For a multiple-leg with legs indexed by II, a partial Frobenius associated to a subset JIJ\subset I applies the qq-power to the leg coordinates in JJ while leaving the other legs fixed, together with the corresponding rotation of the Frobenius-modification chain.

On the base XIX^I, the map is

FrobJ((xi)iI)=(xi)iI,xi={FrobX(xi),iJ,xi,iJ.{\rm Frob}_J((x_i)_{i\in I})=(x_i')_{i\in I}, \qquad x_i'= \begin{cases} {\rm Frob}_X(x_i),&i\in J,\\ x_i,&i\notin J. \end{cases}
Modification-chain description

For an ordered partition I=I1IkI=I_1\sqcup\cdots\sqcup I_k, a shtuka is a chain from G0\mathcal G_0 to τG0{}^\tau\mathcal G_0. Partial Frobenius for the first block moves that block to the end, replaces G0\mathcal G_0 by the next bundle in the chain, and applies Frobenius to the moved legs. This gives a morphism between the appropriately ordered shtuka stacks.

Relations

Partial Frobenius operators for disjoint individual legs commute. Their product over all legs is the total Frobenius action. On the inductive system of truncated shtuka cohomology, an operator may enlarge the ; it is therefore naturally a map in that inductive system rather than always an endomorphism of one finite-type truncation.

From Frobenius to Galois

turns a over a power of a curve equipped with commuting partial Frobenius structures into a representation of a product of . This is the source of the independent Galois actions (γi)iI(\gamma_i)_{i\in I} in an .

References
  1. Vincent Lafforgue, “Chtoucas pour les groupes réductifs et paramétrisation de Langlands globale,” §§0.2–0.4 and Chapter 3. arXiv.
  2. Cong Xue, “Smoothness of cohomology sheaves of stacks of shtukas,” 2020. arXiv.