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Roots of a compact connected Lie group
Definition
Assume the Axiom of Choice (The Axiom of Choice). Let be a compact connected Lie group with maximal torus , and put , . Complexification is over .
Circle convention. The lattice definition Character and cocharacter lattices uses . Here its character values are transported to the multiplicative complex circle by The exponential addition law makes a homomorphism (, and the complex exponential extends the real exponential), and its kernel is trivial by , and exactly when . The modulus formula , , and and surjectivity of the complex exponential The complex exponential maps onto show that its image is all of : a logarithm of a unit-modulus number has real part zero. Thus is a continuous bijection from a compact circle to a Hausdorff circle, with continuous inverse. It identifies addition in with multiplication in . All scalar character values below use this identification; they are not elements of the additive group .
The smooth adjoint representation of (Adjoint is a smooth Lie-group representation) extends complex-linearly to . A root of is a nontrivial continuous character whose weight space is nonzero. This is a character in via . Write for the set of roots. The trivial character is denoted , and its weight space is denoted to agree with additive weight notation: The trivial character is not a root.
There is a finite direct sum decomposition Indeed, unitarizability under AC (Finite-dimensional compact-group representations are unitarizable) makes the commuting operators 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 , its eigenvalue function is , with inner product linear in the first argument, so is continuous. The representation law makes it multiplicative and unitarity gives . 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 define and extend this real-linear differential complex-linearly to . The displayed derivative is taken only for real ; no exponential in the real group is applied to a general complex tangent vector. If is the additive circle-valued character and , then on . We often also denote by , explicitly switching from the group character to its differential.
Differentiating the weight equation and using The differential of Ad is ad gives , first for real , then by complex linearity for . Restricted to the real form , this functional is real-valued since . 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 , hence all of . 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 : one direction follows by differentiation; in the other direction Adjoint exponential identity makes all , , act trivially on the vector, and these generate by local invertibility and connectedness. Every root character is trivial on , since conjugation by such an element is the identity, and its differential vanishes on by the bracket formula.
- If is a torus, its adjoint action is trivial and 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 , the map sends to the weight space for , by the representation law. Conjugacy of maximal tori (Conjugacy of maximal tori) therefore identifies these root sets and weight spaces for different maximal tori.
Depends on
- The Axiom of Choice
- Character and cocharacter lattices
- $\exp(z+w)=\exp z\,\exp w$, and the complex exponential extends the real exponential
- $\ker(\exp)=2\pi i\mathbb Z$, and $\exp z=\exp w$ exactly when $z-w\in2\pi i\mathbb Z$
- $\exp(x+iy)=e^x(\cos y+i\sin y)$, $|\exp(x+iy)|=e^x$, and $e^{i\pi}+1=0$
- The complex exponential maps $\mathbb C$ onto $\mathbb C\setminus\{0\}$
- Adjoint is a smooth Lie-group representation
- Finite-dimensional compact-group representations are unitarizable
- 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
- Continuous homomorphisms between Lie groups are smooth
- The differential of Ad is ad
- Exponential map is natural for Lie-group homomorphisms
- The exponential map is a local diffeomorphism at zero
- Adjoint exponential identity
- Conjugacy of maximal tori
Used by
- Root datum of a compact connected Lie group Definition
- Weyl Jacobian Definition
- Central quotients and intermediate character lattices Proposition
- Root and weight lattice sandwich Proposition
- The Weyl Jacobian is independent and invariant Proposition
- Analytic and root-system Weyl groups agree Theorem
- Compact connected Lie groups are classified by root data Theorem
- Compact roots form a reduced crystallographic root system Theorem
- Weyl integration formula Theorem
Dependency tree · two levels
85 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Anthony W. Knapp, Lie Groups Beyond an Introduction, 2nd ed. (standard reference, not scraped)
- Brian Conrad and Aaron Landesman, Compact Lie Groups (standard reference, not scraped)