Chapter XII: Cohomological correspondences between Shimura varieties
12.2 Main Theorem
Let(πΊ1, π1) and(πΊ2, π2)be two Hodge type Shimura data (cf. [Mil05]) equipped with an isomorphism π : πΊ1,
Aπ ' πΊ2,
Aπ. Let {ππ} denote the conjugacy class of Hodge cocharacters determined by ππ and consider them as dominant characters of Λπ. In particular, π1 and π2 are both minuscule. Then [XZ17, Corollary 2.1.5]
implies that there is a canonical inner twistΞ¨R:πΊ1β πΊ2overC. Recall notations in Β§1.3. We defineππ,ad to be the composition ofππwith the quotientπΊ β πΊadand consider it as a character of Λπsc. We assume that
π1,ad |
π(πΊΛ
ΞQ
sc )= π2,ad |
π(πΊΛ
ΞQ sc ) .
It follows from [XZ17, Corollary 2.1.6] thatΞ¨Rcomes from a unique global inner twistΞ¨ : πΊ
1 Β―Q β πΊ
2 Β―Q such thatΞ¨ = Int(β) β¦π, for some π : πΊ1,
Aπ ' πΊ2,
Aπ and ββπΊ2,ad(AΒ―π).
We assume thatπΎπ β πΊ(Aπ) to be sufficiently small such thatπ πΎ1=πΎ2. Choose a prime πsuch thatπΎ1, π (and therefore πΎ2, π) is hyperspecial. LetπΊπ be the integral model ofπΊπ,
QπoverZπdetermined byπΎπ, π. ThenπΊ1 'πΊ2, and we can thus identify their Langlands dual groups (πΊ ,Λ π΅,Λ πΛ). Choose an isomorphism π : C ' QΒ―π. Let π | π be a place of the compositum of reflex fields of (πΊπ, ππ) determined by our choice of isomorphismπ. We write Shππfor the mod πfibre of the canonical integral model of ShπΎπ(πΊπ, ππ) base change toππ. We make the following assumption
π1 |
π(πΊΛ
ΞQπ)= π2 |
π(πΊΛ
ΞQπ) . (12.2)
The assumption guarantees the existence of the ind-scheme Shπ1|π2 which fits into the following commutative diagram
Shπ1,πΎ1 Shπ1|π2 Shπ2,πΎ2
Shtlocπ1 Shtlocπ
1|π2 Shtlocπ2
ββ βπ
1
locπ
β
β βπ
2
locπ
ββ βloc
π1
β
β βloc
π2
, (12.3)
and makes both squares to be Cartesian.
Remark 12.2.1. In the case that(πΊ1, π1)= (πΊ2, π2),Shπ1|π2is the perfection of the mod p fibre of a natural integral model of some Hecke correspondence. If(πΊ1, π1) β (πΊ2, π2), thenShπ1|π2can be regarded as βexotic Hecke correspondencesβ between mod p fibres of different Shimura varieties. We refer to [XZ17, Β§7.3.3, Β§7.3.4] for a detailed discussion.
Let (πΊπ, ππ) π = 1,2,3 be three Hodge type Shimura data, together with the iso- morphismsππ, π :πΊπ,
Aπ 'πΊπ ,
Aπ satisfying the natural cocycle condition. Choose a common level πΎ using the isomorphismππ, π. Let π be an unramified prime, such that the assumption(12.2)holds for each pair of( (πΊπ, ππ),(πΊπ, ππ)). Choose a half Tate twistQβ(1/2).
Let ππ := ππ
π be the highest weight representation of ΛπΊ
Qβ of highest weight ππ. Write πeπ β CohπΊΛQβ(πΊΛ
Qβπ) for the vector bundle associated to ππ analogous to
Β§11.4. Recall fromΒ§12.1 that, to each representationπ ofπΊ
Qβ, we can attach the Γ©tale local systemLπ ,Qβ on Shππ. Letππ =h2π, ππi=dim ShπΎ(πΊπ, ππ). Denote the global section of the structure sheaf on the quotient stack [πΊ πΛ /πΊΛ] by J, and the prime-to-π Hecke algebra byHπ.
Theorem 12.2.2. There exists a map Spc : Hom
CohπΊΛQβ(πΊΛ
Qβπ)(πe1,πe2) βHomHπβJ(Hβπ(Shπ1,Lπ ,Qβhπ1i),Hβπ(Shπ2,Lπ ,Qβhπ2i), (12.4)
which is compatible with compositions on the source and target.
