Xiaojin Lin is currently a graduate student under the tutelage of Prof. Mao Sheng at the University of Science and Technology of China. His research interests focus on Hodge theory and vector bundle
We provide an intrinsic algebraic definition of the intersection complex for a variety.
Graphical Abstract
A normal crossing divisor gives rise to a stratification of a smooth scheme, and a logarithmic connection of a vector bundle along the divisor induces residue maps along each stratums.
Abstract
We provide an intrinsic algebraic definition of the intersection complex for a variety.
Public Summary
We provide an intrinsic definition of intersection subcomplex via these residues.
Intersection homology theory is a generalization of singular homology for singular algebraic varieties. In Ref. [1], Sheng and Zhang established a positive characteristic analog of an intersection cohomology theory for polarised variations of Hodge structures and proposed an algebraic definition of the intersection complex, but with the help of coordinate systems. Here, we provide an intrinsic definition of the intersection complex via residues and provide a geometric description of it.
The remainder of this paper is organized as follows. Section 2 establishes notations and presents key definitions. Section 3 provides the main theorem and its proof. Finally, in Section 4, an explicit computation following the spirit of proof in surface case is made, and a counterexample is discussed.
2.
Intersection complex
Let (X,D) be a smooth scheme over a regular locally Noetherian scheme S with a reduced smooth normal crossing divisor D=∑i∈IDi, where I is a finite index set, and ε be a locally free coherent sheaf with an integrable logarithmic λ-connection ∇ along D.
We introduce some natural morphisms of log-differential sheaves before providing our definitions.
Suppose X is of relative dimension n over S. Owing to smoothness of X and the definition of simple normal crossing divisors, for any x∈X, there exists a neighborhood U of x such that we can find a coordinate system (t1,⋯,tr;tr+1,⋯,tn) such that D∩U is defined by the equation t1⋅t2⋯tr=0. As an immediate result, Ω1U/S(logD) admits an OU basis
{ω1=dlogt1,⋯,ωr=dlogtr;ωr+1=dtr+1,⋯,ωn=dtn}.
Moreover, it induces a free system of generators for ΩaU/S(logD).
One can consider βai as taking the residual part of a log differential form along Di, and γaj is the restriction of the Di regular log differential forms to Di. Obviously, βai and γaj are surjective and independent of the coordinate system, respectively. For simplicity, we omit the upper symbol a.
Clearly, for any log connection ∇, the composite map (βi⊗Id)∘∇ factors through γi
εγi⟶ODi⊗ε⟶ODi⊗ε.
We call the second map the residue map of ∇ along Di, and denote it as Resi(∇).
We can generalize morphisms above to the multi-indices case as follows. For a subset I={j1,⋯,ja}⊆{1,2,⋯,r} with j1<j2<⋯<ja, set DI=∩i∈IDi, and define the residue ResI of the connection ∇ along DI as follows:
then the following descending chain gives rise to a stratification of X:
Xn:=X⊃Xn−1⊃⋯⊃Xn−|I|⊃Xn−|I|−1=∅.
And let js:Us:=X−Xs→Us−1=X−Xs−1 be the natural inclusion for n−|I|⩽s⩽n−1.
Definition 2.1. Notations as above. We inductively define res-intersection complex ICr as follows:
• IC∗r(ε,∇)|Un−1=IC∗r(ε,∇)|Un−1;
• Assume IC∗r(H,∇)(Us) is defined. A section β∈js∗IC∗r(H,∇)(Us) belongs to IC∗r(ε,∇)(Us−1) when the following two conditions are satisfied:
① β has log pole along D|Us−1;
② ResDJβ∈Im(ResDJ∇:ε|DJ→ε|DJ)⊗Ωl−n+sDJ/S,∀J⊂I with |J|=n−s.
Then we provide a geometric description of res-intersection complex in the sequel of this section. For any subset I of I, let DI=∩i∈IDi, D∗I=DI−∪j∉I(Di∩DI) and let D∗∅=X−D. Set theoretically, we have X=∐I⊂ID∗I. Each D∗I is a locally closed subspace of X, and thus we can endow D∗I with reduced subscheme structure.
Proposition 2.1. If Resi(∇) are bundle morphisms for all i∈{1,2,⋯,r}, then the res-intersection complex is a complex of locally free sheaves if it is restricted to each stratum D∗I, where I is an index subset of {1,2,⋯,r} and D∗I is endowed with a reduced subscheme structure.
