Table of Lie groups explained

This article gives a table of some common Lie groups and their associated Lie algebras.

The following are noted: the topological properties of the group (dimension; connectedness; compactness; the nature of the fundamental group; and whether or not they are simply connected) as well as on their algebraic properties (abelian; simple; semisimple).

For more examples of Lie groups and other related topics see the list of simple Lie groups; the Bianchi classification of groups of up to three dimensions; see classification of low-dimensional real Lie algebras for up to four dimensions; and the list of Lie group topics.

Real Lie groups and their algebras

Column legend

\pi0

: Gives the group of components of G. The order of the component group gives the number of connected components. The group is connected if and only if the component group is trivial (denoted by 0).

\pi1

: Gives the fundamental group of G whenever G is connected. The group is simply connected if and only if the fundamental group is trivial (denoted by 0).
Lie groupDescriptionCpt

\pi0

\pi1

UCRemarksLie algebradim/R
align=center RnEuclidean space with additionN00abelianalign=center Rnalign=center n
align=center R×nonzero real numbers with multiplicationNZ2 - abelianalign=center Ralign=center 1
align=center R+positive real numbers with multiplicationN00abelianalign=center Ralign=center 1
align=center S1 = U(1)the circle group: complex numbers of absolute value 1 with multiplication;Y0ZRabelian, isomorphic to SO(2), Spin(2), and R/Zalign=center Ralign=center 1
align=center Aff(1)invertible affine transformations from R to R.NZ2 - solvable, semidirect product of R+ and R×align=center

\left\{\left[\begin{smallmatrix}a&b\ 0&1\end{smallmatrix}\right]:a\in\R*,b\inR\right\}

align=center 2
align=center H×non-zero quaternions with multiplicationN00align=center Halign=center 4
align=center S3 = Sp(1)quaternions of absolute value 1 with multiplication; topologically a 3-sphereY00isomorphic to SU(2) and to Spin(3); double cover of SO(3)align=center Im(H)align=center 3
align=center GL(n,R)general linear group

invertible n×n real matrices

NZ2 - align=center M(n,R)align=center n2
align=center GL+(n,R)n×n real matrices with positive determinantN0Z  n=2
Z2 n>2
GL+(1,R) is isomorphic to R+ and is simply connectedalign=center M(n,R)align=center n2
align=center SL(n,R)special linear group

real matrices with determinant 1

N0Z  n=2
Z2 n>2
SL(1,R) is a single point and therefore compact and simply connectedalign=center sl(n,R)align=center n2-1
align=center SL(2,R)Orientation-preserving isometries of the Poincaré half-plane, isomorphic to SU(1,1), isomorphic to Sp(2,R).N0ZThe universal cover has no finite-dimensional faithful representations.align=center sl(2,R)align=center 3
align=center O(n)orthogonal group

real orthogonal matrices

YZ2 - The symmetry group of the sphere (n=3) or hypersphere.align=center so(n)align=center n(n-1)/2
align=center SO(n)special orthogonal group

real orthogonal matrices with determinant 1

Y0Z  n=2
Z2 n>2
Spin(n)
n>2
SO(1) is a single point and SO(2) is isomorphic to the circle group, SO(3) is the rotation group of the sphere.align=center so(n)align=center n(n-1)/2
align=center SE(n)special euclidean group: group of rigid body motions in n-dimensional space.N0align=center se(n)align=center n + n(n-1)/2
align=center Spin(n)spin group

double cover of SO(n)

Yn>1n>2Spin(1) is isomorphic to Z2 and not connected; Spin(2) is isomorphic to the circle group and not simply connectedalign=center so(n)align=center n(n-1)/2
align=center Sp(2n,R)symplectic group

real symplectic matrices

N0Zalign=center sp(2n,R)align=center n(2n+1)
align=center Sp(n)compact symplectic group

quaternionic n×n unitary matrices

Y00align=center sp(n)align=center n(2n+1)
align=center Mp(2n,R)metaplectic group

double cover of real symplectic group Sp(2n,R)

Y0ZMp(2,R) is a Lie group that is not algebraicalign=center sp(2n,R)align=center n(2n+1)
align=center U(n)unitary group

complex n×n unitary matrices

Y0ZR×SU(n)For n=1: isomorphic to S1. Note: this is not a complex Lie group/algebraalign=center u(n)align=center n2
align=center SU(n)special unitary group

complex n×n unitary matrices with determinant 1

Y00Note: this is not a complex Lie group/algebraalign=center su(n)align=center n2-1

Real Lie algebras

See main article: Classification of low-dimensional real Lie algebras.

