Contents

General linear group

Group of n × n invertible matrices

Algebraic structure → Group theory Group theory
Basic notions Subgroup Normal subgroup Quotient group (Semi-)direct product Group homomorphisms kernel image direct sum wreath product simple finite infinite continuous multiplicative additive cyclic abelian dihedral nilpotent solvable action Glossary of group theory List of group theory topics
Finite groups Cyclic groupZn Symmetric groupSn Alternating groupAn Dihedral groupDn Quaternion groupQ Cauchy's theorem Lagrange's theorem Sylow theorems Hall's theorem p-group Elementary abelian group Frobenius group Schur multiplier Classification of finite simple groups cyclic alternating Lie type sporadic
Discrete groups Lattices Integers (${\displaystyle \mathbb {Z} }$) Free group Modular groups PSL(2, ${\displaystyle \mathbb {Z} }$) SL(2, ${\displaystyle \mathbb {Z} }$) Arithmetic group Lattice Hyperbolic group
Topological and Lie groups Solenoid Circle General linear GL(n) Special linear SL(n) Orthogonal O(n) Euclidean E(n) Special orthogonal SO(n) Unitary U(n) Special unitary SU(n) Symplectic Sp(n) G2 F4 E6 E7 E8 Lorentz Poincaré Conformal Diffeomorphism Loop Infinite dimensional Lie group O(∞) SU(∞) Sp(∞)
Algebraic groups Linear algebraic group Reductive group Abelian variety Elliptic curve
v t e

Lie groups and Lie algebras
Classical groups General linear GL(n) Special linear SL(n) Orthogonal O(n) Special orthogonal SO(n) Unitary U(n) Special unitary SU(n) Symplectic Sp(n)
Simple Lie groups Classical An Bn Cn Dn Exceptional G2 F4 E6 E7 E8
Other Lie groups Circle Lorentz Poincaré Conformal group Diffeomorphism Loop Euclidean
Lie algebras Lie group–Lie algebra correspondence Exponential map Adjoint representation Killing form Index Simple Lie algebra Loop algebra Affine Lie algebra
Semisimple Lie algebra Dynkin diagrams Cartan subalgebra Root system Weyl group Real form Complexification Split Lie algebra Compact Lie algebra
Representation theory Lie group representation Lie algebra representation Representation theory of semisimple Lie algebras Representations of classical Lie groups Theorem of the highest weight Borel–Weil–Bott theorem
Lie groups in physics Particle physics and representation theory Lorentz group representations Poincaré group representations Galilean group representations
Scientists Sophus Lie Henri Poincaré Wilhelm Killing Élie Cartan Hermann Weyl Claude Chevalley Harish-Chandra Armand Borel
Glossary Table of Lie groups
v t e

Inmathematics, the general linear group of degree n is the set of n×n 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 R (the set of real numbers) is the group of n×n invertible matrices of real numbers, and is denoted by GL_n(R) or GL(n, R).

More generally, the general linear group of degree n over any field F (such as the complex numbers), or a ring R (such as the ring of integers), is the set of n×n invertible matrices with entries from F (orR), again with matrix multiplication as the group operation.^[1] Typical notation is GL_n(F) or GL(n, F), or simply GL(n) if the field is understood.

More generally still, the general linear group of a vector space GL(V) is the automorphism group, not necessarily written as matrices.

The special linear group, written SL(n, F) or SL_n(F), is the subgroupofGL(n, F) consisting of matrices with a determinant of 1.

The group GL(n, F) and its subgroups are often called linear groupsormatrix groups (the automorphism group GL(V) 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 SL(2, Z).

Ifn ≥ 2, then the group GL(n, F) is not abelian.

General linear group of a vector space[edit]

IfV is a vector space over the field F, the general linear group of V, written GL(V) or Aut(V), is the group of all automorphismsofV, i.e. the set of all bijective linear transformations V → V, together with functional composition as group operation. If V has finite dimension n, then GL(V) and GL(n, F) are isomorphic. The isomorphism is not canonical; it depends on a choice of basisinV. Given a basis (e₁, ..., e_n)ofV and an automorphism T in GL(V), we have then for every basis vector e_i that

${\displaystyle T(e_{i})=\sum _{j=1}^{n}a_{ji}e_{j}}$

for some constants a_ijinF; the matrix corresponding to T is then just the matrix with entries given by the a_ji.

In a similar way, for a commutative ring R the group GL(n, R) may be interpreted as the group of automorphisms of a free R-module M of rank n. One can also define GL(M) for any R-module, but in general this is not isomorphic to GL(n, R) (for any n).