We employ the following lemma to prove Proposition 2.1, see Ref. [2] for details.
Lemma 2.1. Let X be a reduced Noetherian scheme, and let F be a coherent sheaf on X. Consider the function
ϕF(x)=dimk(x)Fx⊗Oxk(x),
where k(x)=Ox/mx is the residue field at point x. If ϕ is constant, then F is locally free.
Proof of Proposition 2.1. Consider the reduced scheme D∗I and its associated coherent sheaf ICiI=ICir(X,ε)|D∗I. Because of the assumption the divisors are reduced, Lemma 2.1, the proposition is proven if we can show that the dimension of the fibre of sheaf, which is ϕICiI(x), is constant over D∗I.
For each x∈D∗I, IC∗r(X,ε)(x) is an Ω∗X,x module spanned by basis
{¯ResJ(∇)(e)⊗dlogtJ|e is the fibre of ε and J is a subset of I},
where ¯ResJ(∇) represents the restriction of ResJ(∇) on fibre. Due to that Resi(∇)are bundle morphisms,ϕICiI is constant if we restrict it to each degree i and stratum D∗I. Therefore, IC∗r(X,ε)|DI∗ is a complex of locally free sheaves.
Proof of Lemma 2.1. It is a local problem, we may assume X=SpecA and F=˜M, where A is a reduced commutative local ring with maximal ideal m and M is a finite A-module.
We only have to show M is a free A-module. Assume that k(m) vector space M/mM has dimension n. We use Nakayama’s lemma to lift the basis for M/mM into a set of generators m1,m2,⋯,mn. It is sufficient to demonstrate that mi is linearly independent. Suppose that ∑iaimi=0, where ai∈A. In addition, ai must lie in m for all i, because the generators mi form the basis of the fibre M/mM. Choose q∈SpecA arbitrarily; then, the images of mi in Mq/qMq generate vector space. In addition, ϕ is constant, implying that they are, in fact, a basis, similarly to ai∈q for all i.
Therefore, ai lies in the intersection of the prime ideals of A, which is the nilradical of A, and thus ai=0 because A is assumed to be reduced. This completes this proof.
It is interesting to investigate the case where (ε,∇) comes from the polarized variation of Hodge structures. Let us consider a quick recall of this (cf. Ref. [3]). If X is a complex variety, and E is a local system over X−D underlies a polarized variation of Hodge structures, then we obtain a vector bundle (ε,∇) equipped with a flat connection via a Riemann-Hilbert correspondence over X−D. There is a canonical extension of ε to a vector bundle with a logarithmic flat connection over X, with the residue of the connection along divisor Di being the log of the monodromy of the divisor (up to a scalar), which we denote as Ni. It can be observed that Ni is topologically defined.
In Refs. [4, 5], the intermediate extension complex can be fibre-wisely expressed as follows: for x∈D∗I and a set of coordinates zi, the fibre of intermediate extension complex at x is an Ω∗X,x sub-module generated by the sections ˜v∧j∈Jdzjzj for v∈NJε and J⊂I. The differential map of the complex at fibre is defined as
d(˜v⊗dlogtI)=∑(Ni(v)⊗dlogti)∧dlogtI.
Note that the residue of the connection ∇I is exactly (up to a scalar) the endomorphism NI if it is restricted to the stratum DI. It can be easily seen that the res-intersection complex coincides with the intermediate extension complex. From this perspective, we provide an algebraic definition of the intermediate extension complex.
3.
Main theorem
In the following, we show that the res-intersection subcomplex above coincides with the intersection subcomplex defined in Ref. [1].
Let X,D,ε be as in the previous section. Given a coordinate system
{t1,t2,⋯,tr;tr+1,⋯,tn}
of U, locally we can write
∇=∑i⩽r∇idlogti+∑k>r∇kdtk,
due to that the set {dlogti,dtk|i⩽r,r+1⩽k⩽n} forms a basis of the log sheaf. For subset I={j1,⋯,ja}⊆I with j1<j2<⋯<ja, let ∇I=∇j1∘∇j2∘⋯∘∇ja. We can generalize diagram (1) as follows:
Proof. It is a basic fact of weight filtration, for a rigorous proof of this lemma the reader is referred to Refs. [6, 7] .