Proof. Choose a latticeΞπ βRepZ
β(πΊΛ
Zβ)inππ. We denote byΞeπ βCohπΊΛZβ(πΊΛ
Zβπ) the coherent sheaf which corresponds toΞπ as in Β§11.1. Then
HomCohπΊΛQβ(πΊΛ
Qβπ)(πe1,πe2) 'HomπΊΛ
Qβ
(π1, π2βQβ[πΊΛ]) (12.5) 'HomπΊΛ
Qβ
(Ξ1βZ
βQβ,(Ξ2βZ
β Zβ[πΊΛ]) βZ
βQβ) 'HomπΊΛ
Zβ
(Ξ1,Ξ2βZβ Zβ[πΊΛ]) βZβ Qβ 'Hom
CohπΊΛZβ(πΊΛ
Zβπ)(fΞ1,Ξf2) βZβQβ. By Theorem 11.2.1, we get a map
SΞ1,Ξ2 : Hom
CohπΊΛZβ(πΊΛ
Zβπ)(Ξf1,Ξf2) βCorrShtloc(π(Ξf1), π(Ξf2)). (12.6) Combining(12.5)with(12.6), we get the following map
HomCohπΊΛQβ(πΊΛ
Qβπ)(πe1,πe2) βCorrShtloc(π(Ξf1), π(Ξf2)) βZβ Qβ. (12.7) Choose a dominant coweightπand a quadruple (π1, π1, π2, π2)that is (π1+π, π)- acceptable and(π2+π, π)-acceptable. We have the following diagram
Shπ1 Shππ
1|π2 Shπ2
Shtlocπ1 Shtπ,loc
π1|π2 Shtlocπ2
Shtloc(π1 π1,π1) Shtπ,πloc(π1,π1)
1|π2 Shtloc(π2 π2,π2)
ββ βπ
1
locπ locππ
β
β βπ
2
locπ
ββ βloc
π1
resπ1, π1
β
β βloc
π2
resππ1, π1 resπ2, π2
ββ βloc(π1
, π1) π1
β
β βloc(π2
, π2) π2
, (12.8)
where
β’ all squares are commutative (discussions on diagram (10.5) and diagram (12.3),
β’ except for the square at the down right corner, and the other three squares are Cartesian (discussions on diagram(12.3)and diagram (12.5),
β’ the morphismββ βπ
1 is perfectly proper ([XZ17, Lemma 5.2.12]),
β’ the morphisms locπ(ππ, ππ) are perfectly smooth (Proposition 12.1.1).
Then the morphism locππ(π1, π1) := resππ1,π1 β¦locππ is also perfectly proper. Thus we can pullback the cohomological correspondences (cf. [XZ17, A.2.11)]) on the right hand side of (12.6) along locππ(π1, π1)to obtain a map
locππ(π1, π1)β : CorrShtloc(π(Ξf1), π(Ξf2)) β CorrShπ
π|π(locπ(π1, π1)β π(fΞ1),locπ(π2, π2)β (π(Ξf2)). Note that ππ are minuscule, then theβ -pullback ofπ(Ξeπ)along locπ(ππ, ππ)equals
Zβhππi. Next, we construct a natural map βπ : CorrShπ
π1|π 2
(Shπ1,Zβhπ1i),(Shπ2,Zβhπ2i)
βCorrShπ
π1|π 2
(Shπ1,Lπ ,Zβhπ1i),(Shπ2,Lπ ,Zβhπ2i) . (12.9)
For eachπ βZ+, we note that there exists an ind-scheme Sh(π)
π1|π2 which fits into the following commutative diagram such that both squares are Cartesian
Shπ1,πΎ(π)
β πΎβ Shπ,(π)
π1|π2 Sh
π2,πΎ(π)
β πΎβ
Shπ1 Shππ
1|π2 Shπ2.
ββ βπ(π)
1
ππ
1
β
β β(π)π
2
ππ ππ
2
ββ βπ
1
β
β βπ
2
Here the three vertical maps are the natural quotients by the finite groupπΎβ/πΎπ
β and are thus Γ©tale.
Let (ππ)π : (ββ βπ
1)β(Z/βπZhπ1i)π β (ββ βπ
2)!(Z/βπZhπ2i)π be a cohomological cor- respondence in CorrShπ
π1|π2
(Shπ1,Zβhπ1i),(Shπ2,Zβhπ2i)
. For each π β Z+, the shifted pullback (cf. [XZ17, A.2.12]) of ππgives rise to a cohomological correspon- dence
Λ ππ: (ββ
β(
π)
π1 )β(Z/βπZhπ1i) β (ββ β(
π)
π2)!(Z/βπZhπ2i)
in CorrShπ ,(π)
π1|π2
(Shπ
1,πΎ(
π) β
πΎβ
,Z/βπZhπ1i),(Shπ
2,πΎ(
π) β
πΎβ
,Z/βπZhπ2i)
. For any repre- sentationπofπΊ
Qβ, recall theZ/βπZmoduleΞπ ,β/βπΞπ ,βconstructed in Β§12.2. The cohomological correspondence Λππgives rise to a cohomological correspondence
Λ
ππβCorr
Shπ ,(π)π
1|π2
(Shπ1,πΎ(π)
β
πΎβ ΓΞπ ,β/βπΞπ ,βhπ1i,Sh
π2,πΎ(π)
β
πΎβ ΓΞπ ,β/βπΞπ ,βhπ2i). In addition, the cohomological correspondence Λππ isπΎβ/πΎ(π)
β -equivariant. Then it follows that the cohomological correspondence Λππ is alsoπΎβ/πΎ(
π)
β -equivariant and descends to a cohomological correspondence
ππ βCorrShπ
π1|π2
( (Shπ1,Lπ ,β,πhπ1i),(Shπ2,Lπ ,β,πhπ2i)). Definingβπ( (ππ)π) :=(ππ)πcompletes the construction ofβπ. Compose the maps we previously construct,
CorrShtπ ,πloc(π1, π1)
1|π2
(Shtlocπ1(π1,π1), π(fΞ1)loc(π1,π1)),(Shtlocπ1(π2,π2), π(Ξf2)loc(π2,π2)) (12.10)
locππ(π1,π1)β
βββββββββββCorrShπ
π1|π2
( (Shπ1,Zβhπ1i),(Shπ2,Zβhπ2i))
βπ
ββββCorrShπ
π1|π 2
( (Shπ1,Lπ ,Zβhπ1i),(Shπ2,Lπ ,Zβhπ2i))
Hβπ
βββHomHπ(Hβπ(Shπ1,Lπ ,Zβhπ1i),Hβπ(Shπ2,Lπ ,Zβhπ2i)).
