Generic vanishing theory via mixed Hodge modules

Mihnea Popa, Christian Schnell

A. Introduction

The attempt to understand cohomology vanishing statements on irregular varieties in the absence of strong positivity has led to what is usually called generic vanishing theory. Perhaps the most famous result is the generic vanishing theorem of Green and Lazarsfeld [GL1], which in a weak form states that on a smooth complex projective variety XX, the cohomology of a generic line bundle L∈Pic⁡0(X)L\in\operatorname{Pic}^{0}(X) vanishes in degrees less than dim⁡a(X)\dim a(X), where a ⁣:X→Alb⁡(X)a\colon X\to\operatorname{Alb}(X) denotes the Albanese mapping of XX. This theorem and its variants have found a surprising number of applications, ranging from results about singularities of theta divisors [EL] to recent work on the birational geometry of irregular varieties, including a proof of Ueno’s conjecture [ChH].

One can consider the set of those line bundles for which the cohomology in a given degree does not vanish, and thanks to the work of many people, the structure of these sets is very well understood. This is more precisely the content of generic vanishing theory. Denoting, for any coherent sheaf F\mathcal{F} on XX, by

the ii-th cohomological support locus of F\mathcal{F}, its main statements are the following:

One has codim Vi(ωX)≥i−dim⁡X+dim⁡a(X){\rm codim}~{}V^{i}(\omega_{X})\geq i-\dim X+\dim a(X) for all ii [GL1, GL2]. This implies the generic vanishing theorem via Serre duality.

The irreducible components of each Vi(ωX)V^{i}(\omega_{X}) are torsion translates of abelian subvarieties of Pic⁡0(X)\operatorname{Pic}^{0}(X) [GL2, Arapura, Simpson2].

If p2:X×Pic⁡0(X)→Pic⁡0(X)p_{2}:X\times\operatorname{Pic}^{0}(X)\rightarrow\operatorname{Pic}^{0}(X) is the second projection, and PP is a Poincaré line bundle on X×Pic⁡0(X)X\times\operatorname{Pic}^{0}(X), then Rp2∗P\mathbf{R}{p_{2}}_{*}P is locally around each point quasi-isomorphic to a linear complex [GL2]. A precise version of this result is known to imply (L), except for the torsion statement, and based on this also (D).

Analogous results have been considered for the cohomology of local systems, replacing Pic⁡0(X)\operatorname{Pic}^{0}(X) by Char(X){\rm Char}(X), the algebraic group parametrizing rank one local systems [Arapura, Simpson, Simpson2]. New approaches and extensions for the theory on Pic⁡0(X)\operatorname{Pic}^{0}(X) have been introduced more recently, for example in [CH, Hacon, PP]. On the other hand, important gaps have remained in our understanding of some of the most basic objects. For instance, while (L) is also known for the sheaf of holomorphic pp-forms ΩXp\Omega_{X}^{p} with p<np<n, a good generic Nakano-type vanishing statement as in (D) has eluded previous efforts, despite several partial results [GL1, PP]. The same applies to the case of local systems of rank one, where the perhaps the even more interesting property (SL) has been missing as well.

In this paper, we answer those remaining questions, and at the same time recover the previous results of generic vanishing theory mentioned above (with the exception of the statement about torsion points, which is of a different nature) by enlarging the scope of the study to the class of filtered D\mathscr{D}-modules associated to mixed Hodge modules on abelian varieties. In fact, there is a version of the Fourier-Mukai transform for D\mathscr{D}-modules, introduced by Laumon [Laumon2] and Rothstein [Rothstein]; it takes D\mathscr{D}-modules on an abelian variety to complexes of coherent sheaves on A♮A^{\natural}, the moduli space of line bundles on AA with integrable connection. Our main results can be summarized briefly as describing the Fourier-Mukai transform of the trivial D\mathscr{D}-module OX\mathscr{O}_{X} on an irregular variety XX.

Why mixed Hodge modules?

To motivate the introduction of mixed Hodge modules into the problem, let us briefly recall the very elegant proof of the generic vanishing theorem for ωX\omega_{X} discovered by Hacon [Hacon]. It goes as follows.

in the same range. Now the sheaves Ria∗ωXR^{i}a_{\ast}\omega_{X} still satisfy a Kodaira-type vanishing theorem, and together with the special geometry of abelian varieties this implies after some work that the Fourier-Mukai transform of Ria∗ωXR^{i}a_{\ast}\omega_{X} is the dual of a coherent sheaf Fi\mathscr{F}_{i} on A^\widehat{A}, which is to say that

The desired inequality for the codimension of the support becomes

which is now a consequence of a general theorem about regular local rings. This proves the dimension statement (D), and hence the generic vanishing theorem for topologically trivial line bundles.

One of the subjects of this paper is to use this framework in order to prove a generic vanishing theorem for general objects of Hodge-theoretic origin. The role of Kollár’s theorem is played by the decomposition theorem [BBD], or more precisely by its Hodge-theoretic version due to Morihiko Saito [Saito-MHM]. This is one main reason why mixed Hodge modules form a natural setting here. Another is the existence of a very general Kodaira-type vanishing theorem for mixed Hodge modules, again due to Saito, which becomes particularly useful on abelian varieties. This vanishing theorem allows us to generalize the second half of the proof above to any coherent sheaf of Hodge-theoretic origin on an abelian variety. Finally, in order to extract the relevant information about the sheaves ΩXp\Omega_{X}^{p} with p<dim⁡Xp<\dim X, one needs a result by Laumon and Saito on the behavior of filtered D\mathscr{D}-modules under direct images, which only works well in the case of D\mathscr{D}-modules that underlie mixed Hodge modules.

The main results

Let us now give a summary of the results we obtain. There are essentially two parts: vanishing and dimension results, for which Hodge modules are crucially needed, and linearity results, which apply to certain Hodge modules, but for which the general theory of D\mathscr{D}-modules and the harmonic theory of flat line bundles suffice in the proofs. The theory of mixed Hodge modules is reviewed in §5 below.

The starting point is a general Kodaira-type vanishing theorem for the graded pieces of the de Rham complex of a mixed Hodge module, proved by Saito. On an abelian variety AA, this can be improved to a vanishing theorem for coherent sheaves of the form gr⁡kFM\operatorname{gr}_{k}^{F}\mathcal{M}, where (M,F)(\mathcal{M},F) is any filtered D\mathscr{D}-module underlying a mixed Hodge module on AA (see Lemma 9.1 below). We use this observation to produce natural classes of perverse coherent sheaves [AB, Kashiwara] on the dual abelian variety A^\widehat{A}, and on the parameter space for Higgs line bundles A^×H0(A,ΩA1)\widehat{A}\times H^{0}(A,\Omega_{A}^{1}).

We first show that every mixed Hodge module on AA gives rise to a collection of sheaves satisfying the generic vanishing condition, or equivalently perverse coherent sheaves on A^\widehat{A} with respect to the dual standard tt-structure (reviewed in §7).

Consequently, its Fourier-Mukai transform RΦP(gr⁡kFM)\mathbf{R}\Phi_{P}(\operatorname{gr}_{k}^{F}\mathcal{M}) is a perverse coherent sheaf on A^\widehat{A}.

This uses Hacon’s general strategy, as in §2 above, and the correspondence established in [Popa, PP] between objects satisfying generic vanishing (or GV⁡\operatorname{GV}-objects) and perverse coherent sheaves in the above sense.

In order to obtain a generic Nakano-type vanishing statement similar to (D), or statements for cohomological support loci of rank one local systems, we apply Theorem 3.1 to the direct image of the trivial Hodge module on an irregular variety under the Albanese map. Here our main tools are the decomposition theorem for Hodge modules [Saito-HM], extending the well-known result of [BBD], and a formula due to Laumon [Laumon] for the behavior of the associated graded objects under projective direct images (which is true for mixed Hodge modules).

Our main results in this direction are the following. Let XX be a smooth complex projective variety of dimension nn, with nonzero irregularity g=h1(X,OX)g=h^{1}(X,\mathscr{O}_{X}). Let a ⁣:X→A=Alb⁡(X)a\colon X\to A=\operatorname{Alb}(X) be the Albanese map of XX. Consider the defect of semismallness of the Albanese map a ⁣:X→Aa\colon X\to A, which is defined by the formula

Let XX be a smooth complex projective variety of dimension nn. Then

Suppose that the Albanese map of XX is semismall. Then

Unlike in the case of ωX\omega_{X}, it is not sufficient to assume that the Albanese map is generically finite over its image; this was already pointed out in [GL1]. Nevertheless, our method also recovers the stronger statement for ωX\omega_{X} [GL1] and its higher direct images [Hacon] (see the end of §10). This is due to the special properties of the first non-zero piece of the Hodge filtration on mixed Hodge modules, established by Saito. Note also that, since χ(ΩXp)=χ(ΩXp⊗L)\chi(\Omega_{X}^{p})=\chi(\Omega_{X}^{p}\otimes L) for any L∈Pic⁡0(X)L\in\operatorname{Pic}^{0}(X) by the deformation invariance of the Euler characteristic of a coherent sheaf, we have as a consequence the following extension of the fact that χ(ωX)≥0\chi(\omega_{X})\geq 0 for varieties of maximal Albanese dimension.

If the Albanese map of XX is semismall, then (−1)n−pχ(ΩXp)≥0(-1)^{n-p}\chi(\Omega_{X}^{p})\geq 0.

Let XX be a smooth complex projective variety of dimension nn. Then

To deduce this from the arguments leading to Theorem 3.2, we need to appeal to the structure results and the relationship with the space of Higgs bundles, proved by Simpson [Simpson, Simpson2] and Arapura [Arapura]; see §12.

While editing this paper, we learned of the very interesting preprint [KW] by T. Krämer and R. Weissauer, who prove vanishing theorems for perverse sheaves on abelian varieties. They also obtain a generic vanishing theorem for ΩXp\Omega_{X}^{p} and for rank one local systems, involving the same quantity δ(a)\delta(a) as in Theorem 3.2, but without precise codimension bounds for the cohomological support loci. Their methods are very different from ours.

Three additional theorems complete the picture, by describing in detail the Fourier-Mukai transform of the trivial D\mathscr{D}-module OX\mathscr{O}_{X}; they include results of type (D), (L) and (SL) on the space of line bundles with integrable connection on XX. Here it is important to consider two different kinds of Fourier-Mukai transforms, corresponding in Simpson’s terminology [Simpson2] to the Dolbeault realization (via Higgs bundles) and the de Rham realization (via line bundles with integrable connection) of Char(X){\rm Char}(X).

where S=Sym⁡V∗S=\operatorname{Sym}V^{\ast}, and the complex in brackets is placed in degrees −n,…,0-n,\dotsc,0, with differential induced by the evaluation morphism OX⊗V→ΩX1\mathscr{O}_{X}\otimes V\to\Omega_{X}^{1}. Since this is a complex of finitely generated graded modules over Sym TA{\rm Sym}~{}\mathscr{T}_{A}, it naturally corresponds to a complex of coherent sheaves on cotangent bundle T∗A=A×VT^{*}A=A\times V, namely

Let a ⁣:X→Aa\colon X\to A be the Albanese map of a smooth complex projective variety of dimension nn, and let p1 ⁣:X×V→Xp_{1}\colon X\times V\to X be the first projection.

where each Ci,j\mathscr{C}_{i,j} is a Cohen-Macaulay sheaf of dimension dim⁡A\dim A.

