Special linear group

Cayley table of SL(2,3).

In mathematics, the special linear group of degree n over a field F is the set of n × n matrices with determinant 1, with the group operations of ordinary matrix multiplication and matrix inversion. This is the normal subgroup of the general linear group given by the kernel of the determinant

\det\colon \operatorname{GL}(n, F) \to F^\times.

where we write F× for the multiplicative group of F (that is, F excluding 0).

These elements are "special" in that they fall on a subvariety of the general linear group – they satisfy a polynomial equation (since the determinant is polynomial in the entries).

Geometric interpretation

The special linear group SL(n, R) can be characterized as the group of volume and orientation preserving linear transformations of Rn; this corresponds to the interpretation of the determinant as measuring change in volume and orientation.

Lie subgroup

When F is R or C, SL(n, F) is a Lie subgroup of GL(n, F) of dimension n2 − 1. The Lie algebra \mathfrak{sl}(n, F) of SL(n, F) consists of all n × n matrices over F with vanishing trace. The Lie bracket is given by the commutator.

Topology

Any invertible matrix can be uniquely represented according to the polar decomposition as the product of a unitary matrix and a hermitian matrix with positive eigenvalues. The determinant of the unitary matrix is on the unit circle while that of the hermitian matrix is real and positive and, since, in the case of a matrix from the special linear group the product of these two determinants must be 1, then each of them must be 1. Therefore, a special linear matrix can be written as the product of a special unitary matrix (or special orthogonal matrix in the real case) and a positive definite hermitian matrix (or symmetric matrix in the real case) having determinant 1.

Thus the topology of the group SL(n, C) is the product of the topology of SU(n) and the topology of the group of hermitian matrices of unit determinant with positive eigenvalues. A hermitian matrix of unit determinant and having positive eigenvalues can be uniquely expressed as the exponential of a traceless hermitian matrix, and therefore the topology of this is that of (n2 − 1)-dimensional Euclidean space.

The topology of SL(n, R) is the product of the topology of SO(n) and the topology of the group of symmetric matrices with positive eigenvalues and unit determinant. Since the latter matrices can be uniquely expressed as the exponential of symmetric traceless matrices, then this latter topology is that of (n + 2)(n − 1)/2-dimensional Euclidean space.

The group SL(n, C), like SU(n), is simply connected while SL(n, R), like SO(n), is not. SL(n, R) has the same fundamental group as GL+(n, R) or SO(n), that is, Z for n = 2 and Z2 for n > 2.

Relations to other subgroups of GL(n,A)

Two related subgroups, which in some cases coincide with SL, and in other cases are accidentally conflated with SL, are the commutator subgroup of GL, and the group generated by transvections. These are both subgroups of SL (transvections have determinant 1, and det is a map to an abelian group, so [GL, GL] ≤ SL), but in general do not coincide with it.

The group generated by transvections is denoted E(n, A) (for elementary matrices) or TV(n, A). By the second Steinberg relation, for n ≥ 3, transvections are commutators, so for n ≥ 3, E(n, A) ≤ [GL(n, A), GL(n, A)].

For n = 2, transvections need not be commutators (of 2 × 2 matrices), as seen for example when A is F2, the field of two elements, then

\operatorname{Alt}(3) \cong [\operatorname{GL}(2, \mathbf{F}_2),\operatorname{GL}(2, \mathbf{F}_2)] < \operatorname{E}(2, \mathbf{F}_2) = \operatorname{SL}(2, \mathbf{F}_2) = \operatorname{GL}(2, \mathbf{F}_2) \cong \operatorname{Sym}(3),

where Alt(3) and Sym(3) denote the alternating resp. symmetric group on 3 letters.

However, if A is a field with more than 2 elements, then E(2, A) = [GL(2, A), GL(2, A)], and if A is a field with more than 3 elements, E(2, A) = [SL(2, A), SL(2, A)].

In some circumstances these coincide: the special linear group over a field or a Euclidean domain is generated by transvections, and the stable special linear group over a Dedekind domain is generated by transvections. For more general rings the stable difference is measured by the special Whitehead group SK1(A) := SL(A)/E(A), where SL(A) and E(A) are the stable groups of the special linear group and elementary matrices.

Generators and relations

If working over a ring where SL is generated by transvections (such as a field or Euclidean domain), one can give a presentation of SL using transvections with some relations. Transvections satisfy the Steinberg relations, but these are not sufficient: the resulting group is the Steinberg group, which is not the special linear group, but rather the universal central extension of the commutator subgroup of GL.

A sufficient set of relations for SL(n, Z) for n ≥ 3 is given by two of the Steinberg relations, plus a third relation (Conder, Robertson & Williams 1992, p. 19). Let Tij := eij(1) be the elementary matrix with 1's on the diagonal and in the ij position, and 0's elsewhere (and i ≠ j). Then

\begin{align} \left[ T_{ij},T_{jk} \right] &= T_{ik} && \mbox{for } i \neq k\\ \left[ T_{ij},T_{kl} \right] &= \mathbf{1} && \mbox{for } i \neq l, j \neq k\\ (T_{12}T_{21}^{-1}T_{12})^4 &= \mathbf{1}\\ \end{align}

are a complete set of relations for SL(n, Z), n ≥ 3.

Structure of GL(n,F)

The group GL(n, F) splits over its determinant (we use F× ≅ GL(1, F) → GL(n, F) as the monomorphism from F× to GL(n, F), see semidirect product), and therefore GL(n, F) can be written as a semidirect product of SL(n, F) by F×:

GL(n, F) = SL(n, F) ⋊ F×.

See also

References

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