We justify that the composition of maps in(12.11)factors through CorrShtloc(π(πe1), π(πe2)).
Note that the proof of Lemma 11.2.3.(3) and the definition of locππ(π1, π1)β imply that for a quadruple (π0
1, π0
1, π0
2, π0
2) of (π1 + π, π)-acceptable and (π2 + π, π)- acceptable integers, the functor locππ(π1, π1)β commutes with the connecting mor- phism in(10.12)(withπ1,π2,πfixed). Letπ β€ π0and(π0
1, π0
1, π0
2, π0
2)be a quadruple of non-negative integers satisfying appropriate acceptance conditions. The proper smooth base change shows that locππ(π0
1, π0
1)β commutes with enlargingπ toπ0. In addition, the proper smooth base change together with the construction ofβπ show that the following diagram commutes:
CorrShπ
π1|π 2
( (Shπ1,Zβhπ1i),(Shπ2,Zβhπ2i)) CorrShπ
π1|π 2
( (Shπ1,Lπ ,Zβhπ1i),(Shπ2,Lπ ,Zβhπ2i))
CorrShπ0
π1|π2
( (Shπ1,Zβhπ1i),(Shπ2,Zβhπ2i)) CorrShπ0
π1|π2
( (Shπ1,Lπ ,Zβhπ1i),(Shπ2,Lπ ,Zβhπ2i)).
βπ
πβ πβ
βπ
Thus the map βπ is compatible with the enlargement of π. Finally, by [XZ17, Lemma A.2.8], the composition of maps Hβπβ¦βπ commutes with enlargingπtoπ0. We complete the proof of the statement at the beginning of this paragraph.
Composing(12.7)with(12.11), we get a canonical map HomCohπΊΛQβ(πΊΛ
Qβπ)(πe1,πe2) βHomHπ(Hβπ(Shπ1,Lπ ,Qβhπ1i),Hβπ(Shπ2,Lπ ,Qβhπ2i)). (12.11) The fact that (12.9) is compatible with the compositions of the source and target can be proved in an analogous way as [XZ17, Lemma 7.3.12], and we omit the details. Then the action of J naturally translates to the right hand side of (12.9) and upgrades it to our desired map
Spc : Hom
CohπΊΛ(πΊ πΛ )(πe1,πe2) βHomHπβJ(Hβπ(Shπ1,Lπ ,Qβhπ1i),Hβπ(Shπ2,Lπ ,Qβhπ2i)). As discussed in loc.cit, the action of J on Hβπ(Shππ,Lπ ,Qβhππi) is expected to coincide with the usual Hecke algebra action, which may be understood as the Shimura variety analogue of V. Lafforgueβs "π = π" theorem (cf. [Laf18]). We prove this in the case of Shimura sets.
Proposition 12.2.3. LetShπΎ(πΊ , π) be a zero-dimensional Shimura variety. Then the action ofJonHβπ(Shππ,Lπ ,Qβhππi)is given by the classical Satake isomorphism.
Proof. Let π β J. Since the Shimura variety we consider is zero-dimensional, it follows from [XZ17, A.2.3(5)] that the cohomological correspondence locβ π(SO(π)) can be identified with a Zβ-valued function on Shπ|π. By our construction of the map Spc, this function is given by the pullback of a function π0 on Shtlocπ|π = πΊ(Zπ)\πΊ(Qπ)/πΊ(Zπ). Corollary 11.2.5(2) thus implies that the function π0 is exactly the function SO(π) β π»
πΊ ,πΈ[πβ1/2, π1/2] which is the image of π under the classical Satake isomorphism.
For any π β Z+, takeπ = Zπβ. Recall our construction ofβπ, the cohomological correspondence Λππis given by a finite direct sum of the function locβ π(SO(π))since the Shimura variety we consider is a set of discrete points. Then the action of Spc(π) on Hβπ(Shππ,Lπ ,Qβhππi) is given by the classical Satake isomorphism. For generalπ, we take resolutions of it as in (12.10), and the statement follows from
the caseπ =Zπβ.
12.3 Non-Vanishing of the Geometric Jacquet-Langlands Transfer