In terms of determinants[edit]

Over a field F, a matrix is invertible if and only if its determinant is nonzero. Therefore, an alternative definition of GL(n, F) is as the group of matrices with nonzero determinant.

Over a commutative ring R, more care is needed: a matrix over R is invertible if and only if its determinant is a unitinR, that is, if its determinant is invertible in R. Therefore, GL(n, R) may be defined as the group of matrices whose determinants are units.

Over a non-commutative ring R, determinants are not at all well behaved. In this case, GL(n, R) may be defined as the unit group of the matrix ring M(n, R).

As a Lie group[edit]

Real case[edit]

The general linear group GL(n, R) over the field of real numbers is a real Lie group of dimension n². To see this, note that the set of all n×n real matrices, M_n(R), forms a real vector space of dimension n². The subset GL(n, R) consists of those matrices whose determinant is non-zero. The determinant is a polynomial map, and hence GL(n, R) is an open affine subvariety of M_n(R) (anon-empty open subset of M_n(R) in the Zariski topology), and therefore^[2]asmooth manifold of the same dimension.

The Lie algebraofGL(n, R), denoted ${\displaystyle {\mathfrak {gl}}_{n},}$ consists of all n×n real matrices with the commutator serving as the Lie bracket.

As a manifold, GL(n, R) 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 GL⁺(n, R), consists of the real n×n matrices with positive determinant. This is also a Lie group of dimension n²; it has the same Lie algebra as GL(n, R).

The polar decomposition, which is unique for invertible matrices, shows that there is a homeomorphism between GL(n, R) and the Cartesian product of O(n) with the set of positive-definite symmetric matrices. Similarly, it shows that there is a homeomorphism between GL⁺(n, R) and the Cartesian product of SO(n) with the set of positive-definite symmetric matrices. Because the latter is contractible, the fundamental groupofGL⁺(n, R) is isomorphic to that of SO(n).

The homeomorphism also shows that the group GL(n, R)isnoncompact. “The” ^[3] maximal compact subgroupofGL(n, R) is the orthogonal group O(n), while "the" maximal compact subgroup of GL⁺(n, R) is the special orthogonal group SO(n). As for SO(n), the group GL⁺(n, R) is not simply connected (except when n = 1), but rather has a fundamental group isomorphic to Z for n = 2orZ₂ for n >2.

Complex case[edit]

The general linear group over the field of complex numbers, GL(n, C), is a complex Lie group of complex dimension n². As a real Lie group (through realification) it has dimension 2n². The set of all real matrices forms a real Lie subgroup. These correspond to the inclusions

GL(n, R) < GL(n, C) < GL(2n, R),

which have real dimensions n², 2n², and 4n² = (2n)². Complex n-dimensional matrices can be characterized as real 2n-dimensional matrices that preserve a linear complex structure — concretely, that commute with a matrix J such that J² = −I, where J corresponds to multiplying by the imaginary unit i.

The Lie algebra corresponding to GL(n, C) consists of all n×n complex matrices with the commutator serving as the Lie bracket.

Unlike the real case, GL(n, C)isconnected. This follows, in part, since the multiplicative group of complex numbers C^∗ is connected. The group manifold GL(n, C) is not compact; rather its maximal compact subgroup is the unitary group U(n). As for U(n), the group manifold GL(n, C) is not simply connected but has a fundamental group isomorphic to Z.

Over finite fields[edit]

IfF is a finite field with q elements, then we sometimes write GL(n, q) instead of GL(n, F). When p is prime, GL(n, p) is the outer automorphism group of the group Z_pⁿ, and also the automorphism group, because Z_pⁿ is abelian, so the inner automorphism group is trivial.

The order of GL(n, q) is:

${\displaystyle \prod _{k=0}^{n-1}(q^{n}-q^{k})=(q^{n}-1)(q^{n}-q)(q^{n}-q^{2})\ \cdots \ (q^{n}-q^{n-1}).}$

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 kth column can be any vector not in the linear span of the first k − 1 columns. In q-analog notation, this is ${\displaystyle [$n]_{q}!(q-1)^{n}q^{n \choose 2}} .

For example, GL(3, 2) has order (8 − 1)(8 − 2)(8 − 4) = 168. It is the automorphism group of the Fano plane and of the group Z₂³, and is also known as PSL(2, 7).

More generally, one can count points of Grassmannian over F: in other words the number of subspaces of a given dimension k. 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 q ↦ 1 the order of GL(n, q) goes to 0! – but under the correct procedure (dividing by (q − 1)ⁿ) 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: S_n ≅ GL(n, 1).