The support of each RΦPCi,j\mathbf{R}\Phi_{P}\mathscr{C}_{i,j} is a finite union of torsion translates of triple tori in A^×V\widehat{A}\times V, subject to the inequalities

The dual objects \mathbf{R}\mathcal{H}\mathit{om}\bigl{(}\mathbf{R}\Phi_{P}\mathscr{C}_{i,j},\mathscr{O}_{\widehat{A}\times V}\bigr{)} also satisfy (ii).

The second and third theorems are best stated in terms of the generalized Fourier-Mukai transform for D\mathscr{D}-modules on abelian varieties, introduced by Laumon [Laumon2] and Rothstein [Rothstein]. Their work gives an equivalence of categories

We review the construction, both algebraically and analytically, in §17 below. This Fourier-Mukai transform is the right context for a strong linearity result (SL) for the D\mathscr{D}-module OX\mathscr{O}_{X}, extending the result for topologically trivial line bundles in [GL2].

placed in degrees −n,…,n-n,\dotsc,n, with differential given by the formula

As discussed in §23, every direct summand of a linear complex (in the derived category) is again quasi-isomorphic to a linear complex. It follows that all direct summands of RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} coming from the decomposition

have the same linearity property (see Corollary 17.3). Note also that using base change for local systems and the description of tangent cones to cohomological support loci as in [Libgober], via arguments as in[GL2]*§4 (which we will not repeat here), Theorem 3.7 gives another proof of the linearity to the cohomological support loci Σk(X)\Sigma^{k}(X), i.e. for the statement of type (L).

Our proof of Theorem 3.7 relies on the harmonic theory for flat line bundles developed by Simpson [Simpson]. As in [GL2], the idea is that after pulling the complex RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} back to the universal covering space of A♮A^{\natural}, one can use harmonic forms to construct a linear complex that is quasi-isomorphic to the pullback in a neighborhood of a given point. Additional technical difficulties arise however from the fact that the wedge product of two harmonic forms is typically no longer harmonic (which was true in the special case of (0,q)(0,q)-forms needed in [GL2], and led to a natural quasi-isomorphism in that case). The new insight in this part of the paper is that a quasi-isomorphism can still be constructed by more involved analytic methods.

Thirdly, using Theorem 3.5, we are able to derive the following generic vanishing-type property of the Laumon-Rothstein transform of the D\mathscr{D}-module OX\mathscr{O}_{X}.

For any smooth projective complex variety XX we have

This is best expressed in terms of the new tt-structure alluded to above; see the equivalent formulation in Theorem 24.1. In particular, in the special case when the Albanese map is semismall, it follows that RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} is a perverse coherent sheaf. Via formal algebraic properties of this tt-structure, we deduce the following vanishing statement for the higher direct images RiΦP♮OXR^{i}\Phi_{P^{\natural}}\mathscr{O}_{X}. It is the analogue of the corresponding statement for the standard Fourier-Mukai transform of OX\mathscr{O}_{X} conjectured by Green and Lazarsfeld, and proved by Hacon [Hacon] (and in the Kähler setting in [PP2]).

For any smooth projective complex variety XX we have

Along the lines of [LP], Theorem 3.7 and Corollary 3.9 can be combined to give, by means of the BGG correspondence, a bound on the complexity of the cohomology algebra

Let XX be a smooth projective complex variety of dimension nn. Then EE is \bigl{(}n+\delta(a)\bigr{)}-regular as a graded EE-module.

Concretely, this means that PXP_{X} is generated in degrees −δ(a),…,n-\delta(a),\dotsc,n; the relations among the generators appear in degrees −δ(a)−1,…,n−1-\delta(a)-1,\dotsc,n-1; and more generally, the pp-th module of syzygies of PXP_{X} has all its generators in degrees −δ(a)−p,…,n−p-\delta(a)-p,\dotsc,n-p. Simple examples show that this result is optimal; see §25.

The last part of the paper contains a few statements extending our results to more general classes of D\mathscr{D}-modules on abelian varieties, not necessarily underlying mixed Hodge modules. The proofs are of a different nature, and will be presented elsewhere. We propose a few natural open problems as well.

Acknowledgements

We are grateful to Mark de Cataldo for pointing out the current statement of Proposition 11.2, which is a strengthening of our original result. We thank Donu Arapura, Takuro Mochizuki and Keiji Oguiso for useful conversations. M.P. is partially supported by NSF grant DMS-1101323. C.S. is partially supported by the World Premier International Research Center Initiative (WPI Initiative), MEXT, Japan, and by NSF grant DMS-1100606.

B. Preliminaries

In this section, we recall a few aspects of Morihiko Saito’s theory of mixed Hodge modules [Saito-MHM] which, as explained in the introduction, offers a convenient setting for the results of this paper. A very good survey can also be found in [Saito-survey]. We only discuss the case of a complex algebraic variety XX, say of dimension nn.

is the analogue for Hodge modules of the decomposition theorem of [BBD]. The proof of this result with methods from algebraic analysis and D\mathscr{D}-modules is one of the main achievements of Saito’s theory.

A regular holonomic DX\mathscr{D}_{X}-module M\mathcal{M}, together with a good filtration F∙MF_{\bullet}\mathcal{M} by OX\mathscr{O}_{X}-coherent subsheaves such that gr⁡∙F ⁣M\operatorname{gr}_{\bullet}^{F}\!\mathcal{M} is coherent over gr⁡∙FDX\operatorname{gr}_{\bullet}^{F}\mathscr{D}_{X}. This filtration plays the role of a Hodge filtration on M\mathcal{M}.

These components are subject to several conditions, which are defined by induction on the dimension of the support of M\mathcal{M}. On a one-point space, a mixed Hodge module is a graded-polarizable mixed Hodge structure; in general, Saito’s conditions require that the nearby and vanishing cycles of M\mathcal{M} with respect to any locally defined holomorphic function are again mixed Hodge modules (now on a variety of dimension n−1n-1); the existence of polarizations; etc. An important fact is that these local conditions are preserved after taking direct images, and that they are sufficient to obtain global results such as the decomposition theorem.

Three theorems about mixed Hodge modules

In this section, we recall from the literature three useful theorems about the associated graded object gr⁡∙FM\operatorname{gr}_{\bullet}^{F}\mathcal{M}, for a filtered D\mathscr{D}-module (M,F)(\mathcal{M},F) underlying a mixed Hodge module.

During the discussion, XX will be a smooth complex projective variety of dimension nn, and M∈MHM⁡(X)M\in\operatorname{MHM}(X) a mixed Hodge module on XX. As usual, we denote the underlying filtered D\mathscr{D}-module by (M,F)(\mathcal{M},F). Recall that the associated graded of the sheaf of differential operators DX\mathscr{D}_{X}, with respect to the filtration by order of differential operators, is isomorphic to AX∙=Sym⁡∙TX\mathcal{A}_{X}^{\bullet}=\operatorname{Sym}^{\bullet}\mathscr{T}_{X}, the symmetric algebra of the tangent sheaf of XX. Since gr⁡∙FM\operatorname{gr}_{\bullet}^{F}\mathcal{M} is finitely generated over this sheaf of algebras, it defines a coherent sheaf C(M,F)\mathscr{C}(\mathcal{M},F) on the cotangent bundle T∗XT^{\ast}X. The support of this sheaf is the characteristic variety of the D\mathscr{D}-module M\mathcal{M}, and therefore of pure dimension nn because M\mathcal{M} is holonomic.

The first of the three theorems is Saito’s generalization of the Kodaira vanishing theorem. Before we state it, observe that the filtration F∙MF_{\bullet}\mathcal{M} is compatible with the D\mathscr{D}-module structure on M\mathcal{M}, and therefore induces a filtration on the de Rham complex of M\mathcal{M} by the formula

The associated graded complex for the filtration in (6.1) is

which is now a complex of coherent sheaves of OX\mathscr{O}_{X}-modules in degrees −n,…,0-n,\dotsc,0. This complex satisfies the following Kodaira-type vanishing theorem.

Let (M,F)(\mathcal{M},F) be the filtered D\mathscr{D}-module underlying a mixed Hodge module on a smooth projective variety XX, and let LL be any ample line bundle.

One has \mathbf{H}^{i}\bigl{(}X,\operatorname{gr}_{k}^{F}\operatorname{DR}_{X}(\mathcal{M})\otimes L\bigr{)}=0 for all i>0i>0.

One has \mathbf{H}^{i}\bigl{(}X,\operatorname{gr}_{k}^{F}\operatorname{DR}_{X}(\mathcal{M})\otimes L^{-1}\bigr{)}=0 for all i<0i<0.

The proof works by reducing the assertion to a vanishing theorem for perverse sheaves on affine varieties, with the help of Saito’s formalism. Details can be found in [Saito-MHM]*Proposition 2.33. ∎

The second theorem gives more information about the coherent sheaf C(M,F)\mathscr{C}(\mathcal{M},F) on the cotangent bundle of XX. Before stating it, we recall the definition of the Verdier dual M′=DXMM^{\prime}=\mathbf{D}_{X}M of a mixed Hodge module. If rat⁡M\operatorname{rat}M is the perverse sheaf underlying MM, then rat⁡M′\operatorname{rat}M^{\prime} is simply the usual topological Verdier dual. On the level of D\mathscr{D}-modules, note that since M\mathcal{M} is left D\mathscr{D}-module, the dual complex

is naturally a complex of right D\mathscr{D}-modules; since M\mathcal{M} is holonomic, it is quasi-isomorphic to a single right D\mathscr{D}-module. If M′\mathcal{M}^{\prime} denotes the left D\mathscr{D}-module underlying the Verdier dual M′M^{\prime}, then that right D\mathscr{D}-module is ωX⊗OXM′\omega_{X}\otimes_{\mathscr{O}_{X}}\mathcal{M}^{\prime}. Thus we have

where the right D\mathscr{D}-module structure on ωX⊗M′\omega_{X}\otimes\mathcal{M}^{\prime} is given by the rule ξ⋅(ω⊗m′)=(ξω)⊗m′−ω⊗(ξm′)\xi\cdot(\omega\otimes m^{\prime})=(\xi\omega)\otimes m^{\prime}-\omega\otimes(\xi m^{\prime}) for ξ∈TX\xi\in\mathscr{T}_{X}. The Hodge filtration on M\mathcal{M} induces a filtration on the dual complex and hence on M′\mathcal{M}^{\prime}. The following result shows that this induced filtration is well-behaved, in a way that makes duality and passage to the associated graded compatible with each other.

Let MM be a mixed Hodge module on a smooth complex algebraic variety XX of dimension nn, and let M′M^{\prime} denote its Verdier dual. Then

where sections of Sym⁡kTX\operatorname{Sym}^{k}\mathscr{T}_{X} act with an extra factor of (−1)k(-1)^{k} on the right-hand side. If we consider both sides as coherent sheaves on T∗XT^{\ast}X, we obtain

where p ⁣:T∗X→Xp\colon T^{\ast}X\to X is the projection. In particular, C(M,F)\mathscr{C}(\mathcal{M},F) is always a Cohen-Macaulay sheaf of dimension nn.

That the coherent sheaf C(M,F)\mathscr{C}(\mathcal{M},F) on T∗XT^{\ast}X is Cohen-Macaulay is proved in [Saito-HM]*Lemme 5.1.13. For an explanation of how this fact implies the formula for the dual of the graded module gr⁡∙FM\operatorname{gr}_{\bullet}^{F}\mathcal{M}, see [duality]*§3.1. ∎

The last of the three theorems gives a formula for the associated graded object of f∗Mf_{*}M, where f ⁣:X→Yf\colon X\to Y is a projective morphism between two smooth complex algebraic varieties. The formula itself first appears in a paper by Laumon [Laumon]*Construction 2.3.2, but it is not true in the generality claimed there (that is to say, for arbitrary filtered D\mathscr{D}-modules).

