In
mathematics
Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, the general linear group of degree
is the set of
invertible matrices, together with the operation of ordinary
matrix multiplication. This forms a
group, because the product of two invertible matrices is again invertible, and the inverse of an invertible matrix is invertible, with the identity matrix as the identity element of the group. The group is so named because the columns (and also the rows) of an invertible matrix are
linearly independent, hence the vectors/points they define are in
general linear position, and matrices in the general linear group take points in general linear position to points in general linear position.
To be more precise, it is necessary to specify what kind of objects may appear in the entries of the matrix. For example, the general linear group over
(the set of
real numbers) is the group of
invertible matrices of real numbers, and is denoted by
or
.
More generally, the general linear group of degree
over any
field (such as the
complex numbers), or a
ring (such as the ring of
integers), is the set of
invertible matrices with entries from
(or
), again with matrix multiplication as the group operation.
[Here rings are assumed to be associative and unital.] Typical notation is
or
, or simply
if the field is understood.
More generally still, the
general linear group of a vector space is the
automorphism group, not necessarily written as matrices.
The
special linear group, written
or
, is the
subgroup of
consisting of matrices with a
determinant
In mathematics, the determinant is a Scalar (mathematics), scalar-valued function (mathematics), function of the entries of a square matrix. The determinant of a matrix is commonly denoted , , or . Its value characterizes some properties of the ...
of 1.
The group
and its
subgroups are often called linear groups or matrix groups (the automorphism group
is a linear group but not a matrix group). These groups are important in the theory of
group representations, and also arise in the study of spatial
symmetries and symmetries of
vector spaces in general, as well as the study of
polynomials. The
modular group may be realised as a quotient of the special linear group
.
If
, then the group
is not
abelian.
General linear group of a vector space
If
is a
vector space over the field
, the general linear group of
, written
or
, is the group of all
automorphisms of
, i.e. the set of all
bijective linear transformations
, together with functional composition as group operation. If
has finite
dimension , then
and
are
isomorphic. The isomorphism is not canonical; it depends on a choice of
basis in
. Given a basis
of
and an automorphism
in
, we have then for every basis vector ''e''
''i'' that
:
for some constants
in
; the matrix corresponding to
is then just the matrix with entries given by the
.
In a similar way, for a commutative ring
the group
may be interpreted as the group of automorphisms of a ''
free''
-module
of rank
. One can also define GL(''M'') for any
-module, but in general this is not isomorphic to
(for any
).
In terms of determinants
Over a field
, a matrix is
invertible if and only if its
determinant
In mathematics, the determinant is a Scalar (mathematics), scalar-valued function (mathematics), function of the entries of a square matrix. The determinant of a matrix is commonly denoted , , or . Its value characterizes some properties of the ...
is nonzero. Therefore, an alternative definition of
is as the group of matrices with nonzero determinant.
Over a
commutative ring , more care is needed: a matrix over
is invertible if and only if its determinant is a
unit in
, that is, if its determinant is invertible in
. Therefore,
may be defined as the group of matrices whose determinants are units.
Over a non-commutative ring
, determinants are not at all well behaved. In this case,
may be defined as the
unit group of the
matrix ring .
As a Lie group
Real case
The general linear group
over the field of
real numbers is a real
Lie group of dimension
. To see this, note that the set of all
real matrices,
, forms a
real vector space of dimension
. The subset
consists of those matrices whose
determinant
In mathematics, the determinant is a Scalar (mathematics), scalar-valued function (mathematics), function of the entries of a square matrix. The determinant of a matrix is commonly denoted , , or . Its value characterizes some properties of the ...
is non-zero. The determinant is a
polynomial map, and hence
is an
open affine subvariety of
(a
non-empty open subset of
in the
Zariski topology), and therefore
a
smooth manifold of the same dimension.
The
Lie algebra
In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi ident ...
of
, denoted
consists of all
real matrices with the
commutator serving as the Lie bracket.
As a manifold,
is not
connected but rather has two
connected components: the matrices with positive determinant and the ones with negative determinant. The
identity component, denoted by
, consists of the real
matrices with positive determinant. This is also a Lie group of dimension
; it has the same Lie algebra as
.
