
TL;DR
This paper extends the infinitesimal Torelli theorem, originally for smooth hypersurfaces, to include nodal hypersurfaces, broadening the understanding of their deformation theory.
Contribution
It introduces a generalization of the infinitesimal Torelli theorem to nodal hypersurfaces, which were not covered by previous results.
Findings
Infinitesimal Torelli theorem holds for certain classes of nodal hypersurfaces.
Extension of deformation theory to singular hypersurfaces.
New techniques for analyzing nodal hypersurface deformations.
Abstract
We extend the infinitesimal Torelli theorem for smooth hypersurfaces to nodal hypersurfaces.
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On Deformations of Nodal Hypersurfaces
ZHENJIAN WANG
Univ. Cte d’Azur, CNRS, LJAD, UMR 7351, 06100 Nice, France.
Abstract.
We extend the infinitesimal Torelli theorem for smooth hypersurfaces to nodal hypersurfaces.
Key words and phrases:
Nodal hypersurfaces, Deformations, Torelli theorem
2010 Mathematics Subject Classification:
Primary 32S35, Secondary 14C30, 14D07, 32S25
1. Introduction
Deformations of smooth hypersurfaces provide examples of great interest and importance in the theory of variation of Hodge structures, especially because of the generic Torelli theorem, see [13], Chapter 6. In a recent thesis [15], Y. Zhao considers deformations of nodal surfaces in the -dimensional complex projective space and shows that the infinitesimal Torelli theorem still holds.
Let be the graded ring of polynomials and let be a homogeneous polynomial of degree . Denote by the hypersurface in defined by . Moreover, let
[TABLE]
be the graded ideal generated by the first derivatives of , also called the Jacobian ideal of . We consider the following map
[TABLE]
As a matter of fact, Y. Zhao [15] proves the infinitesimal Torelli theorem by showing that the map is injective when and is a nodal surface. This result can be extended to higher dimensional cases.
Theorem 1.1**.**
Assume is an integer and . Let be a homogeneous polynomial of degree such that is a nodal hypersurface in . Then the map is injective.
As it is proved in [15], Chapter 3, Example 3.1.3, parameterizes the equivalence classes of deformations of the pair . Alternatively, let be the general linear group of rank . Then acts on by coordinate transformations and for any , the tangent space at of the orbit is given by , see [1], Chapter 4, Formula (4.16). It follows that can be seen as the set of directions in that are transversal to the orbit at . In addition, any smooth analytic subset can be seen as a family of hypersurfaces in . If and , then we call an effective deformation of . From this point of view, is the maximal set of effective deformations of .
Now let be a nodal hypersurface in and let be the number of nodes in . Then we have a moduli space, denoted by , parameterizing all nodal hypersurfaces in having exactly nodes. By the discussion following Corollary 3.8 in [2], Chapter 1, we have that is a constructible subvariety of and the topological type of is locally trivial for . Moreover, for any lying in the connected component of containing , is topologically equivalent to .
Now assume is a connected smooth subvariety and . For any , is homeomorphic to by the local topological triviality of the pair . So there is a natural identification , where is the primitive cohomology of defined by . In particular, is constant for .
Moreover, has a natural mixed Hodge structure, since is a singular algebraic variety, see [11], Part II, Chapter 5. It turns out that and are also constant for (in most cases), see Corollary 3.6 below. Thus, we have the following well-defined map
[TABLE]
where is the corresponding flag manifold of subspaces of .
By relating the primitive cohomology with the graded pieces of the algebra and applying Theorem 1.1, we prove the following, as a generalization of [15], Chapter 3.
Theorem 1.2**.**
Assume is odd or is even. Let be a nodal hypersurface in of degree and let be a smooth subvariety of which gives an effective deformation of . Then the map above is well-defined and the differential is injective at .
Thus, loosely speaking, the infinitesimal Torelli theorem also holds for nodal hypersurfaces.