Before stating the precise result, we give an informal version. The following diagram of morphisms, induced by ff, will be used throughout:

Let f ⁣:X→Yf\colon X\to Y be a projective morphism between smooth complex algebraic varieties, and let M∈MHM⁡(X)M\in\operatorname{MHM}(X). Then with notation as above,

This can be easily proved using Saito’s formalism of induced D\mathscr{D}-modules; both the factor of ωX/Y\omega_{X/Y} and the shift in the grading come from the transformation between left and right D\mathscr{D}-modules that is involved. To illustrate what is going on, we shall outline a proof based on factoring ff through its graph. By this device, it suffices to verify the formula in two cases: (1) for a regular closed embedding f ⁣:X↪Yf\colon X\hookrightarrow Y; (2) for a projection f ⁣:Y×Z→Yf\colon Y\times Z\to Y with ZZ smooth and projective.

and so the formula we need to prove is that

By [Saito-HM]*p. 850, we have f∗(M,F)≃M[∂1,…,∂r]f_{\ast}(\mathcal{M},F)\simeq\mathcal{M}[\partial_{1},\dotsc,\partial_{r}], with filtration given by

which is the desired formula. Globally, the factor of det⁡NX∣Y\det N_{X\mid Y} is needed to make the above isomorphism coordinate independent.

Next, consider the case where X=Y×ZX=Y\times Z, with ZZ smooth and projective of dimension rr, and f=p1f=p_{1}. Then ωX/Y≃p2∗ωZ\omega_{X/Y}\simeq p_{2}^{\ast}\omega_{Z}. In this case, we have

where DR⁡Y×Z/Y(M)\operatorname{DR}_{Y\times Z/Y}(\mathcal{M}) is the relative de Rham complex

supported in degrees −r,…,0-r,\dotsc,0. As in (6.1), the Hodge filtration on the D\mathscr{D}-module M\mathcal{M} induces a filtration on the relative de Rham complex by the formula

Now the key point is that since ZZ is smooth and projective, the induced filtration on the direct image complex is strict by [Saito-MHM]*Theorem 2.14. It follows that

On the other hand, a graded locally free resolution of ωZ\omega_{Z} as a graded AZ\mathcal{A}_{Z}-module is given by the complex

again in degrees −r,…,0-r,\dotsc,0. Therefore ωX/Y⊗OXf∗AY\omega_{X/Y}\otimes_{\mathscr{O}_{X}}f^{\ast}\mathcal{A}_{Y} is naturally resolved, as a graded AX\mathcal{A}_{X}-module, by the complex

and so gr⁡∙+rFM⊗AXf∗AY⊗OXωX/Y\operatorname{gr}_{\bullet+r}^{F}\mathcal{M}\otimes_{\mathcal{A}_{X}}f^{\ast}\mathcal{A}_{Y}\otimes_{\mathscr{O}_{X}}\omega_{X/Y} is represented by the complex

from which the desired formula follows immediately. ∎

Perverse coherent sheaves

The following fundamental result is proved in [Kashiwara]*Theorem 5.9 and, based on an idea of Deligne, in [AB]*Theorem 3.10.

which means that the duality functor RHom(−,OX)\mathbf{R}\mathcal{H}\mathit{om}(-,\mathscr{O}_{X}) exchanges the two perverse tt-structures defined by pp and p^\hat{p}. The heart of the tt-structure defined by pp is denoted

and is called the abelian category of pp-perverse coherent sheaves.

The dual object RHom(E,OX)\mathbf{R}\mathcal{H}\mathit{om}(E,\mathscr{O}_{X}) is a coherent sheaf.

It is easily verified that both mm and the dual function

The next lemma follows easily from [Kashiwara]*Lemma 5.5.

The perverse tt-structures defined by mm and m^\hat{m} satisfy

By duality, this also describes the subcategories with ≥k\geq k.

By translation it is enough to prove this for k=0k=0, where the result is obvious from the fact that m(x)≥0m(x)\geq 0. ∎

Integral functors and GV-objects

(2) For any sufficiently ample line bundle LL on YY, and every i>ki>k,

(3) RiΦP∨(ωX⊗E∨)=0R^{i}\Phi_{P^{\vee}}(\omega_{X}\otimes E^{\vee})=0 for all i<n−ki<n-k.

An object EE satisfying the equivalent conditions in the Theorem with k=0k=0, is called a GV⁡\operatorname{GV}-object (with respect to PP); if it is moreover a sheaf, then it is called a GV⁡\operatorname{GV}-sheaf.

C. Mixed Hodge modules and generic vanishing

Let AA be a complex abelian variety of dimension gg, and let M∈MHM⁡(A)M\in\operatorname{MHM}(A) be a mixed Hodge module on AA. As usual, we denote the underlying filtered holonomic D\mathscr{D}-module by (M,F)(\mathcal{M},F). From Theorem 6.2, we know that the associated graded pieces of the de Rham complex DR⁡(M,F)\operatorname{DR}(\mathcal{M},F) satisfy an analogue of Kodaira vanishing. A key observation is that on abelian varieties, the same vanishing theorem holds for the individual coherent sheaves gr⁡kFM\operatorname{gr}_{k}^{F}\mathcal{M}, due to the fact that the cotangent bundle of AA is trivial. As we shall see, this implies that each gr⁡kFM\operatorname{gr}_{k}^{F}\mathcal{M} is a GV⁡\operatorname{GV}-sheaf on AA (and therefore transforms to a perverse coherent sheaf on A^\widehat{A} with respect to the tt-structure given by cc in §7).

supported in degrees −g,…,0-g,\dotsc,0. According to Theorem 6.2, this complex has the property that, for i>0i>0,

Using the fact that ΩA1≃OA⊕g\Omega_{A}^{1}\simeq\mathscr{O}_{A}^{\oplus g}, one can deduce the asserted vanishing theorem for the individual sheaves gr⁡kFM\operatorname{gr}_{k}^{F}\mathcal{M} by induction on kk. Indeed, since gr⁡kFM=0\operatorname{gr}_{k}^{F}\mathcal{M}=0 for k≪0k\ll 0, inductively one has for each kk a distinguished triangle

with EkE_{k} an object satisfying Hi(A,Ek⊗L)=0\mathbf{H}^{i}(A,E_{k}\otimes L)=0. ∎

We now obtain the first theorem of the introduction, by combining Lemma 9.1 with Theorem 8.1 and a trick invented by Mukai. As mentioned above, the method is the same as in Hacon’s proof of the generic vanishing theorem [Hacon, PP].

Let LL be an ample line bundle on A^\widehat{A}. By Theorem 8.1, it suffices to show that

for i>0i>0. Let φL ⁣:A^→A\varphi_{L}\colon\widehat{A}\to A be the isogeny induced by LL. Then, by virtue of φL\varphi_{L} being étale,

is injective, and so we are reduced to proving that the group on the right vanishes whenever i>0i>0.

Let N=φL∗MN=\varphi_{L}^{\ast}M be the pullback of the mixed Hodge module MM to A^\widehat{A}. If (N,F)(\mathcal{N},F) denotes the underlying filtered holonomic D\mathscr{D}-module, then FkN=φL∗FkMF_{k}\mathcal{N}=\varphi_{L}^{\ast}F_{k}\mathcal{M} because φL\varphi_{L} is étale. On the other hand, by [Mukai] 3.11

Going back to the de Rham complex, it is worth recording the complete information one can obtain about gr⁡kFDR⁡A(M)\operatorname{gr}_{k}^{F}\operatorname{DR}_{A}(\mathcal{M}) from Saito’s theorem, since this produces further natural examples of GV⁡\operatorname{GV}-objects on AA. One one hand, just as in the proof of Theorem 3.1, we see that each gr⁡kFDR⁡A(M)\operatorname{gr}_{k}^{F}\operatorname{DR}_{A}(\mathcal{M}) is a GV⁡\operatorname{GV}-object. On the other hand, since gr⁡kFDR⁡A(M)\operatorname{gr}_{k}^{F}\operatorname{DR}_{A}(\mathcal{M}) is supported in non-positive degrees, its transform with respect to the standard Fourier-Mukai functor

given by the normalized Poincaré bundle on A×A^A\times\widehat{A}, could a priori have cohomology in negative degrees. The following proposition shows that this is not the case.

If (M,F)(\mathcal{M},F) underlies a mixed Hodge module on AA, then

By a standard application of Serre vanishing (see [PP]*Lemma 2.5), it suffices to show that for any sufficiently positive ample line bundle LL on A^\widehat{A},

for i<0i<0. Assuming that LL is symmetric, R0ΨP(L)R^{0}\Psi_{P}(L) is easily seen to be the dual of the locally free sheaf RgΨP(L−1)R^{g}\Psi_{P}(L^{-1}), and so arguing as in the proof of Theorem 3.1, we are reduced to proving that

whenever i<0i<0. But since φL∗gr⁡kFDR⁡(M,F)≃gr⁡kFDR⁡(N,F)\varphi_{L}^{\ast}\operatorname{gr}_{k}^{F}\operatorname{DR}(\mathcal{M},F)\simeq\operatorname{gr}_{k}^{F}\operatorname{DR}(\mathcal{N},F), this is an immediate consequence of part (2) of Saito’s vanishing Theorem 6.2. ∎

If (M,F)(\mathcal{M},F) underlies a mixed Hodge module on AA, then

are GV⁡\operatorname{GV}-objects on AA. Therefore the graded pieces of the de Rham complexes associated to such D\mathscr{D}-modules form a class of GV⁡\operatorname{GV}-objects which is closed under Grothendieck duality.

The decomposition theorem for the Albanese map

Let XX be a smooth complex projective variety of dimension nn, let A=Alb⁡(X)A=\operatorname{Alb}(X) be its Albanese variety, and let a ⁣:X→Aa\colon X\to A be the Albanese map (for some choice of base point). As before, we set g=dim⁡Ag=\dim A.

where Mi,jM_{i,j} has strict support equal to some irreducible subvariety Zi,j⊆AZ_{i,j}\subseteq A; the perverse sheaf underlying Mi,jM_{i,j} is the intersection complex of a local system on a Zariski-open subset of Zi,jZ_{i,j}. Note that since aa is projective, we have the Lefschetz isomorphism [Saito-MHM]*Théorème 1

induced by ii-fold cup product with the first Chern class of an ample line bundle. The Tate twist, necessary to change the weight of MiM_{i} from n+in+i to n−in-i, requires some explanation. If (Mi,F)(\mathcal{M}_{i},F) denotes the filtered D\mathscr{D}-module underlying MiM_{i}, then the filtered D\mathscr{D}-module underlying Mi(i)M_{i}(i) is (Mi,F∙−i)(\mathcal{M}_{i},F_{\bullet-i}); thus the above isomorphism means that FkM−i≃Fk−iMiF_{k}\mathcal{M}_{-i}\simeq F_{k-i}\mathcal{M}_{i}.

with differential induced by the evaluation morphism OX⊗H0(X,ΩX1)→ΩX1\mathscr{O}_{X}\otimes H^{0}(X,\Omega_{X}^{1})\to\Omega_{X}^{1}.

