Definition

Let GG be a group and let θ\theta be an of GG. Two elements x,yGx,y\in G are θ\theta-conjugate if

y=gxθ(g)1y=gx\theta(g)^{-1}

for some gGg\in G. Equivalently, they lie in the same for the twisted action gθx=gxθ(g)1g\mathbin{\cdot_\theta}x=gx\theta(g)^{-1}. When θ\theta is the identity this is ordinary conjugacy.

The twisted centralizer of xx is the Gx,θ={g:gxθ(g)1=x}G_{x,\theta}=\{g:gx\theta(g)^{-1}=x\}.

Frobenius and sigma-conjugacy

If GG is defined over a or and σ\sigma is , then twisted conjugacy is usually called σ\sigma-conjugacy. The is the set of σ\sigma-conjugacy classes in G(F˘)G(\breve F).

Twisted conjugacy also appears in the nonidentity components of such as G^θ\widehat G\rtimes\langle\theta\rangle: ordinary conjugacy within the coset of the G^θ\widehat G\theta becomes θ\theta-conjugacy in G^\widehat G.

Stable variant

For one can likewise compare twisted conjugacy over the base field with twisted conjugacy over an . The latter gives stable twisted classes, whose rational orbits are controlled by Galois of the twisted centralizer.

References
  1. Robert E. Kottwitz, “Isocrystals with additional structure,” Compositio Mathematica 56 (1985), 201–220. Numdam.
  2. Robert E. Kottwitz, “Stable trace formula: cuspidal tempered terms,” Duke Mathematical Journal 51 (1984), 611–650.