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ANNALES MATHÉMATIQUES

BLAISE PASCAL

Avner Ash & Darrin Doud

Reducible Galois representations and arithmetic homology forGL(4) Volume 25, no2 (2018), p. 207-246.

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Reducible Galois representations and arithmetic homology for GL ( 4 )

Avner Ash

Darrin Doud

Abstract

We prove that a sum of two odd irreducible two-dimensional Galois representations with squarefree relatively prime Serre conductors is attached to a Hecke eigenclass in the homology of a subgroup of GL(4,Z), with the level, nebentype, and coefficient module of the homology predicted by a generalization of Serre’s conjecture to higher dimensions. To do this we prove along the way that any Hecke eigenclass in the homology of a congruence subgroup of a maximal parabolic subgroup of GL(n,Q)has a reducible Galois representation attached, where the dimensions of the components correspond to the type of the parabolic subgroup. Our main new tool is a resolution ofZby GL(n,Q)-modules consisting of sums of Steinberg modules for all subspaces ofQn.

1. Introduction

Serre’s conjecture [23] (now a theorem of Khare, Wintenberger, and Kisin [18, 19, 20]) gives a connection between odd irreducible Galois representationsρ:GQ→GL(2,F¯p) and modular forms that are simultaneous eigenvectors of all the Hecke operators. Via the Eichler–Shimura isomorphism [24], it can be interpreted as giving a connection between such Galois representations and elements of a cohomology groupH10(N),V)for an appropriate coefficient moduleV. This interpretation of Serre’s conjecture was generalized by [10] to a conjecture relating odd Galois representations ρ : GQ → GL(n,F¯p) to eigenclasses of the Hecke operators in cohomology groups H0(n,N),V), where Γ0(n,N)is the congruence subgroup of SL(n,Z) that generalizes Γ0(N) ⊂ SL(2,Z). Refinements of the conjecture [8, 16] make more precise predictions concerning the proper coefficient modules.

Some proven cases of the conjectured connection between Galois representations and cohomology eigenclasses are known. In particular, the conjecture is known for two- dimensional Galois representations. In [12], the conjecture is proven for certain irreducible symmetric square representations of odd irreducible two-dimensional representations.

Our long-term goal is to prove the conjecture for any odd reducible Galois representation under the assumption that the conjecture holds for each constituent. In [3], odd Galois representations that are sums of characters are shown to correspond to cohomology eigenclasses. This work was extended in [5] to show that any sum of characters with a Galois representation satisfying the conjecture such that the resulting representation

Keywords:Galois representations, arithmetic homology.

2010Mathematics Subject Classification:11F75, 11R80.

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is odd will satisfy the conjecture. In [6], it is shown that if ρ1 and ρ2are two Galois representations, each attached to a cohomology eigenclass with trivial coefficient module, then a twisted sum of the two representations will also be attached to a cohomology Hecke eigenclass with trivial coefficients (although not in the cohomology of a group of the formΓ0(n,N)).

In this paper, we prove that Galois representations of the formρ1⊕ρ2of squarefree level N with ρ1 and ρ2 two-dimensional irreducible and odd are attached to Hecke eigenclasses in the cohomology ofΓ0(4,N). Together with our previous results cited above, we have now proven the conjecture of [8] for all odd reducible four-dimensional Galois representations, as long as the constituents have squarefree pairwise relatively prime conductors, and satisfy the conjecture themselves.

The two main new tools that we use in the proof are an exact sequence of GL(n,K)- modules for any fieldKthat involves the Steinberg modules for GL(W)for all subspaces W ofKn (Section 4), and Theorem 11.5 on the reducibility of Galois representations attached to the cohomology of arithmetic subgroups of parabolic subgroups of GL(n,Q). The exact sequence of Section 4 generalizes the exact sequence used in [5, 7], which only works forn=3, to arbitraryn. It is a resolution ofZby non-free modules which are induced from various parabolic subgroups. Using a certain Hecke equivariant spectral sequence arising from this exact sequence, we are able to construct a system of Hecke eigenvalues that have ρ1⊕ρ2attached.

Our other main tool, Theorem 11.5 proves that any Hecke eigenclass attached to the cohomology of a maximal parabolic subgroup of type(n1,n2)has an attached Galois representation that is a sum of (possibly reducible) Galois representationsρ1⊕ρ2, with ρi :GQ→GL(ni,F¯p)fori=1,2.

On the more technical side, this paper includes extensions fromn=3 to generaln of the study we made in [5, 7] of orbits of subspaces ofQn under certain congruence subgroups of GL(n,Z). We also study the action of a Levi component on the groups H(Γ∩U,M)appearing in the Hochschild–Serre spectral sequence for

1→Γ∩U→Γ∩P→Γ∩L→1,

where U is the unipotent radical of a maximal parabolic subgroupP=LUof GL(n,Q). We show in Theorem 7.11 that under certain hypotheses, the Hecke algebra forΓP acts in an equivariant fashion on the spectral sequence. This is surprisingly hard to do and we don’t even know if this continues to be the case if Pis not maximal. A third generalization of our earlier work concerns the detailed action of the matrices defining the Hecke operators on the homology. The last new technical point regards the interplay of the Hecke operators and the Künneth formula in Section 10.

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We expect to be able to apply these methods to higher dimensional Galois represen- tations; at present, we are not able to because we have not yet been able to prove that a certain Hochschild–Serre spectral sequence, used to construct the systems of Hecke eigenvalues that we need, degenerates whenn>4.

