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Compact Lie Groups - Key Properties

Compact Lie groups possess remarkable properties that distinguish them from general Lie groups. These properties make compact groups particularly amenable to analysis and central to representation theory.

Theorem

Complete Reducibility (Peter-Weyl Theorem)

Every continuous finite-dimensional representation of a compact Lie group GG is completely reducible: it decomposes as a direct sum of irreducible representations. Moreover, the matrix coefficients of irreducibles are dense in L2(G)L^2(G).

This is the fundamental result making representation theory of compact groups tractable. Unlike general Lie groups, there are no indecomposable non-irreducible representations.

Theorem

Weyl's Unitary Trick

Every representation ρ:GGL(V)\rho: G \to GL(V) of a compact Lie group admits a GG-invariant inner product on VV, making ρ(G)\rho(G) consist of unitary operators. This allows using tools from functional analysis.

The proof uses averaging over the group with Haar measure: define v,wG=Gρ(g)v,ρ(g)w0dμ(g)\langle v, w\rangle_G = \int_G \langle \rho(g)v, \rho(g)w\rangle_0 \, d\mu(g) for any initial inner product ,0\langle\cdot, \cdot\rangle_0.

Remark

Weyl's integraldimension formula: For irreducible representation VλV_\lambda of compact semisimple GG with highest weight λ\lambda: dimVλ=αΦ+λ+ρ,αρ,α\dim V_\lambda = \prod_{\alpha \in \Phi^+} \frac{\langle \lambda + \rho, \alpha\rangle}{\langle \rho, \alpha\rangle} where Φ+\Phi^+ are positive roots and ρ\rho is half-sum of positive roots. This gives explicit dimensions.

Theorem

Maximal Torus Theorem

For compact connected GG:

  1. All maximal tori are conjugate
  2. Every element of GG is conjugate to an element of any fixed maximal torus TT
  3. G=gGgTg1G = \bigcup_{g \in G} gTg^{-1} (every element lies in some maximal torus)

This reduces questions about GG to questions about the torus TT and the Weyl group W=NG(T)/TW = N_G(T)/T.

Example

For SU(n)SU(n), the maximal torus consists of diagonal unitary matrices diag(eiθ1,,eiθn)\text{diag}(e^{i\theta_1}, \ldots, e^{i\theta_n}) with θi=0(mod2π)\sum \theta_i = 0 \pmod{2\pi}. This has dimension n1n-1, the rank of SU(n)SU(n).

Integration formulas: The Weyl integration formula expresses integrals over GG as integrals over the maximal torus: Gf(g)dg=1WTf(t)Δ(t)2dt\int_G f(g) \, dg = \frac{1}{|W|} \int_T f(t) |\Delta(t)|^2 \, dt where Δ(t)=α>0(eiα(t)/2eiα(t)/2)\Delta(t) = \prod_{\alpha > 0}(e^{i\alpha(t)/2} - e^{-i\alpha(t)/2}) is the Weyl denominator.

Theorem

Compact Form Correspondence

Every complex simple Lie algebra gC\mathfrak{g}_\mathbb{C} has a unique (up to isomorphism) compact real form gu\mathfrak{g}_u: a real Lie algebra whose complexification is gC\mathfrak{g}_\mathbb{C} and which is the Lie algebra of a compact Lie group.

For example, su(n)\mathfrak{su}(n) is the compact form of sln(C)\mathfrak{sl}_n(\mathbb{C}). This correspondence allows transferring results between compact groups and complex algebras.

Remark

The Cartan decomposition states that for non-compact semisimple GG, there exists a maximal compact subgroup KK such that G/KG/K is diffeomorphic to Euclidean space. This reduces topology questions to the compact case.

These properties make compact Lie groups the most thoroughly understood class of Lie groups, serving as anchors for understanding general Lie theory.