The
polar decomposition, which is unique for invertible matrices, shows that there is a homeomorphism between
and the Cartesian product of
with the set of positive-definite symmetric matrices. Similarly, it shows that there is a homeomorphism between
and the Cartesian product of
with the set of positive-definite symmetric matrices. Because the latter is contractible, the
fundamental group of
is isomorphic to that of
.
The homeomorphism also shows that the group
is
noncompact. “The”
maximal compact subgroup
In mathematics
Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. T ...
of
is the
orthogonal group , while "the" maximal compact subgroup of
is the
special orthogonal group . As for
, the group
is not
simply connected (except when
, but rather has a
fundamental group isomorphic to
for
or
for
.
Complex case
The general linear group over the field of
complex numbers,
, is a ''complex''
Lie group of complex dimension
. As a real Lie group (through realification) it has dimension
. The set of all real matrices forms a real Lie subgroup. These correspond to the inclusions
:
,
which have real dimensions
,
, and
. Complex
-dimensional matrices can be characterized as real
-dimensional matrices that preserve a
linear complex structure; that is, matrices that commute with a matrix
such that
, where
corresponds to multiplying by the imaginary unit
.
The
Lie algebra
In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi ident ...
corresponding to
consists of all
complex matrices with the
commutator serving as the Lie bracket.
Unlike the real case,
is
connected. This follows, in part, since the multiplicative group of complex numbers
is connected. The group manifold
is not compact; rather its
maximal compact subgroup
In mathematics
Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. T ...
is the
unitary group . As for
, the group manifold
is not
simply connected but has a
fundamental group isomorphic to
.
Over finite fields
If
is a
finite field with
elements, then we sometimes write
instead of
. When ''p'' is prime,
is the
outer automorphism group of the group
, and also the
automorphism group, because
is abelian, so the
inner automorphism group is trivial.
The order of
is:
:
This can be shown by counting the possible columns of the matrix: the first column can be anything but the zero vector; the second column can be anything but the multiples of the first column; and in general, the
th column can be any vector not in the
linear span of the first
columns. In
''q''-analog notation, this is
.
For example, has order . It is the automorphism group of the
Fano plane and of the group
. This group is also isomorphic to .
More generally, one can count points of
Grassmannian over
: in other words the number of subspaces of a given dimension
. This requires only finding the order of the
stabilizer subgroup of one such subspace and dividing into the formula just given, by the
orbit-stabilizer theorem.
These formulas are connected to the
Schubert decomposition of the Grassmannian, and are
''q''-analogs of the
Betti numbers of complex Grassmannians. This was one of the clues leading to the
Weil conjectures.
Note that in the limit
the order of
goes to 0! – but under the correct procedure (dividing by
) we see that it is the order of the symmetric group (see Lorscheid's article). In the philosophy of the
field with one element, one thus interprets the
symmetric group as the general linear group over the field with one element:
.
History
The general linear group over a prime field,
, was constructed and its order computed by
Évariste Galois in 1832, in his last letter (to Chevalier) and second (of three) attached manuscripts, which he used in the context of studying the
Galois group of the general equation of order
.
Special linear group
The ''special linear group'',
, is the group of all matrices with
determinant
In mathematics, the determinant is a Scalar (mathematics), scalar-valued function (mathematics), function of the entries of a square matrix. The determinant of a matrix is commonly denoted , , or . Its value characterizes some properties of the ...
1. These matrices are special in that they lie on a
subvariety: they satisfy a polynomial equation (as the determinant is a polynomial in the entries). Matrices of this type form a group as the determinant of the product of two matrices is the product of the determinants of each matrix.
If we write
for the
multiplicative group of
(that is,
excluding 0), then the determinant is a
group homomorphism
:
that is surjective and its
kernel is the special linear group. Thus,
is a
normal subgroup of
, and by the
first isomorphism theorem,
is
isomorphic to
. In fact,
can be written as a
semidirect product:
:
.
The special linear group is also the
derived group (also known as commutator subgroup) of
(for a field or a
division ring ), provided that
or
is not the
field with two elements.