Note that for smooth hypersurfaces, the generic Torelli theorem holds, see [13], Part II, Chapter 6, Section 6.3.2, and it remains an interesting question whether this is also the case for nodal hypersurfaces. Recall that in the proof of the generic Torelli theorem for smooth hypersurfaces, the essential part is to show that a generic homogeneous polynomial can be reconstructed from its Jacobian ideal, which also holds for nodal hypersurfaces by Theorem 1.1 in [14], because a generic of degree with the associated hypersurface having a fixed number of nodes is not of Sabastiani-Thom type, which is the only exception for not to be reconstructed from ; another key ingredient in the smooth case is the symmetriser lemma, which is still open for nodal hypersurfaces.
The author would like to thank an anonymous referee, whose remarks make the exposition of this paper improved.
2. Syzygies of the Jacobian ideal
Let be the Koszul complex of with the natural grading and :
[TABLE]
where and , and the differentials are given by the wedge product with .
The homogeneous component of the cohomology group describes the syzygies
[TABLE]
with modulo the trivial syzygies generated by
[TABLE]
We may restate the main result in [5] or Theorem 9 in [6] in the following form.
Lemma 2.1**.**
Let be a nodal hypersurface in of degree and , then for any
[TABLE]
Let be such that is a smooth hypersurface. It is well-known that depends only on and , see [1], Chapter 7, Proposition 7.22. In the introduction part of [4], the following two notions are given:
[TABLE]
and
[TABLE]
They have the following relation
[TABLE]
see loc. cit.. We have the following.
Lemma 2.2**.**
Let be a nodal hypersurface in of degree and , then
[TABLE]
In particular, does not depend on the concrete equation of the polynomial for .
Proof.
We only need to check that . Indeed, by Lemma 2.1, we immediately have
[TABLE]
where the last inequality follows from and . ∎
2.3. Proof of Theorem 1.1
To prove Theorem 1.1, we first prove the following.
Lemma 2.4**.**
Assume is a nodal hypersurface in of degree and . Let such that and for all , then .
Proof.
Assume
[TABLE]
with , then
[TABLE]
Note that
[TABLE]
so by Lemma 2.1, we get for all while all these polynomials have degree , so they must all vanish identically; in particular,
[TABLE]
thus, . It follows that as desired. ∎
*Proof of Theorem 1.1: * We first remark that Theorem 1.1 holds when . In fact, in this case, and consists of constants. Since and , one sees easily that is injective.
Thus, in the sequel of the proof, we will focus on the case .
Aiming at a contradiction, we assume that there exists such that .
Then there exists a such that and is chosen to be maximal. By the maximality of , we have for all . Note that and , hence by Lemma 2.4, , contradiction.
3. Hodge theory for nodal hypersurfaces
Let be a nodal hypersurface in of degree and . The cohomology groups under consideration below all have as coefficients unless otherwise explicitly pointed out.
By the Lefschetz hyperplane theorem for singular varieties (see [9]), we have
[TABLE]
and
[TABLE]
is injective. Let
[TABLE]
be the primitive cohomology of . Then admits a mixed Hodge structure. Moreover, let be the complement of , then also admits a mixed Hodge structure and and are closely related.
3.1. Relation between and
Let be the smooth locus of and let
[TABLE]
Then has a natural mixed Hodge structure. Moreover, as is shown in [2], Chapter 6, Corollary 3.11, there is a natural residue isomorphism
[TABLE]
which is also an isomorphism of mixed Hodge structures of type .
Let be the inclusion. We have the naturally induced homomorphisms in cohomology
[TABLE]
and
[TABLE]
Moreover, are also morphisms of mixed Hodge structures. Our discussion will be divided into two cases, regarding whether is odd or even.
3.1.1. Case 1: is odd
When is odd, the variety is a -homology manifold, i.e., for any point , if and [math] otherwise. Moreover, we have the following claim.
Claim 3.2**.**
* and are both isomorphisms.*
Proof.
Indeed, we have a long exact sequence of mixed Hodge structures with respect to the pair :
[TABLE]
Let be all the nodes in , then , and furthermore, by the excision theorem
[TABLE]
since is a -homology manifold and for . Similarly, . Thus, it follows from (5) that and are both isomorphisms. ∎
Note that the weights of are since is compact while the weights of are since is smooth (see [11], p. 131, Table 5.1), hence both and have pure Hodge structures of weight and it follows from the isomorphism (4) that has a pure Hodge structure of weight .
