Let HH be a connected complex . If h,hHh,h'\in H are , then

hHhtr(ρ(h))=tr(ρ(h))h\sim_H h' \quad\Longleftrightarrow\quad \operatorname{tr}(\rho(h)) = \operatorname{tr}(\rho(h'))

for every finite-dimensional algebraic representation ρ\rho of HH. It suffices to range over .

Invariant-theory explanation

Choose a TT with WW. Semisimple conjugacy classes are identified with WW-orbits in TT, and restriction gives

O(H)HO(T)W.\mathcal O(H)^H\simeq\mathcal O(T)^W.

The characters of irreducible algebraic representations span the and generate enough Weyl-invariant regular functions to distinguish the closed, hence semisimple, .

Closed-orbit qualification

Invariant regular functions separate closed orbits in the affine quotient. For a general element they recover the semisimple part of its Jordan , not its full conjugacy class. This is why reconstruction naturally produces semisimple parameters.

Disconnected and twisted scope

A fiber in an is a coset of the G^\widehat G, not a connected group. Its conjugacy is by the action. The analogous separation statement uses invariant functions on the twisted quotient; the connected theorem should not be applied to that coset without this modification.

Relation to the letter

Values of all dual-group characters on the Satake class determine that semisimple class. This is the invariant-theoretic reason that the collection of unramified Euler factors can record a .

References
  1. T. A. Springer, Linear Algebraic Groups, second edition, Birkhäuser, 1998.
  2. Claudio Procesi, Lie Groups: An Approach through Invariants and Representations, Springer, 2007.