We know that a system of Hecke eigenvalues appears inHk0(n,N),V)if and only if it appears inHk0(n,N),V). We have discussed mostly cohomology in the introduction to conform with common usage. Our theorems and proofs below will all be stated for homology.

2. Galois representations, Hecke Operators, cohomology and homology Letp>2 be a prime number, and letF=Fp. Throughout the paper, we use Borel–Serre duality for subgroups of GL(n,Z)[13, Section 11.4], and the fact that the Borel–Serre duality isomorphism is Hecke equivariant [9, Corollary 3]; when we do this we will requirep >n+1, so that no torsion element of GL(n,Z)has order divisible byp. By a Galois representation we mean a continuous homomorphism ρ:GQ→GL(n,F)for some positive integern. For each prime`, we fix a choice of Frobenius element Fr`∈GQ; we use the arithmetic Frobenius, so that ifω : GQ → F is the cyclotomic character, ω(Fr`)=`. Ifρis unramified at`, thenρ(Fr`)is defined up to similarity. Hence, forρ unramified at`, the characteristic polynomial det(I−ρ(Fr`)X)ofρ(Fr`)is well defined.

Definition 2.1. Letn>1 andN ∈N, and letpbe a prime inZ.

(1) S0±(n,N)consists of the set of alln×nmatrices with integer entries and nonzero determinant prime topNwhose first row is congruent to(∗,0, . . . ,0)moduloN. (2) S0(n,N)consists of elements ofS0±(n,N)with positive determinant.

(3) Γ0±(n,N)=S0±(n,N) ∩GL(n,Z). (4) Γ0(n,N)=S0(n,N) ∩SL(n,Z).

For a given primepand positive integerNprime top,(Γ0(n,N),S0(n,N))is a Hecke pair (see [1]), and we denote theF-algebra of its double cosets byHn,N. We note that Hn,N is commutative, and is generated by the double cosets

Γ0(n,N)s(`,n,k)Γ0(n,N),

wheres(`,n,k)=diag(1, . . . ,1, `, . . . , `)is a diagonal matrix withkcopies of`on the diagonal,`runs over all primes not dividingpN, and 0≤k≤n. The algebraHn,N acts on the homology or cohomology ofΓ0(n,N)with coefficients in anyF[S0(n,N)]-module

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M. When the double coset ofs(`,n,k)acts on homology or cohomology, we will denote it byTn(`,k).

Definition 2.2. LetVbe anyHn,N-module, and suppose thatv∈V is a simultaneous eigenvector of all theTn(`,k)for` - pN, with eigenvalues a(`,k) ∈ F. Suppose that ρ:GQ→GL(n,F)is a Galois representation unramified outsidepN. We say thatρis attachedtovif, for all`-pN,

det(I−ρ(Fr`)X)= Õn

k=0

(−1)k`k(k1)/2a(`,k)Xk. Ifρis attached tov∈V, we will also say thatρfitsV.

3. Conjectures relating Galois representations and arithmetic homology/co- homology

Definition 3.1([7]). LetSbe a subsemigroup of the matrices in GL(n,Q)with integer entries whose determinants are prime to pN. A(p,N)-admissible S-moduleM is an F[S]-module of the formM0⊗F, whereM0is anF[S]-module on whichS∩GL(n,Q)+ acts via its reduction modulop, andis a character:S →F×which factors through the reduction ofSmoduloN. HereFis the vector spaceF, withSacting as multiplication via . An admissible module is one which is(p,N)-admissible for some choice ofpandN. We can construct(p,N)-admissible modules by starting with GL(n,Fp)-modules, and lettingSact via reduction modulop. We have the following parametrization of irreducible GL(n,Fp)-modules.

Theorem 3.2([15]). Call ann-tuple of(a1, . . . ,an)of integersp-restricted if0≤an <

p−1and, for eachi <n,0 ≤ ai −ai+1 ≤ p−1. Then there is a bijection between p-restrictedn-tuples of integers and irreducibleF[GL(n,Fp)]-modules, with then-tuple (a1, . . . ,an)corresponding to the unique simple submodule of the dual Weyl module with highest weight(a1, . . . ,an).

Definition 3.3. Denote byF(a1, . . . ,an)the irreducibleF[GL(n,Fp)]-module correspond- ing to thep-restrictedn-tuple(a1, . . . ,an).

As described above,F(a1, . . . ,an)becomes anS-module on whichSacts via reduction modulop. We will relax the condition on the value ofan, allowing it to be an arbitrary integer; this has the effect that a given module corresponds to infinitely manyn-tuples, all congruent to somep-restrictedn-tuple modulop−1, and it allows flexibility in specifying modules. Given a character:S→F×that factors through the reduction ofSmoduloN, we see thatF(a1, . . . ,an) =F(a1, . . . ,an) ⊗F is a(p,N)-admissible module.

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If S = S0(n,N) and : (Z/NZ)× → F× is a character, we will also denote by :S→F×the character sendings∈Sto the image underof the modNreduction of the(1,1)entry ofs. In this case, we callanebentype character.

In order to state the main conjecture of [8], we recall the following definition.

Definition 3.4. Forn > 1, a Galois representationρ : GQ → GL(n,F)is odd if the image of complex conjugation is similar to a matrix with alternating 1’s and−1’s on the diagonal. A Galois representation ρ:GQ →GL(1,F)=F×is odd if the image of complex conjugation is−1, and is called even otherwise.

