Oz's crib sheet: Lie theory
Edited by Toby Bartels
A Lie group G has a lie algebra g.
If a is an element of g
and A is defined to be exp a,
then A is an element of G.
- R means the real numbers.
- C means the complex numbers.
- H means the quaternions.
- G & g mean "general", which doesn't mean anything.
- L & l mean "linear"
-- which is obvious, because they're matrices!
- S means "special", det A = 1,
so s must mean tr a = 0 (traceless).
- O means "orthogonal",
At = A-1,
so o must mean at = -a (antisymmetric).
- U means "unitary", A* = A-1,
so u must mean a* = -a (antiHermitian).
- Sp means "symplectic",
which is the same as unitary only for quaternions.
Therefore:
- GL(n,R) is
the Lie group of invertible real matrices of dimension n,
and gl(n,R) is
its Lie algebra of all real matrices of dimension n.
- GL(n,C) is
the Lie group of invertible complex matrices of dimension n,
and gl(n,C) is
its Lie algebra of all complex matrices of dimension n.
- GL(n,H) is
the Lie group of invertible quaternionic matrices of dimension n,
and gl(n,H) is
its Lie algebra of all quaternionic matrices of dimension n.
- SL(n,R) is
the Lie group of special real matrices of dimension n,
and sl(n,R) is
its Lie algebra of traceless real matrices of dimension n.
- SL(n,C) is
the Lie group of special complex matrices of dimension n,
and sl(n,C) is
its Lie algebra of traceless complex matrices of dimension n.
- O(n) is
the Lie group of real orthogonal matrices of dimension n,
and o(n) is
its Lie algebra of real antisymmetric matrices of dimension n.
- SO(n) is
the Lie group of special real orthogonal matrices of dimension n,
and so(n) is
its Lie algebra of
traceless real antisymmetric matrices of dimension n.
- U(n) is
the Lie group of complex unitary matrices of dimension n,
and u(n) is
its Lie algebra of complex antiHermitian matrices of dimension n.
- SU(n) is
the Lie group of special complex unitary matrices of dimension n,
and su(n) is
its Lie algebra of
traceless complex antiHermitian matrices of dimension n.
- Sp(n) is
the Lie group of quaternionic unitary matrices of dimension n,
and sp(n) is
its Lie algebra of
quaternionic antiHermitian matrices of dimension n.
Examples:
- U(1) is the complex numbers of unit magnitude,
and u(1) is the purely imaginary complex numbers.
Topologically, U(1) is a circle, and u(1) is a line.
- SU(2) is the quaternions of unit magnitude,
and su(2) is the purely imaginary quaternions.
Topologically, SU(2) is a 3D sphere, and su(2) is 3space.
A Lie bracket [,] is defined on the lie algebra g
and produces another element of the set g.
For matrices, this is
[a,b] = ab-ba.
Same examples:
- The Lie bracket on u(1) is trivial;
[a,b] = 0 always.
- The Lie bracket on su(2) is just the vector cross product.
Complete definitions:
- A Lie group must have a notion of multiplication
and must be a smooth manifold.
- If A and B are in G,
then AB is in G.
- Multiplication is associative:
(AB)C = A(BC).
- Multiplication has an identity: 1A = A = A1.
- Multiplication has an inverse:
AA-1 = 1 =
A-1A.
- The multiplication and inverse operations must be smooth.
- A Lie algebra must have notions of
addition, scalar multiplication, and a Lie bracket.
- If a and b are in g,
then a + b is in g.
- Addition is associative:
(a + b) + c = a + (b + c).
- Addition has an identity: a + 0 = a = 0 + a.
- Addition has an inverse:
a + -a = 0 = -a + a.
- Addition is commutative:
a + b = b + a.
- If a is in g and k is a real number,
then ka is in g.
- Scalar multiplication is associative:
(kl)a = k(la).
- Scalar multiplication has an identity: 1a = a.
- Scalar multiplication is linear on the left:
(k + l)a = ka + la.
- Scalar multiplication is linear on the right:
k(a + b) =
ka + kb.
- If a is in g and b is in g,
then [a,b] is in g.
- The Lie bracket is linear on the left:
[a+b,c] = [a,c] + [b,c].
- The Lie bracket is linear on the right:
[a,b+c] = [a,b] + [a,c].
- The Lie bracket is alternating: [a,a] = 0.
- The Lie bracket is antisymmetric:
[a,b] = -[b,a].
- The Lie bracket satisfies the Jacobi identity on the left:
[[a,b],c] + [[b,c],a] +
[[c,a],b] = 0.
- The Lie bracket satisfies the Jacobi identity on the right:
[a,[b,c]] + [b,[c,a]] +
[c,[a,b]] = 0.
- The Lie bracket satisfies the Leibniz law on the left:
[a,[b,c]] = [[a,b],c] +
[b,[a,c]].
- The Lie bracket satisfies the Leibniz law on the right:
[[a,b],c] = [[a,c],b] +
[a,[b,c]].
- (Some of the requirements for the Lie bracket
are redundant.)
- Q
- Given a Lie group G, which specific Lie algebra g
is the Lie algebra of the Lie group G?
- A
- The space tangent to the identity element 1 of G.
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Toby reserves no legal rights to it.
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