The cotangent bundle of AA is isomorphic to the product A×VA\times V, and so using the notation from §6, we have AA=OA⊗S\mathcal{A}_{A}=\mathscr{O}_{A}\otimes S as well as a∗AA=OX⊗Sa^{*}\mathcal{A}_{A}=\mathscr{O}_{X}\otimes S. Consequently, ωX⊗a∗AA\omega_{X}\otimes a^{*}\mathcal{A}_{A} can be resolved by the complex

placed as usual in degrees −n,…,0-n,\dotsc,0. Applying Theorem 6.5, we find that

with Koszul-type differential induced by the morphism OX→ΩX1⊗V∗\mathscr{O}_{X}\to\Omega_{X}^{1}\otimes V^{\ast}, which in turn is induced by the evaluation morphism OX⊗V→ΩX1\mathscr{O}_{X}\otimes V\to\Omega_{X}^{1}. ∎

On the other hand, we know from the discussion above that

It follows that gr⁡∙Fa∗(OX,F)\operatorname{gr}_{\bullet}^{F}a_{*}(\mathscr{O}_{X},F) splits, as a complex of graded modules over AA=OA⊗S\mathcal{A}_{A}=\mathscr{O}_{A}\otimes S, into a direct sum of modules of the form gr⁡∙FMi,j\operatorname{gr}_{\bullet}^{F}\mathcal{M}_{i,j}. Putting everything together, we obtain a key isomorphism which relates generic vanishing, zero sets of holomorphic one-forms on XX, and the topology of the Albanese mapping.

in the bounded derived category of graded OA⊗S\mathscr{O}_{A}\otimes S-modules.

Since the Mi,jM_{i,j} are Hodge modules on an abelian variety, it follows from Theorem 3.1 that each gr⁡kFMi,j\operatorname{gr}_{k}^{F}\mathcal{M}_{i,j} is a GV⁡\operatorname{GV}-sheaf on AA. The isomorphism in Corollary 10.2 shows that whether or not the entire complex gr⁡kFa∗(OX,F)\operatorname{gr}_{k}^{F}a_{\ast}(\mathscr{O}_{X},F) satisfies a generic vanishing theorem is determined by the presence of nonzero Mi,jM_{i,j} with i>0i>0. We shall see in §12 how this leads to a generic vanishing theorem of Nakano-type.

The defect of semismallness

The defect of semismallness of the map a ⁣:X→Aa\colon X\to A is

is the usual mixed Hodge structure on the cohomology of the projective variety FF. By the above, this mixed Hodge structure is nonzero; it follows for dimension reasons that n−dim⁡Z+k≤2dim⁡Fn-\dim Z+k\leq 2\dim F. Consequently, k≤δ(a)k\leq\delta(a) as claimed.

Now the conditions of support for the perverse sheaf rat⁡Mi\operatorname{rat}M_{i} imply that

The final assertion is a consequence of the isomorphism M−k≃Mk(k)M_{-k}\simeq M_{k}(k). ∎

Generic vanishing on the Picard variety

We now address the generic vanishing theorem of Nakano type, Theorem 3.2 in the introduction, and related questions. Ideally, such a theorem would say that

has codimension at least ∣p+q−n∣\lvert p+q-n\rvert in A^\widehat{A}. Unfortunately, such a good statement is not true in general (see Example 12.3 below, following [GL1]). To simplify our discussion of what the correct statement is, we make the following definition.

Let XX be a smooth projective variety. We say that XX satisfies the generic Nakano vanishing theorem with index kk if

Note that the absolute value is consistent with Serre duality, which implies that

We can use the analysis in §10 to obtain a precise formula for the index kk, namely we show that XX satisfies generic Nakano vanishing with index δ(a)\delta(a), but not with index δ(a)−1\delta(a)-1.

Recall from Proposition 11.2 that we have

It follows from the equivalence established in [Popa]*§3 that generic Nakano vanishing with index kk is equivalent to the statement that

We shall prove that this formula holds with k=δ(a)k=\delta(a) by descending induction on p≥0p\geq 0, starting from the trivial case p=n+1p=n+1. To simplify the bookkeeping, we set

Our result explains the original counterexample from [GL1]*§3. The example consisted in blowing up an abelian variety AA of dimension four along a smooth curve CC of genus at least two; if XX denotes the resulting variety, then a ⁣:X→Aa\colon X\to A is the Albanese mapping, and a short computation shows that

for every L∈Pic⁡0(A)L\in\operatorname{Pic}^{0}(A). This example makes it clear that the index in the generic Nakano vanishing theorem is not equal to the dimension of the generic fiber of the Albanese mapping. On the other hand, it is not hard to convince oneself that

Thus δ(a)=1\delta(a)=1 is the correct value for the index in this case.

Theorem 3.2, combined with the equivalence between (1) and (3) in Theorem 8.1, implies a vanishing result for the cohomology sheaves of the Fourier-Mukai transform of any ΩXp\Omega_{X}^{p}, in analogy with the result for OX\mathscr{O}_{X} conjectured by Green and Lazarsfeld and proved in [Hacon] (note again that P−1≃(1×(−1))∗PP^{-1}\simeq(1\times(-1))^{*}P, so for vanishing PP and P−1P^{-1} can be used interchangeably).

With the notation above, for every integer pp we have

Moreover, Rn−p−δ(a)ΦPΩXp≠0R^{n-p-\delta(a)}\Phi_{P}\Omega_{X}^{p}\neq 0 for some pp.

Let us finally note that Theorem 3.2 and its proof improve the previously known generic vanishing results for ΩXp\Omega_{X}^{p} with p<np<n, and recover those for ωX\omega_{X} (or its higher direct images):

First, it was proved in [PP]*Theorem 5.11 that

with μ(a)=max{k,m−1}\mu(a)={\rm max}\{k,m-1\}, kk being the minimal dimension and mm the maximal dimension of a fiber of the Albanese map. It is a routine check that δ(a)≤μ(a)\delta(a)\leq\mu(a).

Secondly, in the case of the lowest nonzero piece of the filtration on a∗(OX,F)a_{*}(\mathscr{O}_{X},F) the situation is better than what comes out of Theorem 3.2. This allows one to recover the original generic vanishing theorem for ωX\omega_{X} of [GL1], as well as its extension to higher direct images Rja∗ωXR^{j}a_{*}\omega_{X} given in [Hacon]. Indeed, in the proof above note that

This shows that Ria∗ωX≃gr⁡g−nFMiR^{i}a_{*}\omega_{X}\simeq\operatorname{gr}_{g-n}^{F}\mathcal{M}_{i}. Since these sheaves are torsion-free by virtue of Kollár’s theorem, it follows that gr⁡g−nFMi=0\operatorname{gr}_{g-n}^{F}\mathcal{M}_{i}=0 unless 0≤i≤dim⁡X−dim⁡a(X)0\leq i\leq\dim X-\dim a(X). Thus one recovers the original generic vanishing theorem of Green and Lazarsfeld. A similar argument works replacing ωX\omega_{X} by higher direct images Rif∗ωYR^{i}f_{*}\omega_{Y}, where f ⁣:Y→Xf\colon Y\rightarrow X is a projective morphism with YY smooth and XX projective and generically finite over AA.

D. Cohomological support loci for local systems

Let AA be an abelian variety of dimension gg, and set as before V=H0(A,ΩA1)V=H^{0}(A,\Omega_{A}^{1}) and S=Sym⁡V∗S=\operatorname{Sym}V^{\ast}. Let MM be a mixed Hodge module on AA, with underlying filtered D\mathscr{D}-module (M,F)(\mathcal{M},F). Then gr⁡∙FM\operatorname{gr}_{\bullet}^{F}\mathcal{M} is a finitely-generated graded module over Sym⁡TA≃OA⊗S\operatorname{Sym}\mathscr{T}_{A}\simeq\mathscr{O}_{A}\otimes S, and we denote the associated coherent sheaf on T∗A=A×VT^{\ast}A=A\times V by C(M,F)\mathscr{C}(\mathcal{M},F). We may then define the total Fourier-Mukai transform of gr⁡∙FM\operatorname{gr}_{\bullet}^{F}\mathcal{M} to be

where the notation is as in the following diagram:

Let now XX be a smooth projective variety of dimension nn, let a ⁣:X→Aa\colon X\to A its Albanese map, and consider again the decomposition

Denote by Ci,j=C(Mi,j,F)\mathscr{C}_{i,j}=\mathscr{C}(\mathcal{M}_{i,j},F) the coherent sheaf on T∗A=A×VT^{\ast}A=A\times V determined by the Hodge module Mi,jM_{i,j}. The supports in A^×V\widehat{A}\times V of the total Fourier-Mukai transforms RΦPCi,j\mathbf{R}\Phi_{P}\mathscr{C}_{i,j} are of a very special kind; this follows by using a result of Arapura [Arapura]. To state the result, we recall the following term coined by Simpson [Simpson2]*p. 365.

A triple torus is any subvariety of A^×H0(A,ΩA1)\widehat{A}\times H^{0}(A,\Omega_{A}^{1}) of the form

for a surjective morphism φ ⁣:A→B\varphi\colon A\to B to another abelian variety BB. A subvariety is called a torsion translate of a triple torus if it is a translate of a triple torus by a point of finite order in A×H0(A,ΩA1)A\times H^{0}(A,\Omega_{A}^{1}).

With notation as above, every irreducible component of the support of RΦPCi,j\mathbf{R}\Phi_{P}\mathscr{C}_{i,j} is a torsion translate of a triple torus in A^×V\widehat{A}\times V.

where p1 ⁣:X×V→Xp_{1}\colon X\times V\to X, and the complex in brackets is placed in degrees −n,…,0-n,\dotsc,0, and has differential induced by the evaluation map OX⊗V→ΩX1\mathscr{O}_{X}\otimes V\to\Omega_{X}^{1}.

where we denote the Koszul complex associated to a single one-form ω∈V\omega\in V by

It follows from [Arapura]*Corollary on p. 312 and [Simpson2] that each irreducible component of Zk(m)Z^{k}(m) is a torsion translate of a triple torus. To relate this information to the support of the total Fourier-Mukai transforms RΦPCi,j\mathbf{R}\Phi_{P}\mathscr{C}_{i,j}, we also introduce

Finally, we observe that each irreducible component of \operatorname{Supp}\bigl{(}\mathbf{R}\Phi_{P}\mathscr{C}_{i,j}\bigr{)} must also be an irreducible component of one the sets Zi,jk:=Zi,jk(1)Z_{i,j}^{k}:=Z_{i,j}^{k}(1), which concludes the proof. More precisely, we have

Indeed, the base change theorem shows that \operatorname{Supp}\bigl{(}R^{k}\Phi_{P}\mathscr{C}_{i,j}\bigr{)}\subset Z^{k}_{i,j} for all kk, with equality if k≫0k\gg 0. Now assume that (L,ω)∈Zi,jk(L,\omega)\in Z^{k}_{i,j} is a general point of a component which is not contained in \operatorname{Supp}\bigl{(}R^{k}\Phi_{P}\mathscr{C}_{i,j}\bigr{)}. We claim that then (L,ω)∈Zi,jk+1(L,\omega)\in Z^{k+1}_{i,j}, which concludes the proof by descending induction. If this were not the case, then again by the base change theorem, the natural map

would be surjective, which would contradict (L,\omega)\notin\operatorname{Supp}\bigl{(}R^{k}\Phi_{P}\mathscr{C}_{i,j}\bigr{)}. ∎

Generic vanishing for rank one local systems

One can define an isomorphism of real (but not complex) algebraic Lie groups

where the Koszul-type complex in brackets is again placed in degrees −n,…,0-n,\dotsc,0.