Conjecture 3.5([8, Conjecture 3.1]). For any odd Galois representation ρ: GQ → GL(n,F), we may find an integerN(called the level), an irreducibleGL(n,Fp)-module M (called the weight), and a Dirichlet character(called the nebentype), such thatρfits Hk0(N),M).

In fact, [8, Conjecture 3.1] predicts the level, weight and nebentype from the structure of ρ. We do not give these definitions in detail in this paper; see [8] for detailed descriptions.

In this paper, we will generalize techniques developed in [3, 5, 7] to prove the following theorem.

Theorem 3.6. Letp>5. Fori=1,2, letρi :GQ→GL(2,F)be odd, irreducible Galois representations with squarefree relatively prime levels. Thenρ1⊕ρ2fits at least one of H60(n,N),M)orH20(n,N),M), withN,M, andas predicted by[8].

4. A Steinberg module exact sequence

Throughout this section, fix a fieldK. In this section, we derive a resolution ofZby GL(n,K)-modules that generalizes the resolution used in [5], which only works for GL(3,K).

For a vector spaceWoverK, denote byP(W)the projective space(W− {0})/K×of nonzero vectors inWmodulo scalar multiplication. For any collectionw1, . . . ,wk ∈P(W), we will denote by span(w1, . . . ,wk)the subspace ofW spanned by lifts of thewi toW (we see easily that the span is independent of the choice of lifts).

We recall the definition of the sharbly complex.

Definition 4.1([2]). LetW be ak-dimensional vector space over a fieldK. Fori ≥0, define thei-sharblies Shi(W)to be the freeZ-module generated by the(k+i)-tuples (w1, . . . ,wk+i)forwi ∈P(W), modulo theZ-span of the following elements:

(1) (wσ(1), . . . ,wσ(k+i)) − (−1)σ(w1, . . . ,wk+i)for all permutationsσ∈Sk+i,

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(2) (w1, . . . ,wk+i)if{w1, . . . ,wk+i}does not spanW.

We denote a basis element of thei-sharblies by the symbol[w1, . . .wk+i]where each wj ∈P(W), with (1) implying that this symbol is antisymmetric in the entries, and (2) implying that it is 0 if the entries do not spanW. By considering GL(W)to act onWby right multiplication, there is a natural right action of GL(W)on Shi(W). The boundary mapdi: Shi(W) →Shi−1(W)is given by

di([w1, . . . ,wk+i])= Õk+i

j=1

(−1)j[w1, . . . ,wˆj, . . . ,wk+i].

Thesharbly complexis the complex of right GL(W)-modules

· · · →Shi(W)−→di Shi1(W) → · · · →Sh1(W)−→d1 Sh0(W).

By [2] the Steinberg module St(W)is isomorphic to the cokernel of the mapd1 : Sh1(W) →Sh0(W), and therefore we get a resolution of the Steinberg module:

· · · →Shj(W) →Shj−1(W) → · · · →Sh1(W) →Sh0(W) →St(W) →0. We will denote the image of a 0-sharbly[w1, . . . ,wk]in St(W)bynw1, . . . ,wko. We note that ifWis 0-dimensional, the Steinberg module and the 0-sharblies are isomorphic toZ(with trivial GL(W)-action), generated by the empty symbolsn oand[ ]. IfW is 1-dimensional, we also have that the Steinberg module and the 1-sharblies are isomorphic toZ(with trivial GL(W)-action), generated by the symbolsnwoand[w], wherewis the unique element ofP(W).

Theorem 4.2. LetVbe ann-dimensional vector space overKwithn>0. Then there is an exact sequence ofGL(V)-modules

0→Ê

Wn

St(Wn)−→δn Ê

Wn−1

St(Wn−1)−→ · · ·δn−1 −→δ2 Ê

W1

St(W1)−→δ1 Ê

W0

St(W0) →0, where eachWi runs through all subspaces ofV of dimensioni, and the map

δk

Wk

St(Wk) →Ê

Wk−1

St(Wk−1) is defined by

δk(nw1, . . . ,wko)= Õk

j=1

(−1)jnw1, . . . ,wˆj, . . . ,wko, fornw1, . . . ,wko∈St(Wk), withWk =span(w1, . . . ,wk)and

nw1, . . . ,wˆj, . . . ,wko∈St(Wk−j 1), whereWjk1=span(w1, . . . ,wˆj, . . . ,wk).

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Proof. Forγ∈GL(V), and a generatornw1, . . . ,wko∈St(Wk), we define nw1, . . . ,wkoγ=nw1γ, . . . ,wkγo∈St(Wkγ).

With this action, we see easily that Ê

Wk

St(Wk)

is a GL(V)-module and thatδkis an equivariant map of GL(V)-modules.

We now check that eachδk is a well defined map.

To begin, letW be a k-dimensional subspace ofV. We may write the Steinberg module ofW asA(W)/(B(W)+C(W)), whereA(W)is the freeZ-module generated by antisymmetric symbols (w1, . . . ,wk)withwi ∈ P(W),B(W)is generated by all such symbols where w1, . . . ,wk are contained in a proper subspace ofWk, andC(W) is generated by elements of the form

k

Õ

j=1

(−1)j(w1, . . . ,wˆj, . . . ,wk).

Defineφ:A(W) → ⊕St(Wk−1)by (w1, . . . ,wk) 7→

k

Õ

j=1

(−1)jnw1, . . . ,wˆj, . . . ,wko.

Note that in any case where the symbolnw1, . . . ,wˆj, . . . ,wkois not in a unique Steinberg module because the dimension of the span ofw1, . . . ,wˆj, . . . ,wk is less thank−1= dimWk−1, the symbol vanishes, regardless of which module it is considered to lie in.

