle{ \begin{pmatrix} c & d \\ 0 & 1 \end{pmatrix}\begin{pmatrix} a & b \\ 0 & 1 \end{pmatrix}\begin{pmatrix} c & d \\ 0 & 1 \end{pmatrix}^{-1}=\begin{pmatrix} a & (1-a)d+bc \\ 0 & 1 \end{pmatrix}\,, }[/math]

we know Aff(F_p) has p conjugacy classes, namely

[math]\displaystyle{ \begin{align} C_{id} &= \left\{\begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix}\right\}\,, \\[6pt] C_{1} &= \left\{\begin{pmatrix} 1 & b \\ 0 & 1 \end{pmatrix}\Bigg|b\in \mathbf{F}_p^*\right\}\,, \\[6pt] \Bigg\{C_{a} &= \left\{\begin{pmatrix} a & b \\ 0 & 1 \end{pmatrix}\Bigg| b\in \mathbf{F}_p\right\}\Bigg|a\in \mathbf{F}_p\setminus\{0,1\}\Bigg\}\,. \end{align} }[/math]

Then we know that Aff(F_p) has p irreducible representations. By above paragraph (§ Matrix representation), there exist p − 1 one-dimensional representations, decided by the homomorphism

[math]\displaystyle{ \rho_k:\operatorname{Aff}(\mathbf{F}_p)\to\Complex^* }[/math]

for k = 1, 2,… p − 1, where

[math]\displaystyle{ \rho_k\begin{pmatrix} a & b \\ 0 & 1 \end{pmatrix}=\exp\left(\frac{2i kj\pi}{p-1}\right) }[/math]

and i² = −1, a = g^j, g is a generator of the group F∗p. Then compare with the order of F_p, we have

[math]\displaystyle{ p(p-1)=p-1+\chi_p^2\,, }[/math]

hence χ_p = p − 1 is the dimension of the last irreducible representation. Finally using the orthogonality of irreducible representations, we can complete the character table of Aff(F_p):

[math]\displaystyle{ \begin{array}{c|cccccc} & {\color{Blue}C_{id}} & {\color{Blue}C_1} & {\color{Blue}C_g} & {\color{Blue}C_{g^2}} & {\color{Gray}\dots} & {\color{Blue}C_{g^{p-2}}} \\ \hline {\color{Blue}\chi_1} & {\color{Gray}1} & {\color{Gray}1} & {\color{Blue}e^{\frac{2\pi i}{p-1}}} & {\color{Blue}e^{\frac{4\pi i}{p-1}}} & {\color{Gray}\dots} & {\color{Blue}e^{\frac{2\pi (p-2)i}{p-1}}} \\ {\color{Blue}\chi_2} & {\color{Gray}1} & {\color{Gray}1} & {\color{Blue}e^{\frac{4\pi i}{p-1}}} & {\color{Blue}e^{\frac{8\pi i}{p-1}}} & {\color{Gray}\dots} & {\color{Blue}e^{\frac{4\pi (p-2)i}{p-1}}} \\ {\color{Blue}\chi_3} & {\color{Gray}1} & {\color{Gray}1} & {\color{Blue}e^{\frac{6\pi i}{p-1}}} & {\color{Blue}e^{\frac{12\pi i}{p-1}}} & {\color{Gray}\dots} & {\color{Blue}e^{\frac{6\pi (p-2)i}{p-1}}} \\ {\color{Gray}\dots} & {\color{Gray}\dots} & {\color{Gray}\dots} & {\color{Gray}\dots} & {\color{Gray}\dots} & {\color{Gray}\dots} & {\color{Gray}\dots} \\ {\color{Blue}\chi_{p-1}} & {\color{Gray}1} & {\color{Gray}1} & {\color{Gray}1} & {\color{Gray}1} & {\color{Gray}\dots} & {\color{Gray}1} \\ {\color{Blue}\chi_{p}} & {\color{Gray}p-1} & {\color{Gray}-1} & {\color{Gray}0} & {\color{Gray}0} & {\color{Gray}\dots} & {\color{Gray}0} \end{array} }[/math]

Planar affine group over the reals

The elements of [math]\displaystyle{ \operatorname{Aff}(2,\mathbb R) }[/math] can take a simple form on a well-chosen affine coordinate system. More precisely, given an affine transformation of an affine plane over the reals, an affine coordinate system exists on which it has one of the following forms, where a, b, and t are real numbers (the given conditions insure that transformations are invertible, but not for making the classes distinct; for example, the identity belongs to all the classes).