We can now obtain the generic vanishing theorem for local systems of rank one, stated in the introduction.

Note first that, since Verdier duality gives an isomorphism

we only need to prove the asserted inequality for k≥nk\geq n. Furthermore, Lemma 14.1 shows that it is enough to prove, for k≥0k\geq 0, the analogous inequality

for the subsets Zk(1)⊆Higgs(X)Z^{k}(1)\subseteq{\rm Higgs}(X) that were introduced during the proof of Proposition 13.2. Recall from there that

Finally, we will see in a moment in the proof of Theorem 15.2 that

Duality and perversity for total transforms

In this section, we take a closer look at the behavior of the object C(M,F)\mathscr{C}(\mathcal{M},F) under the total Fourier-Mukai transform. We begin with a result that shows how the total Fourier-Mukai transform interacts with Verdier duality for mixed Hodge modules.

Let MM be a mixed Hodge module on AA, let M′M^{\prime} be its Verdier dual, and let C(M,F)\mathscr{C}(\mathcal{M},F) and C(M′,F)\mathscr{C}(\mathcal{M}^{\prime},F) be the associated coherent sheaves on A×VA\times V. Then

where ι=(−1A^)×(−1V)\iota=(-1_{\widehat{A}})\times(-1_{V}).

Recall that the Grothendieck dual on a smooth algebraic variety XX is given by \mathbf{D}_{X}(-)=\mathbf{R}\mathcal{H}\mathit{om}\bigl{(}-,\omega_{X}[\dim X]\bigr{)}. To simplify the notation, set C=C(M,F)\mathscr{C}=\mathscr{C}(\mathcal{M},F) and C′=C(M′,F)\mathscr{C}^{\prime}=\mathscr{C}(\mathcal{M}^{\prime},F). Then

For the first isomorphism we use Grothendieck duality, while for the second we use Theorem 6.4. Since dim⁡A^×V=2g\dim\widehat{A}\times V=2g, this implies the result. ∎

With notation as above, each RΦPCi,j\mathbf{R}\Phi_{P}\mathscr{C}_{i,j} is a mm-perverse coherent sheaf on A^×V\widehat{A}\times V. More precisely, the support of the object RΦPCi,j\mathbf{R}\Phi_{P}\mathscr{C}_{i,j} is a finite union of torsion translates of triple tori, subject to the inequality

Let q ⁣:A^×V→A^q\colon\widehat{A}\times V\to\widehat{A} be the first projection. Since we are dealing with sheaves of graded modules, the support of the quasi-coherent sheaf

Perverse coherent sheaves on the space of holomorphic one-forms

We conclude this part by observing that, in analogy with the method described in [Popa], our method also produces natural perverse coherent sheaves on the affine space V=H0(A,ΩA1)V=H^{0}(A,\Omega_{A}^{1}), where AA is an abelian variety of dimension gg. We shall use the following projection maps:

This is an exercise in interchanging Grothendieck duality with pushforward by proper maps and pullback by smooth maps. ∎

We can essentially rephrase Lemma 9.1 as follows.

Let MM be a mixed Hodge module on an abelian variety AA, with underlying filtered D\mathscr{D}-module (M,F)(\mathcal{M},F), and let C(M,F)\mathscr{C}(\mathcal{M},F) be the coherent sheaf on A×VA\times V associated to gr⁡∙FM\operatorname{gr}_{\bullet}^{F}\mathcal{M}. Then for every ample line bundle LL on AA, one has

VV being affine, it suffices to prove that the hypercohomology of the complex is concentrated in degree . But this hypercohomology is equal to

which vanishes for i>0i>0 because of Lemma 9.1. ∎

We can now obtain perverse coherent sheaves on the affine space VV by pushing forward along the projection q ⁣:A×V→Vq\colon A\times V\to V.

Let MM be a mixed Hodge module on AA, with underlying filtered D\mathscr{D}-module (M,F)(\mathcal{M},F), and let C(M,F)\mathscr{C}(\mathcal{M},F) be the coherent sheaf on A×VA\times V associated to gr⁡∙FM\operatorname{gr}_{\bullet}^{F}\mathcal{M}. Then for every ample line bundle LL on A^\widehat{A}, one has

By Lemma 16.1 and Theorem 6.4, this object is isomorphic to

where C(M′,F)\mathscr{C}(\mathcal{M}^{\prime},F) is associated to the Verdier dual M′=DAMM^{\prime}=\mathbf{D}_{A}M. Now we apply the usual covering trick. Let φL ⁣:A^→A\varphi_{L}\colon\widehat{A}\to A be the isogeny defined by LL. Then the object in (16.4) will belong to Coh⁡(OV)\operatorname{Coh}(\mathscr{O}_{V}) provided the same is true for

Since φL∗C(M′,F)\varphi_{L}^{\ast}\mathscr{C}(\mathcal{M}^{\prime},F) comes from the mixed Hodge module φL∗M′\varphi_{L}^{\ast}M^{\prime}, this is a consequence of Lemma 16.2. ∎

E. Strong linearity

We start by setting up some notation. Let AA be a complex abelian variety of dimension gg, and let A♮A^{\natural} be the moduli space of algebraic line bundles with integrable connection on AA. Note that A♮A^{\natural} naturally has the structure of a quasi-projective algebraic variety: on A^\widehat{A}, there is a canonical vector bundle extension

and A♮A^{\natural} is isomorphic to the preimage of A^×{1}\widehat{A}\times\{1\} inside EA^E_{\widehat{A}}. The projection

is thus a torsor for the trivial bundle A^×H0(A,ΩA1)\widehat{A}\times H^{0}(A,\Omega_{A}^{1}); this corresponds to the fact that ∇+ω\nabla+\omega is again an integrable connection for any ω∈H0(A,ΩA1)\omega\in H^{0}(A,\Omega_{A}^{1}). Note that A♮A^{\natural} is a group under tensor product, and that the trivial line bundle (OA,d)(\mathscr{O}_{A},d) plays the role of the zero element.

Recall now that Laumon [Laumon2] and Rothstein [Rothstein] have extended the Fourier-Mukai transform to D\mathscr{D}-modules. Their generalized Fourier-Mukai transform takes bounded complexes of coherent algebraic D\mathscr{D}-modules on AA to bounded complexes of algebraic coherent sheaves on A♮A^{\natural}; we briefly describe it following the presentation in [Laumon2]*§3, which is more convenient for our purpose. On the product A×A♮A\times A^{\natural}, the pullback P♮P^{\natural} of the Poincaré bundle PP is endowed with a universal integrable connection ∇♮ ⁣:P♮→ΩA×A♮/A♮1⊗P♮\nabla^{\natural}\colon P^{\natural}\to\Omega_{A\times A^{\natural}/A^{\natural}}^{1}\otimes P^{\natural}, relative to A♮A^{\natural}. Given any algebraic left D\mathcal{D}-module M\mathcal{M} on AA, interpreted as a quasi-coherent sheaf with integrable connection, we consider p1∗M⊗P♮p_{1}^{*}\mathcal{M}\otimes P^{\natural} on A×A♮A\times A^{\natural}, endowed with the natural tensor product integrable connection ∇\nabla relative to A♮A^{\natural}. We then define

where DR(p1∗M⊗P♮,∇){\rm DR}(p_{1}^{*}\mathcal{M}\otimes P^{\natural},\nabla) is the usual (relative) de Rham complex

placed in degrees −g,…,0-g,\ldots,0. As all of the entries in this complex are relative to A♮A^{\natural}, it follows that RΦP♮M\mathbf{R}\Phi_{P^{\natural}}\mathcal{M} is represented by a complex of algebraic quasi-coherent sheaves on A♮A^{\natural}. Restricted to coherent D\mathcal{D}-modules, this is shown to induce an equivalence of categories

The same result is obtained by a different method in [Rothstein]*Theorem 6.2.

Since A♮A^{\natural} is not compact, it is essential to consider algebraic coherent sheaves on A♮A^{\natural} in the above equivalence. On AA, this problem does not arise, because the category of coherent analytic D\mathscr{D}-modules on a smooth projective variety is equivalent to the category of coherent algebraic D\mathscr{D}-modules by a version of the GAGA theorem.

Now let XX be a smooth projective variety with Albanese map a ⁣:X→Aa\colon X\to A. By first pushing forward to AA, or equivalently by working with the pullback of (P♮,∇♮)(P^{\natural},\nabla^{\natural}) to X×A♮X\times A^{\natural}, one can similarly define

In this and the following six subsections, our goal is to prove the following linearity property for the Fourier-Mukai transform of the trivial D\mathscr{D}-module OX\mathscr{O}_{X} (see Definition 23.1 below for the definition of a linear complex over a local ring).

We conclude this subsection by noting that, regardless of the explicit linear representation, in combination with Proposition 23.3 below we obtain that every direct summand of RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} is also isomorphic to a linear complex in an analytic neighborhood of any given point on A♮A^{\natural}.

Analytic description

and this is compatible with the exact sequence

We can similarly interpret the pullback of the Poincaré bundle to the complex manifold X×WX\times W. Let Ck(X×W/W)\mathscr{C}^{k}(X\times W/W) be the sheaf of smooth complex-valued relative kk-forms on X×WX\times W that are in the kernel of ∂ˉW\bar{\partial}_{W}, meaning holomorphic in the direction of WW, and denote by

This leads to the following analytic description of the Fourier-Mukai transform (similar to [GL2]*Proposition 2.3). Let

be the differential operator defined by the rule D(α)=dXα+T∧αD(\alpha)=d_{X}\alpha+T\wedge\alpha. Using that dXT=0d_{X}T=0, it is easy to see that D∘D=0D\circ D=0.

The complex of OW\mathscr{O}_{W}-modules \bigl{(}C^{\bullet}(X\times W/W),D\bigr{)} is quasi-isomorphic to the pullback π∗RΦP♮OX\pi^{\ast}\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X}, where π:W→A♮\pi:W\rightarrow A^{\natural} is the universal cover.

By the definition of the Fourier transform, RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} is the derived pushforward, via the projection p2 ⁣:X×A♮→A♮p_{2}\colon X\times A^{\natural}\to A^{\natural}, of the complex

where (P♮,∇♮)(P^{\natural},\nabla^{\natural}) denotes the pullback of the Poincaré bundle to X×A♮X\times A^{\natural}. Since π ⁣:W→A♮\pi\colon W\to A^{\natural} is a covering map, we thus obtain

To obtain the desired result, it suffices then to note that

This follows from a standard partition of unity argument as in [GH]*p. 42. ∎

Then the RR-module CkC^{k} consists of all convergent power series of the form

Then each differential D ⁣:Ck→Ck+1D\colon C^{k}\to C^{k+1} is given by the formula

Note that each RR-module in the complex has infinite rank; moreover, in the formula for the differential DD, the first of the two terms is not linear in z1,…,z2gz_{1},\dotsc,z_{2g}. Our goal is then to build a linear complex quasi-isomorphic to

by using harmonic forms with coefficients in the flat line bundle corresponding to τ\tau. The space of dτd_{\tau}-harmonic forms has the advantage of being finite-dimensional; in addition, any such form α∈Ak(X)\alpha\in A^{k}(X) satisfies dτα=0d_{\tau}\alpha=0, and hence

This shows that the differential is linear when restricted to the free RR-module generated by the dτd_{\tau}-harmonic forms. The only problem is that we do not obtain a subcomplex of (C∙,D)(C^{\bullet},D) in this way, because the wedge product ej∧αe_{j}\wedge\alpha is in general no longer harmonic. This difficulty can be overcome by constructing a more careful embedding of the space of dτd_{\tau}-harmonic kk-forms into CkC^{k}, as we now explain.