Hence, sinceA(W)is free overZ,φis well-defined, and ifφmaps bothB(W)andC(W) to 0, then the mapδkthat it induces onA(W)/(B(W)+C(W))will be well defined.

NowφmapsC(W)to 0 by the standard argument that the boundary of the boundary is 0. Further, if(w1, . . . ,wk) ∈B(W), then lettingWk−1be a(k−1)-dimensional subspace ofW containingw1, . . . ,wk, we find that

Õk

j=1

(−1)j(w1, . . . ,wˆj. . . ,wk) ∈C(Wk1).

NowC(Wk1)maps to 0 in St(Wk−1), soφ(w1, . . . ,wk)=0 andφ(B(W))=0. Thus, we see thatδkis well defined.

It is clear that the compositionδk−1◦δkis equal to 0 fork>0. In addition,δ1is clearly surjective, since there is only one zero-dimensional subspace ofVandδ1(w)=−n ofor anyw∈V.

Now we wish to prove that any element of kerδkis contained in the image ofδk+1.

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Suppose that for some index setA, and some integerscafora∈ A, we have s= Õ

a∈ A

canw1a, . . . ,wkao

is in the kernel ofδk for 0<k<n. We will show that it is in the image ofδk+1. Choose an arbitraryx∈P(V). Then

Õ

a

canx,wa1, . . . ,wkao∈Ê

Wk+1

St(Wk+1)

(note that some of the terms may be 0, ifx∈span(wa1, . . . ,wka)). In any case, we have

δk+1 Õ

a

canx,w1a, . . . ,wkao

!

=−Õ

a

canw1a, . . . ,wkao

−Õ

a

Õk

j=1

(−1)jcanx,w1a, . . . ,wˆaj, . . . ,wkao. Adding this tos, we obtain a new elements0∈kerδk that differs fromsby an element of the image ofδk+1. It thus suffices to prove thats0is in the image ofδk+1. We note that each symbol comprisings0has as its first component the chosenx. Hence, (changing the wia, theca, and indeed the index setA), we may write

s0= Õ

a∈ A

canx,w2a, . . . ,wkao. By eliminating terms where{x,w2a, . . . ,wa

k}does not span ak-dimensional space, we may also assume that for eacha, we havex<span(w2a, . . . ,wka).

Now,

0=δk(s0)=−Õ

a

canw2a, . . . ,wkao− Õk

j=1

Õ

a

(−1)jcanx,w2a, . . . ,wˆaj, . . . ,wkao. Since, for eacha, we havex<span(w2a, . . . ,wka), we see that no terms of the double sum are in the same component of

Ê

Wk−1

St(Wk−1) as any term in the first sum. Hence, we must have

Õ

a

canw2a, . . . ,wkao=0.

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For each(k−1)-dimensional subspaceWofV, setAW ={a: span(w2a, . . . ,wka)=W}. Then eachais in precisely oneAW. We see that for eachW

Õ

a∈ AW

canwa2, . . . ,wkao=0.

For anyW withAW nonempty, since the Steinberg module ofW is the cokernel of Sh1(W)−→d1 Sh0(W), we see that there is an index setB, integerscb and elements [y1b, . . . ,ybk] ∈Sh1(W)for eachb∈ Bsuch that

Õ

a∈ AW

ca[w2a, . . . ,wka]=d1 Õ

b∈ B

cb[y1b, . . . ,ybk]

!

b∈ B k

Õ

j=1

(−1)jcb[y1b, . . . ,yˆbj, . . . ,ykb].

LetWxbe the span ofWand a lift ofx. Then in Sh0(Wx)we have Õ

a∈ AW

ca[x,w2a, . . . ,wka]= Õ

b∈ B k

Õ

j=1

(−1)jcb[x,y1b, . . . ,yˆbj, . . . ,ykb].

Hence, in St(Wx), Õ

a∈ AW

canx,wa2, . . . ,wkao= Õ

b∈ B k

Õ

j=1

(−1)jcbnx,yb1, . . . ,yˆbj, . . . ,ykbo. Becausey1b, . . . ,ykbspan a(k−1)-dimensional subspace, this equals

−Õ

b

©

­

«

cbny1b, . . . ,ybko− Õk

j=1

(−1)jcbnx,y1b, . . . ,yˆbj, . . . ,ykb

®

¬ ,

which is equal to

−δk+1 Õ

b

cbnx,y1, . . . ,yko

! , so that

Õ

a∈ AW

canx,wa2, . . . ,wkao=δk+1 −Õ

b

cbnx,y1, . . . ,yko

! . Since this is true for allW, we have thats0

acanx,w2a, . . . ,wa

kois in the image of δk+1.

The proof thatδnis injective is similar, but usesd1 : Sh1(V) →Sh0(V)in place of the nonexistentδn+1, and is left to the reader (see [4, Theorem 2.1] for more details).

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5. Γ0(n,N)-orbits of subspaces ofQn

By considering the elements ofQnas row vectors, right multiplication by elements of GL(n,Q)yields a right action of GL(n,Q)onQn. This action restricts to an action of Γ0(n,N)onQn. In a natural way, we may also consider GL(n,Q)(and hence alsoΓ0(n,N)) as acting on the set ofk-dimensional subspaces ofQn, for 0≤k ≤n. We wish to find explicit representatives of theΓ0(n,N)-orbits ofk-dimensional subspaces. Note that for k =0 andk =n, there is only onek-dimensional subspace, and hence only one orbit, with a unique orbit representative.

