Let EE be a , let WEW_E be its , and let the G^\widehat G carry the WEW_E-action determined by a GG. The stack of local LL-parameters is the

LocSysG^(WE)=[Z1(WE,G^)/G^],\operatorname{LocSys}_{\widehat G}(W_E) = [Z^1(W_E,\widehat G)/\widehat G],

where Z1(WE,G^)Z^1(W_E,\widehat G) is the moduli scheme of suitably continuous 11-cocycles and G^\widehat G acts by conjugation.

A cocycle ϕ\phi is equivalently a homomorphism WELGW_E\to{}^LG into the whose projection to WEW_E is the identity.

Why a stack

The of a point is the

Sϕ=CentG^(ϕ).S_\phi=\operatorname{Cent}_{\widehat G}(\phi).

Keeping this is necessary for and categorical actions. The coarse conjugacy-class set loses it, and the invariant-function spectrum can identify nonclosed orbits with their .

Algebraic construction

For p\ell\neq p and a coefficient ring Λ\Lambda, continuity must be formulated uniformly in families. Fargues–Scholze use condensed 11-cocycles. The resulting Z1(WE,G^)Z^1(W_E,\widehat G) is a union of open and closed indexed by sufficiently deep wild-inertia quotients; each finite-depth piece is a flat local complete intersection under their hypotheses.

Parameter content

This stack records Weil-group cocycles. In the Fargues–Scholze semisimplified correspondence it does not retain a separate monodromy operator or Deligne SL2\operatorname{SL}_2. Thus it should not be identified without qualification with the moduli of full .

Spectral role

Global functions on the stack form the , while on it act on sheaves on BunG\operatorname{Bun}_G through the .

References
  1. Laurent Fargues and Peter Scholze, “Geometrization of the local Langlands correspondence,” Chapters VIII and I.8. arXiv.
  2. Jean-François Dat, David Helm, Robert Kurinczuk, and Gilbert Moss, “Moduli of Langlands parameters,” 2020. arXiv.