[, Theorem II.9.4]
When
is
or
,
is a
Lie subgroup of
of dimension
. The
Lie algebra
In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi ident ...
of
consists of all
matrices over
with vanishing
trace. The Lie bracket is given by the
commutator.
The special linear group
can be characterized as the group of ''
volume and
orientation-preserving'' linear transformations of
.
The group
is simply connected, while
is not.
has the same fundamental group as
, that is,
for
and
for
.
Other subgroups
Diagonal subgroups
The set of all invertible
diagonal matrices forms a subgroup of
isomorphic to
. In fields like
and
, these correspond to rescaling the space; the so-called dilations and contractions.
A scalar matrix is a diagonal matrix which is a constant times the
identity matrix. The set of all nonzero scalar matrices forms a subgroup of
isomorphic to
. This group is the
center of
. In particular, it is a normal, abelian subgroup.
The center of
is simply the set of all scalar matrices with unit determinant, and is isomorphic to the group of
th
roots of unity in the field
.
Classical groups
The so-called
classical groups are subgroups of
which preserve some sort of
bilinear form on a vector space
. These include the
*
orthogonal group,
, which preserves a
non-degenerate quadratic form on
,
*
symplectic group,
, which preserves a
symplectic form on
(a non-degenerate
alternating form),
*
unitary group,
, which, when
, preserves a non-degenerate
hermitian form on
.
These groups provide important examples of Lie groups.
Related groups and monoids
Projective linear group
The
projective linear group and the
projective special linear group are the
quotients of
and
by their
centers (which consist of the multiples of the identity matrix therein); they are the induced
action on the associated
projective space.
Affine group
The
affine group is an
extension of
by the group of translations in
. It can be written as a
semidirect product:
:
where
acts on
in the natural manner. The affine group can be viewed as the group of all
affine transformations of the
affine space underlying the vector space
.
One has analogous constructions for other subgroups of the general linear group: for instance, the
special affine group is the subgroup defined by the semidirect product,
, and the
Poincaré group is the affine group associated to the
Lorentz group,
.
General semilinear group
The
general semilinear group is the group of all invertible
semilinear transformations, and contains
. A semilinear transformation is a transformation which is linear “up to a twist”, meaning “up to a
field automorphism under scalar multiplication”. It can be written as a semidirect product:
:
where
is the
Galois group of
(over its
prime field), which acts on
by the Galois action on the entries.
The main interest of
is that the associated
projective semilinear group , which contains
, is the
collineation group of
projective space, for
, and thus semilinear maps are of interest in
projective geometry.
Full linear monoid
The Full Linear Monoid, derived upon removal of the determinant's non-zero restriction, forms an algebraic structure akin to a monoid, often referred to as the full linear monoid or occasionally as the full linear semigroup or general linear monoid. Notably, it constitutes a regular semigroup.
If one removes the restriction of the determinant being non-zero, the resulting algebraic structure is a
monoid, usually called the full linear monoid,
but occasionally also ''full linear semigroup'',
''general linear monoid''
etc. It is actually a
regular semigroup.
Infinite general linear group
The infinite general linear group or
stable general linear group is the
direct limit of the inclusions
as the upper left
block matrix. It is denoted by either
or
, and can also be interpreted as invertible infinite matrices which differ from the identity matrix in only finitely many places.
It is used in
algebraic K-theory to define
K1, and over the reals has a well-understood topology, thanks to
Bott periodicity.
It should not be confused with the space of (bounded) invertible operators on a
Hilbert space, which is a larger group, and topologically much simpler, namely contractible – see
Kuiper's theorem.
See also
*
List of finite simple groups
*
SL2(R)
*
Representation theory of SL2(R)
*
Representations of classical Lie groups
Notes
References
*
External links
*{{springer, title=General linear group, id=p/g043680
"GL(2, ''p'') and GL(3, 3) Acting on Points"by
Ed Pegg, Jr.,
Wolfram Demonstrations Project, 2007.
Abstract algebra
Linear algebra
Lie groups
Linear algebraic groups