Theorem 5.1. Let0<k<nand assume thatNis squarefree. Then theΓ0(n,N)-orbits of k-dimensional subspaces ofQnare in one-to-one correspondence with the set of positive divisors ofN, where the orbit corresponding to the divisordcontains thek-dimensional subspace spanned by

e1+dek+1,e2,e3,e4, . . . ,ek,

whereei denotes the standard basis element ofQnwith a1in theith column, and0’s elsewhere.

Multiplication by elements ofS0±(n,N)preserves theΓ0(n,N)-orbits.

Proof. LetW be ak-dimensional subspace, and letM be ak×nmatrix with integer entries whose rows spanW. Forγ∈Γ0(n,N),Mγhas row spaceWγ. Left multiplication by an element of GL(k,Q)does not change the row space of a matrix, so we wish to find a canonical element of the double coset

GL(k,Q)MΓ0(n,N).

Integer column operations on the rightmostn−1 columns ofMcan be represented by right multiplication by an element of Γ0(n,N); similarly, arbitrary row operations correspond to left multiplication by an element of GL(k,Q). Using these operations we find that the row space ofMisΓ0(n,N)-equivalent to the row space of

M0=

a 0tk−1 b 0 · · · 0

0k−1 Ik−1 0k−1 0k−1 · · · 0k1

,

wherea,b∈Zand gcd(a,b)=1. Here, 0k−1denotes the column vector of all zeros and lengthk−1, and 0tk−1denotes its transpose.

Since gcd(a,b)= 1, we may findr andsso thatar +bs =1. Then for all` ∈ Z, a(r+b`)+b(s−a`)=1 and for alld∈Z,

(a+d(s−a`))(r+b`)+(b−d(r+b`))(s−a`)=1.

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Hence, the matrix

S=

r+`b −(b−d(r+`b)) s−a` a+d(s−a`)

has determinant 1. In order for it to be inΓ0(2,N), we needb−d(r+`b)=mNfor some m∈Z. To guarantee this, we choosed =gcd(b,N). SinceNis squarefree, we see that gcd(b,N/d)=1, so that there are integers`,mwithb`+mN/d =b/d−r. With this choice of`, we see thatS ∈Γ0(2,N).

Form the matrixTby replacing the(1,1),(1,k+1),(k+1,1)and(k+1,k+1)entries ofInby the(1,1),(1,2),(2,1), and(2,2)entries ofS. ThenTis clearly inΓ0(n,N). Thus, the row space ofMisΓ0(n,N)-equivalent to the row space of

M0T = 1 0tk−1 d 0 · · · 0 0k−1 Ik−1 0k−1 0k−1 · · · 0k1

.

Hence, everyΓ0(n,N)-orbit of ak-dimensional subspace ofQncontains a subspace of the proper form.

SupposeS∈S0±(n,N)takes a subspace in theΓ0(n,N)-orbit corresponding tod|N, to a subspace in the orbit corresponding tod0|N. Then, after multiplyingSby an appropriate element ofΓ0(n,N)so that it takes the representative subspace of the orbit corresponding todto the representative corresponding tod0, for somex∈Z, we must have

(1,0tk−1,d,0tn−k−1)S=(x,∗, . . . ,∗,xd0,0tn−k−1).

If we now denote the(1,1),(1,k+1),(k+1,1)and(k+1,k+1)entries ofSbya,bN,r, ands, respectively, and note that gcd(a,N)=1, we see that we must havea+r d=xand bN+sd=d0x. Hence,bN+sd=d0a+r dd0, and we see thatd|d0a, so thatd|d0. Now using that det(S) ·S1=S0 ∈S0±(n,N), replacingS byS0, and reversing the roles ofd andd0, we must similarly haved0|d. Hence,d=d0.

Now, letW0k be the row space of thek×nmatrix M0 =

Ik 0

.

Letgdbe equal to then×nidentity matrixIn, with the(1,k+1)entry replaced byd. Let P0kbe the stabilizer (in GL(n,Q), acting on the right) ofW0k. DefinePkd=g1

d P0gd; it is the stabilizer of the row spaceWdkofM0gd, or in other words the stabilizer of the canonical representative of theΓ0(n,N)-orbit ofk-dimensional subspaces ofQncorresponding to the divisordofN. Typically, whenkis understood, we will omit it, writingP0,Pd, orWd

rather thanPk0,Pkd, orWdk. We will call a subgroupPdarepresentative maximal parabolic subgroup, and denote its unipotent radical byUdand its Levi quotient byLd =Pd/Ud. Note thatUd=gd1U0gd, whereU0is the unipotent radical ofP0.

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The subgroupP0consists of block matrices A 0 B C

in which Ais an invertiblek×kmatrix,Cis an invertible(n−k) × (n−k)matrix,B is an arbitrary(n−k) ×k matrix, and the block of zeroes isk× (n−k). For a block matrix g ∈ P0 as above, we define ψ01(g) = Aand ψ02(g) = C. One sees easily that ψ10 :P0 →GL(k,Q)andψ02:P0 →GL(n−k,Q)are group homomorphisms.

Fors∈Pd, defineψdi(s)=ψ0i(gdsgd1).

We have the following straightforward generalization of [3, Theorem 7].

Theorem 5.2. Letdbe a positive divisor ofNand assume that(d,N/d)=1. (1) Ifs∈Pd∩S0(n,N)±, thenψ1

d(s)11≡s11 (modd)andψ2

d(s)11≡s11 (modN/d).