Harmonic theory for flat line bundles

In this section, we summarize the theory of harmonic forms with coefficients in a flat line bundle, developed by Simpson [Simpson]. Let Ak(X)A^{k}(X) be the space of smooth complex-valued kk-forms on XX. Choose a Kähler metric on XX, with Kähler form ω∈A2(X)\omega\in A^{2}(X), and denote by

the associated Lefschetz operator. The metric gives rise to the ∗\ast-operator

defines a Hermitian inner product on the space Ak(X)A^{k}(X). With respect to these inner products, the adjoint of L ⁣:Ak(X)→Ak+2(X)L\colon A^{k}(X)\to A^{k+2}(X) is the operator Λ ⁣:Ak(X)→Ak−2(X)\Lambda\colon A^{k}(X)\to A^{k-2}(X). Likewise, the adjoint of the exterior derivative d ⁣:Ak(X)→Ak+1(X)d\colon A^{k}(X)\to A^{k+1}(X) is the operator d∗ ⁣:Ak(X)→Ak−1(X)d^{\ast}\colon A^{k}(X)\to A^{k-1}(X), described more explicitly as d∗α=−∗d∗αd^{\ast}\alpha=-\ast d\ast\alpha. We use the notation d=∂+∂ˉd=\partial+\bar{\partial} for the decomposition of dd by type; thus ∂\partial maps (p,q)(p,q)-forms to (p+1,q)(p+1,q)-forms, and ∂ˉ\bar{\partial} maps (p,q)(p,q)-forms to (p,q+1)(p,q+1)-forms.

and both the ∗\ast-operator and the inner product induced by the harmonic metric agree with the standard ones defined above.

As before, we let dτ=d+τd_{\tau}=d+\tau be the operator encoding the complex structure and integrable connection on (L,∇)(L,\nabla); concretely,

Let dτ∗ ⁣:Ak(X)→Ak−1(X)d^{\ast}_{\tau}\colon A^{k}(X)\to A^{k-1}(X) be the adjoint of dτd_{\tau} with respect to the inner products, and let Δτ=dτdτ∗+dτ∗dτ\Delta_{\tau}=d_{\tau}d^{\ast}_{\tau}+d^{\ast}_{\tau}d_{\tau} be the Laplace operator; it is an elliptic operator of second order. If we denote by

the space of dτd_{\tau}-harmonic kk-forms, then Hτk\mathcal{H}_{\tau}^{k} is finite-dimensional, and Hodge theory gives us a decomposition

orthogonal with respect to the inner product on Ak(X)A^{k}(X). Let Hτ ⁣:Ak(X)→HτkH_{\tau}\colon A^{k}(X)\to\mathcal{H}_{\tau}^{k} be the orthogonal projection to the space of harmonic forms. It is not hard to see that any α∈Ak(X)\alpha\in A^{k}(X) can be uniquely written in the form

where Gτα∈ΔτAk(X)G_{\tau}\alpha\in\Delta_{\tau}A^{k}(X) is the so-called Green’s operator. The uniqueness of the decomposition implies that dτGτ=Gτdτd_{\tau}G_{\tau}=G_{\tau}d_{\tau} and dτ∗Gτ=Gτdτ∗d^{\ast}_{\tau}G_{\tau}=G_{\tau}d^{\ast}_{\tau}.

Following Simpson, we have a decomposition dτ=∂τ+∂ˉτd_{\tau}=\partial_{\tau}+\bar{\partial}_{\tau}, where

The justification for defining these two peculiar operators is that they satisfy the usual Kähler identities (which fail for the naive choice ∂+τ1,0\partial+\tau^{1,0} and ∂ˉ+τ0,1\bar{\partial}+\tau^{0,1}).

We have ∂τ∂τ=∂ˉτ∂ˉτ=∂τ∂ˉτ+∂ˉτ∂τ=0\partial_{\tau}\partial_{\tau}=\bar{\partial}_{\tau}\bar{\partial}_{\tau}=\partial_{\tau}\bar{\partial}_{\tau}+\bar{\partial}_{\tau}\partial_{\tau}=0.

Let ∂τ∗\partial^{\ast}_{\tau} and ∂ˉτ∗\bar{\partial}^{\ast}_{\tau} denote the adjoints of ∂τ\partial_{\tau} and ∂ˉτ\bar{\partial}_{\tau}, respectively. Then the first-order Kähler identities

We have ∂ˉτ∂τ∗+∂τ∗∂ˉτ=∂τ∂ˉτ∗+∂ˉτ∗∂τ=0\bar{\partial}_{\tau}\partial^{\ast}_{\tau}+\partial^{\ast}_{\tau}\bar{\partial}_{\tau}=\partial_{\tau}\bar{\partial}^{\ast}_{\tau}+\bar{\partial}^{\ast}_{\tau}\partial_{\tau}=0.

and consequently, dτd_{\tau}-harmonic forms are both ∂τ\partial_{\tau}-closed and ∂τ∗\partial^{\ast}_{\tau}-closed.

We have H∂τ=H∂ˉτ=H∂τ∗=H∂ˉτ∗=0H\partial_{\tau}=H\bar{\partial}_{\tau}=H\partial^{\ast}_{\tau}=H\bar{\partial}^{\ast}_{\tau}=0.

The Green’s operator GτG_{\tau} commutes with ∂τ\partial_{\tau}, ∂ˉτ\bar{\partial}_{\tau}, ∂τ∗\partial^{\ast}_{\tau}, and ∂ˉτ∗\bar{\partial}^{\ast}_{\tau}.

Note that θ\theta is holomorphic on account of ∂ˉτ∂ˉτ=0\bar{\partial}_{\tau}\bar{\partial}_{\tau}=0. The complex structure on the original flat line bundle is defined by the operator ∂ˉ+τ0,1\bar{\partial}+\tau^{0,1}, which means that the two line bundles are different unless τ0,1=−τ1,0‾\tau^{0,1}=-\overline{\tau^{1,0}}.

Harmonic theory can be used to solve equations involving ∂τ\partial_{\tau} (or any of the other operators), as follows. Suppose that we are given an equation of the form ∂τα=β\partial_{\tau}\alpha=\beta. A necessary and sufficient condition for the existence of a solution α\alpha is that ∂τβ=0\partial_{\tau}\beta=0 and Hτβ=0H_{\tau}\beta=0. If this is the case, then among all possible solutions, there is a unique one that is ∂τ∗\partial^{\ast}_{\tau}-exact, namely 2∂τ∗Gτβ2\partial^{\ast}_{\tau}G_{\tau}\beta. (In fact, this is the solution of minimal norm.) Note that we can always define α=2∂τ∗Gτβ\alpha=2\partial^{\ast}_{\tau}G_{\tau}\beta; but since

we only obtain a solution to the original equation when Hτβ=0H_{\tau}\beta=0 and ∂τβ=0\partial_{\tau}\beta=0. This idea will appear again in the construction below.

Sobolev spaces and norm estimates

At some point of the construction below, we will need to prove the convergence of certain power series. This requires estimates for the norms of the two operators ∂ˉτ\bar{\partial}_{\tau} and GτG_{\tau} introduced above, which hold in suitable Sobolev spaces. Since this is standard material in the theory of partial differential equations, we only give the briefest possible summary; all the results that we use can be found, for example, in [Wells]*Chapter IV.

From the Kähler metric on XX, we get an L2L^{2}-norm on the space Ak(X)A^{k}(X) of smooth kk-forms, by the formula

It is equivalent to the usual L2L^{2}-norm, defined using partitions of unity. There is also a whole family of higher Sobolev norms: for α∈Ak(X)\alpha\in A^{k}(X), the mm-th order Sobolev norm ∥α∥m\lVert\alpha\rVert_{m} controls the L2L^{2}-norms of all derivatives of α\alpha of order at most mm. The Sobolev space Wmk(X)W_{m}^{k}(X) is the completion of Ak(X)A^{k}(X) with respect to the norm ∥−∥m\lVert-\rVert_{m}; it is a Hilbert space. Elements of Wmk(X)W_{m}^{k}(X) may be viewed as kk-forms α\alpha with measurable coefficients, all of whose weak derivatives of order at most mm are square-integrable. Here is the first result from analysis that we need.

The second result consists of a pair of norm inequalities, one for the differential operator ∂τ∗\partial^{\ast}_{\tau}, the other for the Green’s operator GτG_{\tau}.

There is a constant C>0C>0, depending on m≥1m\geq 1, such that

for every α∈Wmk(X)\alpha\in W_{m}^{k}(X) with m≥1m\geq 1.

There is another constant C>0C>0, depending on m≥0m\geq 0, such that

The inequality in (1) is straightforward, using the fact that ∂τ∗\partial^{\ast}_{\tau} is a first-order operator and XX is compact. On the other hand, (2) follows from the open mapping theorem. To summarize the argument in a few lines, (19.1) is actually derived from an orthogonal decomposition

of the Hilbert space Wmk(X)W_{m}^{k}(X). It implies that the bounded linear operator

is bijective; by the open mapping theorem, the inverse must be bounded as well. Since GτG_{\tau} is equal to this inverse on (Hτk)⊥(\mathcal{H}_{\tau}^{k})^{\perp}, and zero on Hτk\mathcal{H}_{\tau}^{k}, we obtain the desired inequality. ∎

Construction of the linear complex

We now return to the proof of Theorem 3.7. Recall that, after pullback to the universal covering space WW of A♮A^{\natural}, the stalk of the Fourier-Mukai transform of the D\mathscr{D}-module OX\mathscr{O}_{X} is represented by the complex of RR-modules

Our goal is to show that \bigl{(}C^{\bullet},D\bigr{)} is quasi-isomorphic to a linear complex over RR.

We begin by constructing a suitable linear complex from the finite-dimensional spaces of dτd_{\tau}-harmonic forms. Let \bigl{(}\mathcal{H}_{\tau}^{\bullet}\otimes R,\delta\bigr{)} be the complex

with differential obtained by RR-linear extension from

One can see that this is indeed a complex by projecting to the harmonic subspace; as a warm-up for later computations, we shall prove directly that δ∘δ=0\delta\circ\delta=0.

Before we begin the actual proof, let us make a useful observation: namely, that for every α∈Ak(X)\alpha\in A^{k}(X), one has

due to the fact that eje_{j} is a closed one-form. Now take α∈Hτk\alpha\in\mathcal{H}_{\tau}^{k}. Then

because dτ(ej∧α)=0d_{\tau}(e_{j}\wedge\alpha)=0 by the above observation. Consequently,

and since Hτdτ=0H_{\tau}d_{\tau}=0, this allows us to conclude that

which means that δ∘δ=0\delta\circ\delta=0. ∎

Note that it is clear from the representation of cohomology via harmonic forms that the complex thus constructed is quasi-isomorphic to the stalk at a point mapping to (L,∇)(L,\nabla) of the complex appearing in the statement of Theorem 3.7.