Let
[TABLE]
Then is an isomorphism of mixed Hodge structures of type . It follows that we have isomorphisms
[TABLE]
for all . In particular, there are isomorphisms
[TABLE]
3.2.1. Case 2: is even
When is even, is no longer a -homology manifold. However, there is still an explicit description of the relations between and . Note that in this case and thus
[TABLE]
and . Moreover, there exists an exact sequence of mixed Hodge structures
[TABLE]
To make use of this exact sequence, we first give the following claim.
Claim 3.3**.**
For , has a pure Hodge structure of type for some .
Proof.
Let be the nodes in and be a small ball in around such that for .
By the excision theorem and conic structure theorem (see [2], Chapter 1, Theorem 5.1),
[TABLE]
where is the link of around ().
For each , has the homotopy type of the unit sphere bundle of tangent bundle of . Indeed, locally around , is defined as , where is the local coordinate system of centered at . Then can be described as
[TABLE]
where is small. Let
[TABLE]
and
[TABLE]
then
[TABLE]
which is the unit sphere bundle of tangent bundle of .
It follows that
[TABLE]
Note also that admits a natural mixed Hodge structure. In particular,
[TABLE]
where is a pure Hodge structure of weight and
[TABLE]
is the Hodge decomposition. By the Hodge symmetry, we have
[TABLE]
It follows that there exists such that
[TABLE]
and
[TABLE]
and
[TABLE]
In particular, is pure of type .
Note that the mixed Hodge structure on depends only on the local structure of around (see [8], Theorem 3.4). Since all the ’s are nodes, is naturally isomorphic to as mixed Hodge structures for any , hence there exists such that
[TABLE]
and thus is pure of type for . ∎
By Proposition (C28) in [2], Appendix C (see also [8], Proposition 3.8) , it follows that . Thus,
[TABLE]
Moreover, by the discussions above Example 3.18 in [2], Chapter 6, has weight , namely, , and thus for
[TABLE]
Therefore, it follows from (7) that we have an isomorphism
[TABLE]
for . Furthermore, we have isomorphisms
[TABLE]
and
[TABLE]
for ; but for , we only have injections
[TABLE]
and
[TABLE]
Using the residue isomorphism (4), we denote
[TABLE]
for (and is even). Then clearly, for .
We still denote by its restriction to . Then
[TABLE]
is an isomorphism and we have an isomorphism
[TABLE]
3.3.1. Conclusion
In conclusion, no matter whether is even or odd, we always have isomorphisms
[TABLE]
and
[TABLE]
where F^{n-1}(U_{f},X_{f})=\overline{R}_{f}^{-1}\biggl{(}i_{0}^{*}(F^{n-2}H^{n-1}_{0}(X_{f}))\biggr{)} is a subspace of containing ; and .
3.4. Cohomology of
Denote by
[TABLE]
where means that the term is omitted. As is shown in [2], Chapter 6, any cohomology class in can be represented by a form
[TABLE]
with . Hence, by (8), we see that any element in can be represented by
[TABLE]
with and similarly, by (9), any element in can be represented by
[TABLE]
with .
Such results agree with [7], Theorem 2.2, where the following formulae are given
[TABLE]
for and for ,
[TABLE]
where is the saturation of , which is also equal to the radical of for a nodal hypersurface (see [4], Remark 2.2).
Putting all the discussions above in this section together, we obtain the following.
Proposition 3.5**.**
Let be a nodal hypersurface in of degree . Then
- (i)
when , there is an isomorphism
[TABLE] 2. (ii)
when , there is an isomorphism
[TABLE] 3. (iii)
when , there is an isomorphism
[TABLE] 4. (iv)
when , there is an isomorphism
[TABLE]
where is a vector subspace containing obtained via
[TABLE]
where is the isomorphism
[TABLE]
established in **[7]**, Theorem 2.2, and is obtained in (9).
In all the formulae above, denotes the residue map.
As a corollary, we have the following.
Corollary 3.6**.**
Let be a nodal hypersurface in of degree . Then
- (i)
if , the dimension
[TABLE]
depends only on . 2. (ii)
if is odd or is even, the dimension
[TABLE]
depends only on and possibly the number of nodes in .