(2) ψd1(Pd∩S0(n,N)±) ⊂S0(k,d)±. (3) ψd2(Pd∩S0(n,N)±) ⊂S0(n−k,N/d)±. (4) There is an exact sequence of groups

1→Ud∩Γ0±(n,N) →Pd∩Γ0±(n,N)ψ

d1×ψ2d

−→ Γ0±(k,d) ×Γ0±(n−k,N/d) →1. Proof. Statements (1), (2), and (3) are proven as in [3, Theorem 7].

The only question in the exactness of the sequence in (4) is whether ψd1 ×ψd2 is surjective. To show this surjectivity, suppose that A=(ai j) ∈Γ0±(k,d)andB=(bi j) ∈ Γ±0(n−k,N/d), chooseq,r∈Zsuch thatq(N/d)+r(d)=a11−b11(which can be done since gcd(d,N/d)=1), and letZ be the block matrix

Z = A 0

C B

, whereC=(ci j)has

ci j =







0 ifi>1,

a1j/d ifi=1 and j>1, r ifi=j=1.

We note that sinceA∈Γ±0(k,d), each of these entries is an integer. One checks easily that gd1Zgd ∈Γ0±(n,N) ∩Pd, and that(ψd1×ψd2)(g1

d Zgd)=(A,B).

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6. A spectral sequence

Definition 6.1. LetV be ann-dimensional vector space over a fieldKwithn>0. For 0 ≤i ≤n, letCibe the set of all subspaces ofVof dimensioni.

Definition 6.2. LetV be ann-dimensional vector space over a fieldKwithn>0. For

−1≤i≤n−1 define

Xi = Ê

W∈Ci+1

St(W).

We note that Theorem 4.2 yields an exact sequence of GL(n,K)-modules,

0→ Xn−1→ Xn−2→ · · · →X0→Z→0, (6.1) sinceX1Z.

LetK =Qand letFbe a field of characteristicp>n+1. Let(Γ,S)=(Γ0(n,N),S0(n,N)), and letMbe an admissible rightS-module overF. We apply the spectral sequence of [5, Section 8], to the exact sequence (6.1) to obtain

Eq,r1 =Hr(Γ,Xq⊗M)=⇒Hq+r(Γ,M).

As in [5] this spectral sequence is equivariant for the action of the Hecke operators. For eachqwith 0≤q≤n−1, we choose a set ˆCq+1ofΓ-orbit representatives ofCq+1. For a W ∈Cˆq+1, letΓW be the stabilizer ofW inΓ. Then we may decompose

Xq ⊗M= Ê

WCˆq+1

IndΓΓWSt(W) ⊗M into a finite direct sum of induced modules.

Now, by the Shapiro isomorphism, we obtain E1q,r

Ê

WCˆq+1

HrW,St(W) ⊗M).

Forq < n−1, we note that ˆCq+1 consists exactly of the subspacesWdq, asd runs through the divisors ofN. In addition,ΓW =Γ∩Pd, which we will denote byΓPd. For q=n−1, we have that ˆCq+1k =V. Hence, the first page of the spectral sequence has the following terms.

Eq,r1 =







Hr(Γ,St(V) ⊗M) ifq=n−1, Ê

d|N

HrPq+1 d

,St(Wdq+1) ⊗M) ifq<n−1.

The remainder of the paper is devoted to studying the terms of this spectral sequence, in order to show that for reducible Galois representationsρ=ρ1⊕ρ2satisfying certain conditions, ρfitsE1q,r, and that the eigenvector withρattached either survives to the

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infinity page of the spectral sequence, showing thatρfitsHq+r(Γ,M), or is killed off in such a way as to show thatρnevertheless fitsHs(Γ,M)for some value ofs.

In order to proceed with this argument, it is necessary to show that the terms of the spectral sequence are finite-dimensional vector spaces overF. For the terms withq=n−1, this follows immediately from Borel–Serre duality. Forq<n−1, we prove the following theorem.

Theorem 6.3. Let0<k<n. LetΓ=Γ0(n,N), and assume thatp>n+1. LetP=Pdk for somed|N, letW =Wdk, and letM be a finite-dimensionalΓP-module. Then forr ≥0, the homology

HrP,St(W) ⊗M) is a finite dimensional vector space overF.

Proof. For convenience, we will write kerψd1for kerψd1∩ΓPin this proof. We use the Hochschild–Serre spectral sequence for the exact sequence

1→kerψ1d→ΓP→ΓP/kerψd1 →1. This gives us a spectral sequence

Ei j2 =HiP/kerψ1d,Hj(kerψd1,St(W) ⊗M)) =⇒ Hi+jP,St(W) ⊗M), and if each term of the E2 page is finite dimensional, the abutment must be finite dimensional. Now kerψ1

dacts trivially on St(W), so a termEi j2 may be written as HiP/kerψd1,St(W) ⊗Hj(kerψd1,M)).

We now note that Theorem 5.2(4) implies thatΓP/kerψd1 ψ1dP) = Γ0±(k,d), so, noting that conjugation bygdtakes the action ofΓPonW to an action ofψd1P)onW0, we have that (as a vector space),Ei j2 is isomorphic to

Hi0±(k,d),St(W0) ⊗Hj(kerψd1,M)),

where the action ofγ∈Γ0±(k,d)onHj(kerψ1d,M)is obtained by choosing anyγ0∈ΓP withψ1d0)=γand allowingγ0to act onHj(kerψ1d,M). By Borel–Serre duality,Ei j2 is then isomorphic to

Hi±0(k,d),Hj(kerψd1,M)),

which is finite dimensional since kerψ1d is an arithmetic group and M is finite

dimensional.