Construction of the quasi-isomorphism

We shall now construct a sequence of maps fk ⁣:Hτk→Ckf^{k}\colon\mathcal{H}_{\tau}^{k}\to C^{k}, in such a way that, after RR-linear extension, we obtain a quasi-isomorphism f ⁣:Hτ∙⊗R→C∙f\colon\mathcal{H}_{\tau}^{\bullet}\otimes R\to C^{\bullet}. In order for the maps fkf^{k} to define a morphism of complexes, the identity

should be satisfied for every α∈Hτk\alpha\in\mathcal{H}_{\tau}^{k}. As a first step, we shall find a formal solution to the problem, ignoring questions of convergence for the time being. Let C^k\hat{C}^{k} be the space of all formal power series

with αI∈Ak(X)\alpha_{I}\in A^{k}(X) smooth complex-valued kk-forms. We extend the various operators from Ak(X)A^{k}(X) to C^k\hat{C}^{k} by defining, for example,

Note that Ck⊆C^kC^{k}\subseteq\hat{C}^{k} is precisely the subspace of those power series that converge in some neighborhood of X×{z=0}X\times\{z=0\}.

To make sure that fk(α)f^{k}(\alpha) induces the correct map on cohomology, we require that Hτfk(α)=αH_{\tau}f^{k}(\alpha)=\alpha. Following the general strategy for solving equations with the help of harmonic theory, we impose the additional conditions ∂τfk(α)=0\partial_{\tau}f^{k}(\alpha)=0 and ∂ˉτ∗fk(α)=0\bar{\partial}^{\ast}_{\tau}f^{k}(\alpha)=0. Under these assumptions, (22.1) reduces to

On account of ∂ˉτ∗fk(α)=0\bar{\partial}^{\ast}_{\tau}f^{k}(\alpha)=0 and the Kähler identities, we should then have

This suggests that we try to solve the equation \bigl{(}\operatorname{id}+2\bar{\partial}^{\ast}_{\tau}G_{\tau}e\bigr{)}f^{k}(\alpha)=\alpha.

For any dτd_{\tau}-harmonic form α∈Hτk\alpha\in\mathcal{H}_{\tau}^{k}, the equation

has a unique formal solution β∈C^k\beta\in\hat{C}^{k}. This solution has the property that Hτβ=αH_{\tau}\beta=\alpha, as well as ∂ˉτ∗β=0\bar{\partial}^{\ast}_{\tau}\beta=0 and ∂τβ=0\partial_{\tau}\beta=0.

The next step is to prove the convergence of the power series defining the solution to (22.3). For ε>0\varepsilon>0, let

which is an open neighborhood of the point τ∈W\tau\in W.

There is an ε>0\varepsilon>0, such that for all α∈Hτk\alpha\in\mathcal{H}_{\tau}^{k}, the formal power series

converges absolutely and uniformly on X×WεX\times W_{\varepsilon} to an element of Ck(X×Wε/Wε)C^{k}(X\times W_{\varepsilon}/W_{\varepsilon}).

If we apply the estimates from Theorem 20.2 to the relation in (22.4), we find that for every m≥1m\geq 1, there is a constant Cm>0C_{m}>0, such that

Now choose a positive real number ε<1/C1\varepsilon<1/C_{1}. We then obtain

from which it follows that β\beta is absolutely and uniformly convergent in the L2L^{2}-norm as long as z∈Wεz\in W_{\varepsilon}. To prove that β\beta is actually smooth, we return to the original form of (22.6). It implies that, for any m≥1m\geq 1,

It remains to show that we have found a solution to the original problem (22.1).

For every α∈Hτk\alpha\in\mathcal{H}_{\tau}^{k}, we have Dfk(α)=fk+1(δα)Df^{k}(\alpha)=f^{k+1}(\delta\alpha).

Let β=fk(α)\beta=f^{k}(\alpha), so that (id⁡+2∂ˉτ∗Gτe)β=α(\operatorname{id}+2\bar{\partial}^{\ast}_{\tau}G_{\tau}e)\beta=\alpha and ∂τβ=0\partial_{\tau}\beta=0. Noting that δ(α)=Hτ(eα)\delta(\alpha)=H_{\tau}(e\alpha), we need to show that

Since e∘e=0e\circ e=0 and e(∂ˉτβ)=−∂ˉτ(eβ)e(\bar{\partial}_{\tau}\beta)=-\bar{\partial}_{\tau}(e\beta), we compute that

We always have eβ=Hτ(eβ)+2∂ˉτ∂ˉτ∗Gτeβ+2∂ˉτ∗∂ˉτGτeβe\beta=H_{\tau}(e\beta)+2\bar{\partial}_{\tau}\bar{\partial}^{\ast}_{\tau}G_{\tau}e\beta+2\bar{\partial}^{\ast}_{\tau}\bar{\partial}_{\tau}G_{\tau}e\beta, and so we can simplify the above to

Thus it suffices to prove that Hτ(eβ)=Hτ(eα)H_{\tau}(e\beta)=H_{\tau}(e\alpha). But this is straightforward: from Hτ(β)=αH_{\tau}(\beta)=\alpha and ∂τβ=0\partial_{\tau}\beta=0, we get β=α+2∂τ∂τ∗Gτβ\beta=\alpha+2\partial_{\tau}\partial^{\ast}_{\tau}G_{\tau}\beta, and therefore

Since Hτ∂τ=0H_{\tau}\partial_{\tau}=0, we obtain the desired identity Hτ(eβ)=Hτ(eα)H_{\tau}(e\beta)=H_{\tau}(e\alpha). ∎

The decomposition β=α+2∂τ∂τ∗Gτβ\beta=\alpha+2\partial_{\tau}\partial^{\ast}_{\tau}G_{\tau}\beta is the reason for imposing the additional condition ∂τfk(α)=0\partial_{\tau}f^{k}(\alpha)=0. Without this, it would be difficult to relate the dτd_{\tau}-harmonic parts of eαe\alpha and eβe\beta in the final step of the proof.

If we extend RR-linearly, we obtain maps of RR-modules fk ⁣:Hτk⊗R→Ckf^{k}\colon\mathcal{H}_{\tau}^{k}\otimes R\to C^{k}. Because (22.1) is satisfied, they define a morphism of complexes f\colon\bigl{(}\mathcal{H}_{\tau}^{\bullet}\otimes R,\delta\bigr{)}\to\bigl{(}C^{\bullet},D\bigr{)}.

f ⁣:Hτ∙⊗R→C∙f\colon\mathcal{H}_{\tau}^{\bullet}\otimes R\to C^{\bullet} is a quasi-isomorphism.

We use the spectral sequence (23.5). The complex Hτ∙⊗R\mathcal{H}_{\tau}^{\bullet}\otimes R is clearly linear, and so the associated spectral sequence

degenerates at E2E_{2} by Lemma 23.6. On the other hand, the complex C∙C^{\bullet} also satisfies the conditions needed to define (23.5), giving us a second convergent spectral sequence with

where ker⁡∇\ker\nabla is the local system corresponding to (L,∇)(L,\nabla). The morphism ff induces a morphism between the two spectral sequences; at E1E_{1}, it restricts to isomorphisms 1E1p,q≃2E1p,q{{}^{1}}E_{1}^{p,q}\simeq{{}^{2}}E_{1}^{p,q}, because Hτk≃Hk(X,ker⁡∇)\mathcal{H}_{\tau}^{k}\simeq H^{k}(X,\ker\nabla). It follows that the second spectral sequence also degenerates at E2E_{2}; it is then not hard to see that ff must be indeed a quasi-isomorphism. ∎

Filtered complexes and linear complexes

This section contains the homological algebra used in the constructions and proofs of the previous sections. It reviews and expands some of the content of [LPS]*§1, the main improvement with respect to that paper being Proposition 23.3.

Let (R,m)(R,\mathfrak{m}) be a regular local kk-algebra of dimension nn, with residue field k=R/mk=R/\mathfrak{m}. A linear complex over RR is a bounded complex \bigl{(}K^{\bullet},d\bigr{)} of finitely generated free RR-modules with the following property: there is a system of parameters t1,…,tn∈mt_{1},\dotsc,t_{n}\in\mathfrak{m}, such that every differential of the complex is a matrix of linear forms in t1,…,tnt_{1},\dotsc,t_{n}.

We say that a complex is quasi-linear over RR if it is quasi-isomorphic to a linear complex over RR.

Let K∙K^{\bullet} be a linear complex quasi-isomorphic to EE, and L∙L^{\bullet} a minimal complex quasi-isomorphic to E′E^{\prime}. Since E′E^{\prime} is a direct summand of EE in the derived category, there are morphisms of complexes

such that p∘sp\circ s is homotopic to the identity morphism of L∙L^{\bullet}. Because L∙L^{\bullet} is minimal, it follows that p∘sp\circ s reduces to the identity modulo m\mathfrak{m}, and is thus an isomorphism. After replacing pp by (p∘s)−1∘p(p\circ s)^{-1}\circ p, we may therefore assume without loss of generality that p∘s=id⁡p\circ s=\operatorname{id}.

Likewise, we may define s0 ⁣:L0i→Kis_{0}\colon L_{0}^{i}\to K^{i} as the constant part of s ⁣:Li→Kis\colon L^{i}\to K^{i}; that is to say, as the unique matrix with entries in the field kk such that (s−s0)(Li)⊆mKi(s-s_{0})(L^{i})\subseteq\mathfrak{m}K^{i}. Now consider the commutative diagram

By taking linear parts in the identity d∘s=s∘dd\circ s=s\circ d, and using the fact that K∙K^{\bullet} is a linear complex, we find that d∘s0=s0∘d0d\circ s_{0}=s_{0}\circ d_{0}; consequently, s0 ⁣:L0∙→K∙s_{0}\colon L_{0}^{\bullet}\to K^{\bullet} is a morphism of complexes. To conclude the proof, we consider the composition

By construction, p∘s0p\circ s_{0} reduces to the identity modulo m\mathfrak{m}, and is therefore an isomorphism. This shows that L∙L^{\bullet} is indeed isomorphic to a linear complex, as claimed. ∎

A necessary condition for quasi-linearity is the degeneration of a certain spectral sequence. To state this, we first recall some general facts. Let \bigl{(}K^{\bullet},F\bigr{)} be a filtered complex in an abelian category. We assume that the filtration is decreasing, meaning that FpKn⊇Fp+1KnF^{p}K^{n}\supseteq F^{p+1}K^{n}, and satisfies

Moreover, the differentials should respect the filtration, in the sense that d\bigl{(}F^{p}K^{n}\bigr{)}\subseteq F^{p}K^{n+1}. Under these assumptions, the filtered complex gives rise to a spectral sequence (of cohomological type)

It converges by the standard convergence criterion [McCleary]*Theorem 3.2.

Going back now to the situation of a regular local kk-algebra (R,m)(R,\mathfrak{m}) as above, on any bounded complex K∙K^{\bullet} of RR-modules with finitely generated cohomology, we can define the m\mathfrak{m}-adic filtration by setting

for all p≥0p\geq 0. Noting that mp/mp+1≃Sym⁡p(m/m2)\mathfrak{m}^{p}/\mathfrak{m}^{p+1}\simeq\operatorname{Sym}^{p}(\mathfrak{m}/\mathfrak{m}^{2}), we have

Provided that each KnK^{n} has the property that

the filtration satisfies the conditions necessary to define (23.4), and we obtain a convergent spectral sequence

It follows from the Artin-Rees theorem that the induced filtration on the limit is m\mathfrak{m}-good; in particular, the completion of H^{n}\bigl{(}K^{\bullet}\bigr{)} with respect to this filtration is isomorphic to H^{n}\bigl{(}K^{\bullet}\bigr{)}\otimes_{R}\hat{R}. In this sense, the spectral sequence describes the formal analytic stalk of the original complex.