History[edit]

The general linear group over a prime field, GL(ν, p), 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 p^ν.^[4]

Special linear group[edit]

The special linear group, SL(n, F), is the group of all matrices with determinant 1. They 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. SL(n, F) is a normal subgroupofGL(n, F).

If we write F^× for the multiplicative groupofF (excluding 0), then the determinant is a group homomorphism

det: GL(n, F) → F^×.

that is surjective and its kernel is the special linear group. Therefore, by the first isomorphism theorem, GL(n, F)/SL(n, F)isisomorphictoF^×. In fact, GL(n, F) can be written as a semidirect product:

GL(n, F) = SL(n, F) ⋊ F^×

The special linear group is also the derived group (also known as commutator subgroup) of the GL(n, F) (for a field or a division ring F) provided that ${\displaystyle n\neq 2}$ork is not the field with two elements.^[5]

When FisRorC, SL(n, F) is a Lie subgroupofGL(n, F) of dimension n² − 1. The Lie algebraofSL(n, F) consists of all n×n matrices over F with vanishing trace. The Lie bracket is given by the commutator.

The special linear group SL(n, R) can be characterized as the group of volume and orientation-preserving linear transformations of Rⁿ.

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

Other subgroups[edit]

Diagonal subgroups[edit]

The set of all invertible diagonal matrices forms a subgroup of GL(n, F) isomorphic to (F^×)ⁿ. In fields like R and C, these correspond to rescaling the space; the so-called dilations and contractions.

Ascalar matrix is a diagonal matrix which is a constant times the identity matrix. The set of all nonzero scalar matrices forms a subgroup of GL(n, F) isomorphic to F^×. This group is the centerofGL(n, F). In particular, it is a normal, abelian subgroup.

The center of SL(n, F) is simply the set of all scalar matrices with unit determinant, and is isomorphic to the group of nthroots of unity in the field F.

Classical groups[edit]

The so-called classical groups are subgroups of GL(V) which preserve some sort of bilinear form on a vector space V. These include the

• orthogonal group, O(V), which preserves a non-degenerate quadratic formonV,
• symplectic group, Sp(V), which preserves a symplectic formonV (a non-degenerate alternating form),
• unitary group, U(V), which, when F = C, preserves a non-degenerate hermitian formonV.

These groups provide important examples of Lie groups.

Related groups and monoids[edit]

Projective linear group[edit]

The projective linear group PGL(n, F) and the projective special linear group PSL(n, F) are the quotientsofGL(n, F) and SL(n, F) 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[edit]

The affine group Aff(n, F) is an extensionofGL(n, F) by the group of translations in Fⁿ. It can be written as a semidirect product:

Aff(n, F) = GL(n, F) ⋉ Fⁿ

where GL(n, F) acts on Fⁿ 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 Fⁿ.

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, SL(n, F) ⋉ Fⁿ, and the Poincaré group is the affine group associated to the Lorentz group, O(1, 3, F) ⋉ Fⁿ.

General semilinear group[edit]

The general semilinear group ΓL(n, F) is the group of all invertible semilinear transformations, and contains GL. 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:

ΓL(n, F) = Gal(F) ⋉ GL(n, F)

where Gal(F) is the Galois groupofF (over its prime field), which acts on GL(n, F) by the Galois action on the entries.

The main interest of ΓL(n, F) is that the associated projective semilinear group PΓL(n, F) (which contains PGL(n, F)) is the collineation groupofprojective space, for n >2, and thus semilinear maps are of interest in projective geometry.

Full linear monoid[edit]

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.

This section needs expansion with: basic properties. You can help by adding to it. (April 2015)

If one removes the restriction of the determinant being non-zero, the resulting algebraic structure is a monoid, usually called the full linear monoid,^[6][7][8] but occasionally also full linear semigroup,^[9] general linear monoid^[10][11] etc. It is actually a regular semigroup.^[7]

Infinite general linear group[edit]

The infinite general linear grouporstable general linear group is the direct limit of the inclusions GL(n, F) → GL(n + 1, F) as the upper left block matrix. It is denoted by either GL(F) or GL(∞, F), and can also be interpreted as invertible infinite matrices which differ from the identity matrix in only finitely many places.^[12]

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[edit]

• List of finite simple groups
• SL₂(R)
• Representation theory of SL₂(R)
• Representations of classical Lie groups

Notes[edit]

References[edit]

External links[edit]

• "General linear group", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
• "GL(2, p) and GL(3, 3) Acting on Points"byEd Pegg, Jr., Wolfram Demonstrations Project, 2007.