We also have the following related theorem.

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Theorem 6.4. Let0<k<n. LetΓ=Γ0(n,N), and assume thatp>n+1. LetP=Pdk for somed|N, letW =Wdk, and letMbe a finite-dimensionalΓLPU-module. Then forr ≥0, the homology

HrL,St(W) ⊗M) is a finite dimensional vector space overF.

Proof. Sinceψ1d is trivial onΓU, it yields a well defined function onΓL. The proof is

then basically the same as the proof of Theorem 6.3.

Remark 6.5. If(Γ,S)=(Γ0(n,N),S0(n,N)), and ifPis a representative maximal parabolic subgroup stabilizing a subspaceW, then the results of [5, Section 3] show that as long as(∗)given anys∈Swe can choose left coset representativessα forΓsΓto be inSP, there is an isomorphism H (Γ,S) H (ΓP,SP)and we can viewHrP,St(W) ⊗M) as anH (Γ,S)-module via this isomorphism. Hence, under condition(∗), in studying systems ofH (Γ,S)-eigenvalues inHrP,St(W) ⊗M)we may study the homology as an H (ΓP,SP)-module. In Theorem 8.6, we show that condition(∗)holds.

7. Two cases of Hecke equivariance of the Hochschild–Serre spectral se- quence

From this section on, we require definitions of additional subsets of GL(n,Q).

Definition 7.1. LetP=Pkdbe a representative maximal parabolic subgroup of GL(n,Q) for some d|N and let p be a prime in Z. We define the following subgroups and subsemigroups of GL(n,Q).

(1) Γ(N)={A∈GL(n,Z): A≡I (modN)}.

(2) Sk(N)is the set of matrices A ∈ GL(n,Q) with integer entries and positive determinant prime topN such that A≡ diag(1, . . . ,1,∗,1, . . . ,1,∗) (modN), with the∗’s in thekandnpositions.

(3) ΓP(N)=Γ(N) ∩P.

(4) SP(N)={s∈Sk(N) ∩P:ψ1d(s), ψ2d(s)both have positive determinant}. We now prove two results involving the Hecke equivariance of the Hochschild–Serre spectral sequence. The first of these results (Theorem 7.11) is closely related to Section 4 of [7]; however, the results here are more general. The second (Theorem 7.15) is similar to [1, Theorem 3.1].

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Definition 7.2. Let Pbe a maximal parabolic subgroup of GL(n,Q)and letUbe the unipotent radical of P. We note thatU(Q)is an abelian group, and we set r equal to the Q-dimension ofU. Let(Γ,S)be a congruence Hecke pair of levelpN (see [1, Definition 1.2]. ThenΓUis a free abelian group of rankr. LetMbe a(p,N)-admissible S-module.

LetTbe the set of matricest∈GL(n,Q)with determinant prime topNsuch that all denominators of bothtandt1are prime topN andtnormalizesU(Q). LetCbe the standard resolution (also known as the bar resolution) ofZover GL(n,Q). Fort∈T, we define an action oftonCΓU M by setting

(c⊗m) ·t= 1 dr

Õ

b

cubt⊗mubt,

whered is any integer prime topsuch that the right conjugation action oftonΓUd is contained inΓU, and{ub : 1≤b≤dr}is a set of coset representatives forΓd

U insideΓU. We can taked=det(t), so there is adthat fits the conditions of the definition (note that the condition thatdbe prime topwas inadvertently omitted in [7]). In [7, Lemma 4.3], this action oftis shown to be well defined; in particular, it does not depend on the choice ofdor on the choice of coset representatives. It also commutes with the boundary operator.

This action of individual elements ofTdoes not normally extend to a group action ofTon CΓUM. However, we now show that the action does, in fact, define a semigroup action ofSP ⊆T onHU,M)under certain hypotheses, makingHU,M)anSP-module.

We note also that an element ofT actually has entries inZ(p)(the localization ofZat the prime ideal(p)), so there is a well defined notion of reduction modulopfor such an element.

The proof of the following lemma is clear.

Lemma 7.3. Fixtanddas in Definition 7.2. Then the largest subgroupHofΓUsuch thatt1Ht⊂ΓUis

H=ΓU∩tΓUt1,

and we haveΓUd ⊆H ⊆ΓU. Hence,U :H]|dr, and is thus prime top(since we may taked=det(t).

By [24, p. 51], we note that if we writeΓUUet

j=1αjΓU, then we haveet=[ΓU: H]. There is a natural action of double cosets on homology and cohomology; when we consider the double cosetΓUUas a Hecke operator, we will denote it by[ΓUU]. Since CΓU M = H0U,CZM), the Hecke operator[ΓUU]acts onCΓU M. This

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action is given by

c⊗m[ΓUU]=

et

Õ

j=1

j⊗mαj.

Lemma 7.4. Lett∈T. Then with the notation defined above, the action oftonC⊗M given in Definition 7.2 is equal to the action of e1

tUU].

Proof. The action of the Hecke operator[ΓUU]is independent of the choice of coset representatives{αj}. We choose theαjas follows: fix a collection of coset representatives {wj: j=1, . . . ,et}ofHinsideΓU, so thatΓUet

j=1wjH. Setαj =wjt. One checks easily that theαjthus defined give distinct cosets ofΓU insideΓUU; since there areet of them, they are a complete set of coset representatives.