If K∙K^{\bullet} is a linear complex, then the spectral sequence

Note that degeneration of the spectral sequence is not a sufficient condition for being quasi-linear: over R=k⟦x,y⟧R=k\llbracket x,y\rrbracket, the complex

is an example of a minimal complex that is not isomorphic to a linear complex, but where the spectral sequence nevertheless degenerates at E2E_{2}.

F. Perversity and the cohomology algebra

An important issue is to understand the exactness properties of the derivative-type complexes appearing in Theorem 3.7. In the case of the standard Fourier-Mukai transform RΦPOX\mathbf{R}\Phi_{P}\mathscr{O}_{X}, it was emphasized in [LP] that this is a crucial step towards obtaining qualitative and quantitative information about the cohomology algebra of XX.

As our complexes locally represent the object RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X}, an equivalent problem is to prove a vanishing statement for the higher direct images RiΦP♮OXR^{i}\Phi_{P^{\natural}}\mathscr{O}_{X}. This turns out to be related to the behavior of RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} with respect to the tt-structure mm defined in §7. Before rephrasing Theorem 3.8 in this language, note that due to the degree convention for the de Rham complex associated to a D\mathscr{D}-module M\mathcal{M}, definition 17.1 implies that RiΦP♮OX=0R^{i}\Phi_{P^{\natural}}\mathscr{O}_{X}=0 for ∣i∣>n:=dim⁡X\lvert i\rvert>n:=\dim X.

For any smooth projective complex variety XX we have

In particular, if the Albanese map of XX is semismall, RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} is an mm-perverse coherent sheaf on A♮A^{\natural}.

This is implied by our generic vanishing statement for local systems. Indeed, note that by Theorem 3.5, in the character space Char(X){\rm Char}(X) we have

for any i≥0i\geq 0. Let us now define the locus

where X♮X^{\natural} denotes the moduli space of line bundles with integrable connection on XX. Via the well-known correspondence between bundles with integrable connection and local systems, we have a biholomorphic identification

such that, as in the proof of Theorem 3.5, one has

and since by base change we have Supp RiΦP♮OX⊂Si(X){\rm Supp}~{}R^{i}\Phi_{P^{\natural}}\mathscr{O}_{X}\subset S^{i}(X), we finally obtain

For any smooth projective complex variety XX we have

This follows immediately from Theorem 24.1 and Lemma 7.4. ∎

The second part of Theorem 24.1 can be generalized by replacing OX\mathscr{O}_{X} (or rather a∗OXa_{*}\mathscr{O}_{X}) by any holonomic D\mathscr{D}-module on AA; see Corollary 26.2 below. Due to this fact, the decomposition theorem, and Proposition 11.2, one can in fact draw an even stronger conclusion about RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X}, namely that

with EiE_{i} an mm-perverse coherent sheaf on A♮A^{\natural} for each ii.

Regularity of the cohomology algebra.

The results of the previous section can be used to understand finer properties of the singular cohomology algebra of XX as a graded module over the cohomology algebra of Alb⁡(X)\operatorname{Alb}(X). We follow the method introduced in [LP]. More precisely, we define

Via cup product, we may view this as a graded module over the exterior algebra

Using the results above, we can bound the degrees of the generators and syzygies of PXP_{X} as an exterior module. To this end, recall the following analogue of Castelnuovo-Mumford regularity for modules over the exterior algebra: given a graded EE-module QQ generated in degrees ≤d\leq d, one says that EE is mm-regular if the generators of QQ appear in degrees d,d−1,…,d−md,d-1,\ldots,d-m, the relations among these generators are in degrees d−1,…,d−m−1d-1,\ldots,d-m-1, and more generally the pp-th module of syzygies of QQ has all its generators in degrees d−p,…,d−m−pd-p,\dotsc,d-m-p. An equivalent condition (see [LP]*Proposition 2.2) is the vanishing

In view of Theorem 3.7 and Corollary 24.2, this follows precisely as in [LP]*§2, and we will only briefly sketch the details. On WW we have the complex K∙\mathcal{K}^{\bullet} of trivial vector bundles

placed in degrees −n,…,n-n,\dotsc,n, appearing in Theorem 3.7 for (L,∇)=(OX,d)(L,\nabla)=(\mathscr{O}_{X},d). Passing to global sections, we obtain a complex LX:=Γ(X,K∙)\mathbf{L}_{X}:=\Gamma(X,\mathcal{K}^{\bullet}), equal to

where S=Sym(W∨)S={\rm Sym}(W^{\vee}). The Koszul-type differential of the complex K∙\mathcal{K}^{\bullet} implies that LX=L(PX)\mathbf{L}_{X}=\mathbf{L}(P_{X}), the BGG-complex associated to the exterior module PXP_{X} via the BGG correspondence; this is a linear complex of free SS-modules. Since WW is an affine space, the exactness properties of LX\mathbf{L}_{X} are dictated by those of K∙\mathcal{K}^{\bullet} around the origin (note that the differentials of K∙\mathcal{K}^{\bullet} scale linearly along radial directions). But by Theorem 3.7, the complex K∙\mathcal{K}^{\bullet} represents RΦP♮OX\mathbf{R}\Phi_{P^{\natural}}\mathscr{O}_{X} in an analytic neighborhood of the origin. Corollary 24.2 therefore implies that LX\mathbf{L}_{X} is exact in cohomological degrees <−δ(a)<-\delta(a). Since the dual graded EE-module is again isomorphic to PXP_{X}, [Eisenbud]*Theorem 7.8 shows that we have

The best possible situation is when the Albanese map of XX is semismall, in which case PXP_{X} is nn-regular. This, as well as the general result, is optimal. We check this in some simple examples.

where i1,…,ia,j1,…,jb,k1,…,kci_{1},\dotsc,i_{a},j_{1},\dotsc,j_{b},k_{1},\dotsc,k_{c} are distinct integers in {1,…,g}\{1,\dotsc,g\}, and a+b+2c+d=n+1a+b+2c+d=n+1. In the notation introduced above, this implies that PCnP_{C_{n}} is generated as a graded EE-module by the elements ηk\eta^{k}, with k=0,…,nk=0,\ldots,n, while the relations imply that for k>n/2k>n/2, these generators are obtained from those in lower degrees. It follows that PCnP_{C_{n}} is actually generated in degrees 0,…,n0,\dotsc,n. On the other hand, note that when nn is even, ηn/2\eta^{n/2} is indeed a new generator in degree , not coming from lower degrees. This shows that in this case Corollary 3.10 is sharp. Equivalently, up to (and including) the degree −1-1 term, the complex LCn\mathbf{L}_{C_{n}} is exact. Is obtained as a direct sum of Koszul complexes in the vector space WW, with a new one starting in each even degree; in other words, at a point w∈Ww\in W, its first half looks as follows:

where the differentials are given by wedging with ww.

Since the differentials are given by wedging with 11-forms, the complex LX\mathbf{L}_{X} is then, up to the H4H^{4}-term, the direct sum of the (truncation of) the Koszul complex corresponding to AA, and the following sequence corresponding to the cohomology of EE, starting at H2H^{2}:

This is exact at the first step, but clearly not at the second, which shows that LX\mathbf{L}_{X} is exact at the first three terms, as in Corollary 3.10, but not at the fourth. Equivalently, PXP_{X} is 55-regular, but not 44-regular.

Finally, we note that the partial exactness of the complex LX\mathbf{L}_{X} in Corollary 3.10 would have numerous quantitative applications related to the Betti numbers of XX, again as in [LP], in the case when R−δ(a)ΦP♮OXR^{-\delta(a)}\Phi_{P^{\natural}}\mathscr{O}_{X} is locally free in a punctured neighborhood of the origin. At the moment we do not have a good understanding of geometric conditions that would imply this. It is however not hard to see that the absence of irregular fibrations for XX does not suffice (as in the case of the standard Fourier-Mukai transform), even when the Albanese map is semismall.

G. Generalizations and open problems

In light of our results, it should be clear that all the theorems in generic vanishing theory are in reality statements about a certain class of filtered D\mathscr{D}-modules on abelian varieties, namely those underlying mixed Hodge modules. Moreover, the dimension (D), linearity (L), and strong linearity (SL) results that we have discussed should be viewed as properties of the Fourier-Mukai transforms of such D\mathscr{D}-modules.

A natural question is then whether there is a larger (and more easily described) class of D\mathscr{D}-modules on abelian varieties for which the same results are true. It is known that when (M,F)(\mathcal{M},F) underlies a mixed Hodge module MM, the D\mathscr{D}-module M\mathcal{M} is always regular and holonomic; when MM is pure, M\mathcal{M} is in addition semi-simple. This suggests that the results of generic vanishing theory might extend to D\mathscr{D}-modules with those properties on abelian varieties.

Using the recent work of Sabbah [Sabbah1, Sabbah2] and Mochizuki [Mochizuki1, Mochizuki2] on the correspondence between semi-simple holonomic D\mathscr{D}-modules and polarizable twistor D\mathscr{D}-modules, such an extension is indeed possible. The results are as follows.

is a finite union of translates of triple tori in A♮A^{\natural}; the translates are by torsion points when M\mathcal{M} is of geometric origin. The cohomological support loci satisfy

in the special case when M\mathcal{M} is a single holonomic D\mathscr{D}-module.

The theorem implies the analogous result for cohomological support loci of constructible complexes and perverse sheaves, which are now subsets of Char(A){\rm Char}(A); this is because of the Riemann-Hilbert correspondence. By the usual base change arguments, one derives the following properties of the Fourier-Mukai transform.

is satisfied, which implies that RΦP♮M\mathbf{R}\Phi_{P^{\natural}}\mathcal{M} is an mm-perverse coherent sheaf on A♮A^{\natural}.

For semi-simple holonomic D\mathscr{D}-modules, there is also a result analogous to (SL).

If M\mathcal{M} is a semi-simple holonomic D\mathscr{D}-module on AA, then the Fourier-Mukai transform RΦP♮M\mathbf{R}\Phi_{P^{\natural}}\mathcal{M} is locally, in the analytic topology, quasi-isomorphic to a linear complex constructed from the cohomology of twists of M\mathcal{M}.

Open problems

Given the discussion above, a very interesting problem in this context is the following:

The two results above give several necessary conditions, so the problem is really to find sufficient conditions. Such a description might also shed some light on the difficult question of which D\mathscr{D}-modules are of geometric origin.

One may also wonder whether there are extensions of various results in this paper in the non-projective setting.

Does the analogue of Theorem 3.1 hold on arbitrary complex tori?

Note that the (SL) type result, Theorem 3.7, generalizes to compact Kähler manifolds, since the proof only uses harmonic theory. This raises the question whether our statements of type (D), here relying heavily on vanishing theorems for ample line bundles, extend to that context as well.

Are there analogues of the generic vanishing theorems 3.2, 3.5 and 3.8 in the Kähler setting?

Finally, with respect to the discussion at the end of §25, it is natural to address the following:

Find geometric conditions on XX under which the higher direct image R−δ(a)ΦP♮OXR^{-\delta(a)}\Phi_{P^{\natural}}\mathscr{O}_{X} is locally free in a punctured neighborhood of the origin. As a stronger question, find such conditions under which cohomological support loci Σi(X)\Sigma^{i}(X) contain the origin as an isolated point for all i>n−δ(a)i>n-\delta(a).

References