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DefinitionDefinition: Literature-sourcedProof: Not applicablePipeline-generatedaudited 2026-09-22
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Roots of a compact connected Lie group

Definition

Assume the Axiom of Choice (The Axiom of Choice). Let G be a compact connected Lie group with maximal torus T, and put g=LieG, t=LieT. Complexification is over R.

Circle convention. The lattice definition Character and cocharacter lattices uses R/Z. Here its character values are transported to the multiplicative complex circle U={zC:z=1} by E:R/ZU,[r]e2πir. The exponential addition law makes E a homomorphism (exp(z+w)=expzexpw, and the complex exponential extends the real exponential), and its kernel is trivial by ker(exp)=2πiZ, and expz=expw exactly when zw2πiZ. The modulus formula exp(x+iy)=ex(cosy+isiny), exp(x+iy)=ex, and eiπ+1=0 and surjectivity of the complex exponential The complex exponential maps C onto C{0} show that its image is all of U: a logarithm of a unit-modulus number has real part zero. Thus E is a continuous bijection from a compact circle to a Hausdorff circle, with continuous inverse. It identifies addition in R/Z with multiplication in U. All scalar character values below use this identification; they are not elements of the additive group C.

The smooth adjoint representation of G (Adjoint is a smooth Lie-group representation) extends complex-linearly to gC. A root of (G,T) is a nontrivial continuous character α:TU whose weight space gα={vgC:Ad(t)v=α(t)v for every tT} is nonzero. This is a character in X(T) via E1. Write Φ(G,T) for the set of roots. The trivial character is denoted 1, and its weight space is denoted g0 to agree with additive weight notation: g0={v:Ad(t)v=v for every tT}. The trivial character is not a root.

There is a finite direct sum decomposition gC=g0αΦ(G,T)gα. Indeed, unitarizability under AC (Finite-dimensional compact-group representations are unitarizable) makes the commuting operators Ad(t) normal. The complex spectral theorem and simultaneous diagonalization (Complex spectral theorem: a normal endomorphism of a finite-dimensional complex inner product space has an orthonormal eigenbasis, and conversely, A family of diagonalisable endomorphisms of a finite-dimensional space is simultaneously diagonalisable if and only if its members commute pairwise) give a common eigenbasis. For a nonzero common eigenvector v, its eigenvalue function is α(t)=Ad(t)v,v/v,v, with inner product linear in the first argument, so is continuous. The representation law makes it multiplicative and unitarity gives α(t)=1. Only finitely many joint eigenvalue functions occur. Separating the trivial one gives exactly the displayed sum.

Differential convention. Continuous Lie-group homomorphisms are smooth under countable choice (Continuous homomorphisms between Lie groups are smooth), which follows from the assumed AC. For Ht define dα(H)=ddss=0α(expG(sH))iR, and extend this real-linear differential complex-linearly to tC. The displayed derivative is taken only for real Ht; no exponential in the real group is applied to a general complex tangent vector. If a=E1α is the additive circle-valued character and dae:tR, then dα=2πidae on t. We often also denote dα by α, explicitly switching from the group character to its differential.

Differentiating the weight equation and using The differential of Ad is ad gives [H,v]=dα(H)v, first for real H, then by complex linearity for HtC. Restricted to the real form tR=it, this functional is real-valued since dα(iH)=idα(H). It is nonzero for a root: naturality of the exponential (Exponential map is natural for Lie-group homomorphisms) shows that a character with zero differential is trivial on an exponential identity neighborhood, using The exponential map is a local diffeomorphism at zero. Its kernel is then an open subgroup of connected T, hence all of T. Applying this to the quotient of two characters also shows that their differentials determine them uniquely. No global torus lattice classification is needed here.

Remarks

  • The zero weight space is the centralizer of tC: one direction follows by differentiation; in the other direction Adjoint exponential identity makes all expG(H), Ht, act trivially on the vector, and these generate T by local invertibility and connectedness. Every root character is trivial on TZ(G), since conjugation by such an element is the identity, and its differential vanishes on tz(g) by the bracket formula.
  • If G is a torus, its adjoint action is trivial and Φ(G,T) is empty. A trivial maximal torus also has no nontrivial characters, so the root set is empty. These cases do not introduce a zero root.
  • For T=gTg1, the map Adg sends gα to the weight space for αCg1T, by the representation law. Conjugacy of maximal tori (Conjugacy of maximal tori) therefore identifies these root sets and weight spaces for different maximal tori.

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