Let GG be a connected with split TT. The adjoint action of TT on gives

Lie⁡(G)=Lie⁡(T)⊕⨁α∈Φgα.\operatorname{Lie}(G) = \operatorname{Lie}(T) \oplus \bigoplus_{\alpha\in\Phi}\mathfrak g_\alpha.

The nonzero characters α∈X∗(T)\alpha\in X^*(T) occurring here are the roots.

Weyl group and positive roots

The Weyl group is

W=NG(T)/TW=N_G(T)/T

where NG(T)N_G(T) is the . The group WW acts on X∗(T)X^*(T) and is generated by the root reflections. Choosing a B⊃TB\supset T selects Φ+\Phi^+ and simple roots Δ\Delta.

A character λ∈X∗(T)\lambda\in X^*(T) is dominant when

⟨λ,α∨⟩≥0\langle\lambda,\alpha^\vee\rangle\geq0

for every α∈Δ\alpha\in\Delta, using the .

Highest weights

Over an of characteristic 00, irreducible finite-dimensional algebraic representations of GG are classified by dominant characters in X∗(T)X^*(T). The abstract of the root system can be larger than X∗(T)X^*(T); only the characters allowed by the occur as representations of GG.

For GL⁡n\operatorname{GL}_n, the roots are ei−eje_i-e_j, the is SnS_n, and the standard Borel gives dominant weights λ1≥⋯≥λn\lambda_1\geq\cdots\geq\lambda_n.

Langlands role

exchanges roots and coroots. of GG become dominant weights of G^\widehat G, indexing both the Satake basis and the Schubert strata used in .

References
  1. J. E. Humphreys, Introduction to Lie Algebras and Representation Theory, Springer, 1972.
  2. A. Borel, Linear Algebraic Groups, second edition, Springer, 1991.