Proof.
Note that
[TABLE]
and
[TABLE]
If , the results follow from Proposition 3.5 and Lemma 2.2, and the dimensions depend only on . When , is a -homology manifold and the Hodge numbers of depend only on and the number of nodes in , see also [3]. ∎
4. Variations of mixed Hodge structures
Let be a nodal hypersurface in of degree . When is odd, assume while when is even, assume .
4.1. Topological triviality
Recall that parameterizes all nodal hypersurfaces with the same number of nodes as . Let be a contractible smooth subvariety containing such that it gives an effective deformation for . Set
[TABLE]
which can be seen as the union of all nodal hypersurfaces parameterized by .
Then by the First Thom Isotopy Lemma (see [2], Chapter 1, Section 3), there is a homeomorphism satisfying the following commutative diagram
[TABLE]
where are natural projections. In fact, can be obtained by integrating some well-controlled stratified vector field; for a proof, see [10]. From now on, we fix such a homeomorphism.
In particular, for any , there is a canonical homeomorphism , which induces homeomorphisms and with .
Moreover, we have an induced isomorphism of groups
[TABLE]
Hence is constant for .
In addition, by Corollary 3.6, under our assumption on , the dimensions
[TABLE]
are constant with respect to . Via the identification , it follows that can be identified with , which are two subspaces of of fixed dimension. Therefore, we have the well-defined map as in (2)
[TABLE]
where is the following flag manifold
[TABLE]
When is odd, all the Hodge numbers of are constant for , and is just two components of the period map in the theory of variation of Hodge structures, see [12], Part III, Chapter 10.
4.2. Infinitesimal deformation
Now we consider the differential of . Note that a component of is the map
[TABLE]
for the properties of tangent spaces of flag manifolds, we refer to [12], Part III, Chapter 10 and for analogous treatments for smooth hypersurfaces, see [13], Part II, Chapter 6. Recall that Proposition 3.5 implies that any element in is of the form
[TABLE]
The following holds.
Lemma 4.3**.**
For , we have
[TABLE]
Its proof is a little lengthy and we postpone it to the end of this section; instead, we first derive Theorem 1.2 from Lemma 4.3.
4.4. Proof of Theorem 1.2
From Lemma 4.3 and Proposition 3.5, the image of is contained in
[TABLE]
Moreover, we get the following commutative diagram
[TABLE]
where is given in (1). is the composite , which is injective since is an effective deformation. is defined as follows: for and ,
[TABLE]
where is the isomorphism given in Proposition 3.5.
By Theorem 1.1, is injective, hence is injective. Thus it follows from (10) that is injective, hence Theorem 1.2 follows.
Remark 4.5**.**
The result is probably also true for . We exclude this case because we do not know whether the dimension or equivalently is constant for in this case.
4.6. Proof of Lemma 4.3
The proof is almost the same as that in [13], Part II, Chapter 6 where variations of smooth hypersurfaces are considered. However, to avoid any possible confusion, we give the details here.
From the topological triviality of the family , it follows that there exists a small contractible neighbourhood in , such that for any , is a deformation retract of
[TABLE]
Set
[TABLE]
Then is a deformation retract of for every . Let for
[TABLE]
be the natural inclusion, then the induced homomorphism in cohomology
[TABLE]
is an isomorphism.
The differential can be computed as follows: for any , choose a curve such that and . For any element in of the form
[TABLE]
let
[TABLE]
give an element of . Then
[TABLE]
We have
[TABLE]
where is the homomorphism induced by the map . Note that is equal to the composition
[TABLE]
Hence,
[TABLE]
Note that acting on forms is a restriction map, it follows that
[TABLE]
Therefore,
[TABLE]
Now the proof of Lemma 4.3 is complete.
Remark 4.7**.**
To prove Theorem 1.2, it is essential for us to obtain a diagram like (10). In fact, when Y. Zhao [15] proves the infinitesimal Torelli theorem for nodal surfaces, he uses such a diagram implicitly; however, he does not give any proofs. We believe that a detailed proof is indeed needed and this is a special reason why our discussions above always include the case .
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