Compact Lie groups are a special class of Lie groups with unique properties. They have finite measures, discrete centers, and compact derived subgroups. Examples include , , , and .
Representations of compact Lie groups are continuous homomorphisms to linear groups. They're finite-dimensional and can be decomposed into irreducible parts. The provides a powerful tool for understanding these representations and their characters.
Compact Lie groups
Definition and properties
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A is a Lie group that is compact as a topological space
Means it is closed and bounded in the topology induced by any Riemannian metric on the group
Compact Lie groups have a unique
This measure is finite and allows integration over the group
Compact Lie groups have a and a
The derived subgroup of a compact Lie group is always closed
Examples
The circle group U(1) is a compact Lie group
The special unitary group SU(n) is a compact Lie group
The special orthogonal group SO(n) for n≥3 is a compact Lie group
The quaternionic unitary group Sp(n) is a compact Lie group
Every compact Lie group has a faithful
This means it can be viewed as a subgroup of GL(n,C) for some n
Representations of compact Lie groups
Definition and properties
A representation of a compact Lie group G is a ρ:G→GL(V), where V is a finite-dimensional vector space over C
Irreducible representations of a compact Lie group are finite-dimensional
Every representation can be decomposed into a direct sum of irreducible representations
The of a representation ρ:G→GL(V) is the function χρ:G→C defined by χρ(g)=tr(ρ(g))
Characters are constant on conjugacy classes and determine the representation up to isomorphism
The of a compact Lie group G on L2(G) decomposes into a direct sum of all irreducible representations, each occurring with equal to its dimension
Construction using the exponential map
Representations can be constructed using the
For a compact Lie group G with Lie algebra g, the exponential map exp:g→G is surjective
This allows representations of G to be constructed from representations of g
Example: The of SU(2) can be constructed using the exponential map and the Pauli matrices as a basis for the Lie algebra su(2)
Peter-Weyl theorem for decomposition
Statement and consequences
The Peter-Weyl theorem states that the matrix coefficients of irreducible representations of a compact Lie group G form an for L2(G)
As a consequence, any representation of G can be decomposed into a direct sum of irreducible representations
The Peter-Weyl theorem implies that any continuous function on G can be uniformly approximated by linear combinations of matrix coefficients of irreducible representations
This is analogous to the Fourier series expansion of periodic functions
Multiplicity and character inner product
The multiplicity of an in a given representation can be computed using the inner product of characters
If ρ is a representation with character χρ and τ is an irreducible representation with character χτ, then the multiplicity of τ in ρ is given by the inner product ⟨χρ,χτ⟩=∫Gχρ(g)χτ(g)∗dg, where dg is the Haar measure
Example: The multiplicity of the trivial representation in the regular representation of a compact Lie group is equal to 1, since the character of the trivial representation is the constant function 1
Representations vs maximal tori
Maximal tori and the Weyl group
A torus in a Lie group G is a connected abelian subgroup
A is a torus that is not properly contained in any other torus
All maximal tori in a compact Lie group are conjugate
Their dimension is called the rank of the group
The W(G,T)=NG(T)/T acts on the of a representation
The character of a representation is determined by its weights and their multiplicities
Weight space decomposition
Representations of a compact Lie group G restrict to representations of a maximal torus T
These restricted representations decompose into one-dimensional representations, or characters, of T
The weights of a representation ρ:G→GL(V) are the characters of T that appear in the restriction of ρ to T
The multiplicity of a weight is the dimension of the corresponding T-eigenspace in V
Example: The fundamental representation of SU(2) decomposes into two one-dimensional weight spaces with weights ±1 when restricted to the maximal torus T={diag(eiθ,e−iθ):θ∈R}
Weyl character formula
The expresses the character of an irreducible representation in terms of its highest weight and the action of the Weyl group
It provides a way to compute characters without explicitly constructing the representation
Example: For the fundamental representation of SU(2) with highest weight λ=1, the Weyl character formula gives χλ(eiθ)=eiθ+e−iθ=2cos(θ)