Lie algebraDescriptionSimple?Semi-simple?Remarksdim/R
align=center Rthe real numbers, the Lie bracket is zeroalign=center 1
align=center Rnthe Lie bracket is zeroalign=center n
align=center R3the Lie bracket is the cross productYesYesalign=center 3
align=center Hquaternions, with Lie bracket the commutatoralign=center 4
align=center Im(H)quaternions with zero real part, with Lie bracket the commutator; isomorphic to real 3-vectors,with Lie bracket the cross product; also isomorphic to su(2) and to so(3,R)YesYesalign=center 3
align=center M(n,R)n×n matrices, with Lie bracket the commutatoralign=center n2
align=center sl(n,R)square matrices with trace 0, with Lie bracket the commutatorYesYesalign=center n2-1
align=center so(n)skew-symmetric square real matrices, with Lie bracket the commutator.Yes, except n=4YesException: so(4) is semi-simple,but not simple.align=center n(n-1)/2
align=center sp(2n,R)real matrices that satisfy JA + ATJ = 0 where J is the standard skew-symmetric matrixYesYesalign=center n(2n+1)
align=center sp(n)square quaternionic matrices A satisfying A = -A, with Lie bracket the commutatorYesYesalign=center n(2n+1)
align=center u(n)square complex matrices A satisfying A = -A, with Lie bracket the commutatorNote: this is not a complex Lie algebraalign=center n2
align=center su(n)
n≥2
square complex matrices A with trace 0 satisfying A = -A, with Lie bracket the commutatorYesYesNote: this is not a complex Lie algebraalign=center n2-1

Complex Lie groups and their algebras

See main article: Complex Lie group. Note that a "complex Lie group" is defined as a complex analytic manifold that is also a group whose multiplication and inversion are each given by a holomorphic map. The dimensions in the table below are dimensions over C. Note that every complex Lie group/algebra can also be viewed as a real Lie group/algebra of twice the dimension.

Lie groupDescriptionCpt

\pi0

\pi1

UCRemarksLie algebradim/C
Cngroup operation is additionN00abelianCnn
C×nonzero complex numbers with multiplicationN0ZabelianC1
GL(n,C)general linear group

invertible n×n complex matrices

N0 ZFor n=1: isomorphic to C×M(n,C)n2
SL(n,C) special linear group

complex matrices with determinant1

N00for n=1 this is a single point and thus compact.sl(n,C)n2-1
SL(2,C)Special case of SL(n,C) for n=2N00Isomorphic to Spin(3,C), isomorphic to Sp(2,C)sl(2,C)3
PSL(2,C)Projective special linear groupN0Z2SL(2,C)Isomorphic to the Möbius group, isomorphic to the restricted Lorentz group SO+(3,1,R), isomorphic to SO(3,C). sl(2,C)3
O(n,C)orthogonal group

complex orthogonal matrices

NZ2 - finite for n=1so(n,C)n(n-1)/2
SO(n,C)special orthogonal group

complex orthogonal matrices with determinant 1

N0Z  n=2
Z2 n>2
SO(2,C) is abelian and isomorphic to C×; nonabelian for n>2. SO(1,C) is a single point and thus compact and simply connectedso(n,C)n(n-1)/2
Sp(2n,C)symplectic group

complex symplectic matrices

N00sp(2n,C)n(2n+1)

Complex Lie algebras

See main article: Complex Lie algebra. The dimensions given are dimensions over C. Note that every complex Lie algebra can also be viewed as a real Lie algebra of twice the dimension.

Lie algebraDescriptionSimple?Semi-simple?Remarksdim/C
Cthe complex numbers1
Cnthe Lie bracket is zeron
M(n,C)n×n matrices with Lie bracket the commutatorn2
sl(n,C)square matrices with trace 0 with Lie bracketthe commutatorYesYesn2-1
sl(2,C)Special case of sl(n,C) with n=2YesYesisomorphic to su(2)

C
3
so(n,C)skew-symmetric square complex matrices with Lie bracketthe commutatorYes, except n=4YesException: so(4,C) is semi-simple,but not simple.n(n-1)/2
sp(2n,C)complex matrices that satisfy JA + ATJ = 0where J is the standard skew-symmetric matrixYesYesn(2n+1)

The Lie algebra of affine transformations of dimension two, in fact, exist for any field. An instance has already been listed in the first table for real Lie algebras.

See also