Now choose a collection{vk : k =1, . . . ,[H :ΓUd]}of coset representatives ofΓUd insideH, so thatH=Ý

kvkΓUd. Then the set{wjvk}is a complete collection of coset representatives ofΓd

U insideΓU. Since the action oft is independent of the choice of coset representatives, we may choose {ub} = {wjvk}. SinceΓU is abelian, we have wjvk =vkwj. We then obtain

(c⊗m) ·t= 1 dn

dn

Õ

b=1

cubt⊗mubt

= 1 dn

Õ

j,k

cvkwjt⊗mvkwjt

= 1 dn

Õ

j,k

cvkαj ⊗mvkαj

= 1 dn

Õ

k

cvk ⊗mvk

!

UU]

= 1 dn

Õ

k

c⊗m

!

UU]

= [H:Γd

U] [ΓUd

U](c⊗m)[ΓUU]

= 1

et(c⊗m)[ΓUU],

where thevk vanish in the sixth line becausevk ∈ ΓU and the tensor product is over

ΓU.

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LetT0be any subgroup ofTsuch that every element ofT0∩U(Q)is congruent modulo pto an element ofΓU. See Theorem 7.10 for examples whereT0may be taken to be the group generated by a semigroupSP. We will show that for any such subgroupT0, the individual actions of elements ofT0onHkU,M)compile together into a group action.

To do this, we need to show that the composition of the actions ofs,t ∈T0is equal to the action ofst. We will see that this can be done on the level of the homology groups HkU,M), but not on the level of chainsCΓU M. Our first step is the following lemma, from [24, p. 51] (since we are working with right modules, we have changed right cosets to left cosets).

Lemma 7.5. Lets,t ∈T, and suppose thatΓUU

isiΓU andΓUU

jtjΓU. We may choose a finite setΞ⊂T such that

ΓUUU

ξ∈Ξ

ΓUξΓU.

Then in the Hecke algebra we have the equalityUU][ΓUU]=Õ

ξ∈Ξ

m(ξ)[ΓUξΓU],

wherem(ξ)=|{(i,j)|sitjΓU =ξΓU}|.

Lemma 7.6. With notation as in Lemma 7.5, for eachξ ∈Ξ, we haveξ =stu(ξ)for someu(ξ) ∈U(Q), and

ΓUξΓUUstΓUu(ξ).

In addition,

UstΓU][ΓUu(ξ)ΓU]=[ΓUξΓU], andest=eξ.

Proof. SinceTnormalizesU(Q), andU(Q)is abelian, this is immediate.

Lemma 7.7. Letu∈T∩U(Q), and assume that there is someu0∈ΓU that is congruent toumodulopN. LetM be a(p,N)-admissibleT-module. ThenUU]acts trivially on the homology groups

HU,M).

Proof. There is only one single coset in the double cosetΓUU, so the Hecke operator [ΓUU]acts on the homology asudoes.

Since u centralizes ΓU, it acts on the homology via its action on M. Since M is (p,N)-admissible the action ofu0and the action ofuon M are the same. Hence, the action ofuand the action ofu0on the homology are the same. However,u0acts trivially

on the homology, by [14, Proposition III.8.1].

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Remark 7.8. We note that this lemma fails if we apply it on the chain level. This is because the chains,C⊗ΓU M =H0U,C⊗ZM), although acted on by the Hecke operators, are the homology with coefficients inC⊗M, which is not an admissible coefficient module.

Corollary 7.9. LetT0be any subgroup ofT such that every element ofT0∩U(Q)is congruent modulopto an element ofΓU. Lets,t ∈T0. Then, with notation as in Lemma 7.5, we have, forz∈HU,M),

z[ΓUU][ΓUU]=z Õ

ξ∈Ξ

m(ξ)

!

UstΓU].

Also,

z 1

esetUU][ΓUU]=z 1

estUstΓU],

and we see that the action of individual elements ofT0onHU,M)in Definition 7.2 yields a group action ofT0given byz·s=ze1

sUU].

Proof. The first displayed equation follows immediately from Lemmas 7.6 and 7.7. For the second, by [24, Proposition 3.3], Lemma 7.5, and Lemma 7.6, we have

est

Õ

ξ∈Ξ

m(ξ)=Õ

ξ∈Ξ

eξm(ξ)=deg([ΓUU][ΓUU])

=deg([ΓUU])deg([ΓUU])=eset. Hence, by Lemma 7.4 and the above equation,

(z·s) ·t=z 1

esetUU][ΓUU]=z Ím(ξ)

esetUstΓU]=z 1

estUstΓU]=z· (st).

Theorem 7.10. LetP=Pdkfor somed|Nand somek. Let(Γ,S)be either(Γ(pN),Sk(pN)) or0(n,N),S0(n,N)). Letz∈HU,M), and lets,t∈SP. Then the action of individual elements of SPonHU,M)in Definition 7.2 yields a semigroup action ofSPunder whichSU acts trivially.

Proof. By the previous lemmas, we are finished if we can show thatSPlies in a subgroup T0such that every element ofT0∩U(Q)is congruent modulopto an element ofΓU. It suffices to show that every element ofSP1SP∩U(Q)is congruent modulopto an element ofΓU.

For (Γ,S) =(Γ0(n,N),S0(n,N)) one checks that the intersectionSP1SP∩U(Q)is contained in the set of matrices

M=

gd1

Ik 0 A In−k

gd

,

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