Chapter VIII: Ind-constructible Weil sheaves
8.1 Ind-constructible Weil sheaves
LetFπ be a finite field of characteristic π > 0, and fix an algebraic closureF. Let π1, . . . , ππbe schemes of finite type overFπ. LetΞbe a condensed ring associated with the one of the following topological rings: a discrete coherent torsion ring (for example, a discrete finite ring), an algebraic field extensionπΈ β Qβ, or its ring of integersOπΈ. We writeπ := π
1ΓFπ. . .ΓFπ ππ, and denote byππ,
F := ππΓFπSpecF and π
F := πΓFπ SpecFthe base change. Recall that under these assumptions, by Chapter 5 Item viii, we have a fully faithful embedding
Ind Dcons(π
F,Ξ)
ββDindcons(π
F,Ξ) β D(π
F,Ξ), (8.1) and likewise for (ind-)lisse sheaves.
Definition 8.1.1. An object π β D(πWeil
1 Γ . . . Γ πWeil
π ,Ξ) is called ind-lisse, resp. ind-constructible if the underlying sheafπ
F βD(π
F,Ξ)is ind-lisse, resp. ind- constructible in the sense of Definition 5.0.1.
We denote by
Dindlis πWeil
1 Γ. . .ΓπWeil
π ,Ξ
β Dindcons πWeil
1 Γ. . .Γ πWeil
π ,Ξ the resulting full subcategories of D(πWeil
1 Γ. . .ΓπWeil
π ,Ξ) consisting of ind-lisse, resp. ind-constructible objects. Both categories are naturally commutative algebra objects in PrStΞβ(see the notation from Chapter 4), that is, presentable stableΞβ-linear symmetric monoidalβ-categories whereΞβ := Ξ(β,Ξ)is the ring underlyingΞ. It is immediate from Definition 8.1.1 that the equivalence (6.6) restricts to an equivalence
Dβ’ πWeil
1 Γ. . .Γ πWeil
π ,Ξ Fix
Dβ’(π
F,Ξ), πβ
π1
, . . . , πβ
ππ
forβ’ β {indlis,indcons}.
Remark 8.1.2. Note that that we have a fully faithful embedding of π·
cons(πWeil) intoDindcons(πWeil) whose image consists of compact objects. However, the latter category is not generated by this image. Indeed, even in the case of a point, the ind-cons category consists ofΞ-modules with an action of an endomorphism, whereas the image of the embedding consists of Ξ-modules with an action of an automorphism. This automorphism does not have to fix any finitely generated submodule, which would be the case for any objects generated by the image of the constructible Weil complexes.
Our goal in this chapter is to obtain a categorical KΓΌnneth formula for the categories of ind-lisse, resp. ind-constructible Weil sheaves. In order to state the result, we need the following terminology. Under our assumptions onΞ, each cohomology sheaf Hπ(π), π βZfor π βDlis(π
F,Ξ
is naturally a continuous representation of the proΓ©tale fundamental groupoidπproΒ΄et
1 (π
F)on a finitely presentedΞ-module, see 6.5.4. Further, the projectionsπ
F β ππ,
Finduce a full surjective map of topological groupoids
πproΒ΄et
1 (π
F) β πproΒ΄et
1 (π
1,F) Γ. . .ΓπproΒ΄et
1 (ππ,
F). (8.2)
Definition 8.1.3. Letπ βD(π
F,Ξ).
1. The sheaf π is called split lisse if it is lisse and the action of πproΒ΄et
1 (π
F) on Hπ(π)factors through(8.2)for all π βZ.
2. The sheafπis called split constructible if it is constructible and there exists a finite subdivision into locally closed subschemes ππ,πΌ β ππ such that for each ππΌ =Γ
πππ,πΌ β π, each restrictionπ|ππΌ is split lisse.
Definition 8.1.4. An objectπ βD(πWeil
1 Γ. . .ΓπWeil
π ,Ξ)is called ind-(split lisse), resp. ind-(split constructible) if the underlying objectπ
F βD(π
F,Ξ)is a colimit of split lisse, resp. split constructible objects.
As the category Dβ’(π
F,Ξ), β’ β {indlis,indcons} is cocomplete, every ind-(split lisse) object is ind-lisse, and likewise, every ind-(split constructible) object is ind- constructible.
Theorem 8.1.5. Assume thatΞis either a finite discrete ring of prime-to-πtorsion, an algebraic field extensionπΈ β Qβ forβ β π, or its ring of integersOπΈ. Then the functor induced by the external tensor product
Dβ’(πWeil
1 ,Ξ) βModΞβ. . .βModΞβ Dβ’(πWeil
π ,Ξ) β Dβ’(πWeil
1 Γ. . .ΓπWeil
π ,Ξ) (8.3) is fully faithful for β’ β {indlis, indcons}. For β’ = indlis, resp. β’ = indcons the essential image contains the ind-(split lisse), resp. ind-(split constructible) objects.
Proof. For full faithfulness, it is enough to consider the caseβ’ = indcons. Using Lemma 4.2.5, it remains to show that the functor
Γ
π
Dindcons ππ,
F,Ξ) Ind Γ
π
Dcons(ππ,
F,Ξ)
!
βDβ’(π
F,Ξ) (8.4) is fully faithful. In view of Equation (8.1), this is immediate from the KΓΌnneth formula for constructibleΞ-sheaves as explained in Section 7.3.
To identify objects in the essential image, we note that the fully faithful functors Equation (8.3) and Equation (8.4) induce a Cartesian diagram (see Lemma 4.2.5):
Γ
πDβ’ πWeil
π ,Ξ) //
Dβ’(πWeil
1 Γ. . .ΓπWeil π ,Ξ)
Γ
πDβ’(ππ,
F,Ξ) //Dβ’(π
F,Ξ),
(8.5)
forβ’ β {indlis, indcons}. Thus, it is enough to show that the object π
Funderlying an ind-split object π lies in the image of the lower horizontal arrow. Since this essential image is closed under colimits, it remains to show it contains the split lisse objects forβ’=indlis, resp. the split constructible objects forβ’=indcons.
By the full faithfulness of Equation (8.4), the split constructible case reduces to the split lisse case, see also the proof of 7.1.2 in Section 7.6. So assumeβ’=indlis and let π
F β D(π
F,Ξ) be split lisse. As each cohomology sheaf Hπ(π
F), π β Zis at least ind-lisse, an induction on the cohomological length of π
Freduces us to show that Hπ(π
F) lies in the essential image. By definition, being split lisse implies that the action ofπproΒ΄et
1 (π
F)on Hπ(π
F)factors throughπproΒ΄et
1 (π
1,F) Γ. . .ΓπproΒ΄et
1 (ππ,
F). Then the arguments of Section 7.6 show that Hπ(π
F)lies is in the essential image of the lower horizontal arrow in Equation (8.5). We leave the details to the reader. β‘ Remark 8.1.6. The functor Equation(8.3) is not essentially surjective in general.
To see this, note that the functor Dindcons(πWeil,Ξ) β Dindcons(π
F,Ξ) admits a left adjoint πΉ that adds a free partial Frobenius action. Explicitly, for an object π β Dindcons(π
F,Ξ) the object πΉ(π) has underlying sheaf πΉ(π)F given by a countable direct sum of copies of π. If π was not originally in the image of the external tensor product, then πΉ(π) will not be either. This is, however, the only obstacle for essential surjectivity: as noted in the proof of Theorem 8.1.5, the diagram Equation(8.5)is Cartesian.