[math]\displaystyle{ \begin{align} \text{1.}&& (x, y) &\mapsto (x +a,y+b),\\[3pt] \text{2.}&& (x, y) &\mapsto (ax,by), &\qquad \text{where } ab\ne 0,\\[3pt] \text{3.}&& (x, y) &\mapsto (ax,y+b), &\qquad \text{where } a\ne 0,\\[3pt] \text{4.}&& (x, y) &\mapsto (ax+y,ay), &\qquad \text{where } a\ne 0,\\[3pt] \text{5.}&& (x, y) &\mapsto (x+y,y+a)\\[3pt] \text{6.}&& (x, y) &\mapsto (a(x\cos t + y\sin t), a(-x\sin t+y\cos t)), &\qquad \text{where } a\ne 0. \end{align} }[/math]

Case 1 corresponds to translations.

Case 2 corresponds to scalings that may differ in two different directions. When working with a Euclidean plane these directions need not be perpendicular, since the coordinate axes need not be perpendicular.

Case 3 corresponds to a scaling in one direction and a translation in another one.

Case 4 corresponds to a shear mapping combined with a dilation.

Case 5 corresponds to a shear mapping combined with a dilation.

Case 6 corresponds to similarities when the coordinate axes are perpendicular.

The affine transformations without any fixed point belong to cases 1, 3, and 5. The transformations that do not preserve the orientation of the plane belong to cases 2 (with ab < 0) or 3 (with a < 0).

The proof may be done by first remarking that if an affine transformation has no fixed point, then the matrix of the associated linear map has an eigenvalue equal to one, and then using the Jordan normal form theorem for real matrices.

Other affine groups and subgroups

General case

Given any subgroup G < GL(V) of the general linear group, one can produce an affine group, sometimes denoted Aff(G), analogously as Aff(G) := V ⋊ G.

More generally and abstractly, given any group G and a representation [math]\displaystyle{ \rho : G \to \operatorname{GL}(V) }[/math] of G on a vector space V, one gets an associated affine group V ⋊_ρ G: one can say that the affine group obtained is "a group extension by a vector representation", and, as above, one has the short exact sequence [math]\displaystyle{ 1 \to V \to V \rtimes_\rho G \to G \to 1. }[/math]

Special affine group

The subset of all invertible affine transformations that preserve a fixed volume form up to sign is called the special affine group. (The transformations themselves are sometimes called equiaffinities.) This group is the affine analogue of the special linear group. In terms of the semi-direct product, the special affine group consists of all pairs (M, v) with [math]\displaystyle{ |\det(M)| = 1 }[/math], that is, the affine transformations [math]\displaystyle{ x \mapsto Mx + v }[/math] where M is a linear transformation of whose determinant has absolute value 1 and v is any fixed translation vector.

The subgroup of the special affine group consisting of those transformations whose linear part has determinant 1 is the group of orientation- and volume-preserving maps. Algebraically, this group is a semidirect product [math]\displaystyle{ SL(V) \ltimes V }[/math] of the special linear group of [math]\displaystyle{ V }[/math] with the translations. It is generated by the shear mappings.

Projective subgroup

Presuming knowledge of projectivity and the projective group of projective geometry, the affine group can be easily specified. For example, Günter Ewald wrote:

The set [math]\displaystyle{ \mathfrak{P} }[/math] of all projective collineations of Pⁿ is a group which we may call the projective group of Pⁿ. If we proceed from Pⁿ to the affine space Aⁿ by declaring a hyperplane ω to be a hyperplane at infinity, we obtain the affine group [math]\displaystyle{ \mathfrak{A} }[/math] of Aⁿ as the subgroup of [math]\displaystyle{ \mathfrak{P} }[/math] consisting of all elements of [math]\displaystyle{ \mathfrak{P} }[/math] that leave ω fixed.

[math]\displaystyle{ \mathfrak{A} \subset \mathfrak{P} }[/math]

Isometries of Euclidean space

When the affine space A is a Euclidean space (over the field of real numbers), the group [math]\displaystyle{ \mathcal{E} }[/math] of distance-preserving maps (isometries) of A is a subgroup of the affine group. Algebraically, this group is a semidirect product [math]\displaystyle{ O(V) \ltimes V }[/math] of the orthogonal group of [math]\displaystyle{ V }[/math] with the translations. Geometrically, it is the subgroup of the affine group generated by the orthogonal reflections.

Poincaré group

The Poincaré group is the affine group of the Lorentz group O(1,3):

[math]\displaystyle{ \mathbf{R}^{1,3}\rtimes \operatorname{O}(1,3) }[/math]

This example is very important in relativity.

See also

• Affine Coxeter group – certain discrete subgroups of the affine group on a Euclidean space that preserve a lattice
• Holomorph

References

• Lyndon, Roger (1985). "Section VI.1". Groups and Geometry. Cambridge University Press. ISBN 0-521-31694-4. https://archive.org/details/groupsgeometry0000lynd.