Firstly, one have to verify that the upper arrow is well defined. That is, one have to show ∇IωI(ε⊗Ωa−|I|X) is contained in W|I|ΩaX(logD)⊗ε. It is straightforward because the source the map ε⊗Ωa−|I|X is weight zero and the map ∇IωI is of weight |I|.
Note that we have βI(W|I|ΩaX(logD))=Ωa−|I|DI, hence the vertical arrow on the right is well-defined. The commutativity of the diagram follows from restricting diagram (1) on subbundle ε⊗Ωa−|I|X⊂ε⊗ΩDI/S(log((D−∑i∈IDi)|D1). It remains to show Eq. (6). It is easy to see the sheaf on right side is contained in left side. By the commutativity of diagram (1) again, one has the left side of Eq. (6) is contained in
(ResI(∇))(ε|DI)⊗ΩDI/S(log((D−∑i∈IDi)|D1).
Therefore, Eq. (6) follows from the following claim.
Claim. If ResI is a bundle morphism, then we have the following equation:
For the "\supseteq" direction, it is obvious. For the other direction, the sheaf {\rm Res}_{I}(\nabla)(\varepsilon|_{D_{I}}) is locally free due to the assumption that {\rm Res}_{I} is a bundle morphism, thus it has no torsion along D_{j} \cap D_{I} , where j\in {\cal{I}} - I. This completes the proof of the claim.
Remark 3.1. The first sublemma illustrates that weight equals to the number of times of the irreducible components of the divisor intersect (in other words, the depth of the stratification). The second provides a local description of the weight filtration along divisor in terms of the coordinates.
We now return to the proof of the main theorem.
Proof of Theorem 3.1.Without loss of generality, we assume that r = n .
Clearly, we have IC^{*}\left( \mathit{X},\varepsilon \right) \subset IC_{r}^{*}\left( \mathit{X},\varepsilon \right), because the restriction of \nabla_{i} on D_{i} is exactly the residue map {\rm Res}_{i}.
Conversely, we consider any s \in IC_{r}^{*} \left( \mathit{X},\varepsilon \right) \left( U\right) \bigcap \varOmega_{X}^{a}\left( {\rm log}\, D\right) \otimes \varepsilon\left( U\right). Taking a = |I| in the diagram (5), we will obtain a section e \in \varepsilon (U) such that {\rm Res}_{I} \circ \gamma_{I} (e) = \beta_{I}(s), by the comutitivity of the diagram we have s-\nabla_{I}(e)\otimes \omega_{I} \in \varepsilon \otimes \ker \beta_{I}, and we denote it as s_{1} . Taking m = a in the exact sequence (4), we know that \ker\beta_{I} is equal to W^{a-1}(\varOmega_{X}^{a}\left( {\rm log}\, D \right) ); hence, s_{1} \in \varepsilon \otimes W^{a-1}(\varOmega_{X}^{a}\left( {\rm log}\, D \right) ).
Replacing s with s_{1} , by the definition of res-intersection complex, one has l_{I}\otimes\beta_{I}(s_{1}) \in {\rm Im}({\rm Res}_{D_I}\nabla:\varepsilon|_{D_I}\to \varepsilon|_{D_I}) \otimes \varOmega_{D_{I}/S}^{a} \left({\rm log }\left( D-\sum_{i \in I}D_{i} \right)\vert_{D_{I}} \right) and one has s_{1} \in \varepsilon \otimes W^{a-1}(\varOmega_{X}^{a}\left( {\rm log}\, D \right) ) by the construction. Then we can chase in the diagram (5) for index set I with |I|=a-1 , by Eq. (6), we obtain a section e_{I} \in \varepsilon \otimes \varOmega_{X/S}^{a-1} such that s_{1}-\nabla_{I}(e_{I})\omega_{I} \in \varepsilon \otimes \ker \beta_{I}, therefore, we have
where I is a of cardinal (a-1) . Therefore, we have s_{2} \in W^{a-2}(\varOmega_{X}^{a}\left( {\rm log}\, D \right) )\otimes \varepsilon by (4).
Repeat the processes above a times, we obtain s_{a} \in \varepsilon \otimes W^{0}=\varOmega_{X}^{a} \otimes E and e_{I} \in \varepsilon \otimes \varOmega_{X/S}^{a-|I|} with I \subseteq \cal{I} , satisfying
which implies s \in IC(X,\varepsilon) \bigcap \varOmega_{X}^{a}\left( {\rm log}\, D\right) \otimes \varepsilon. This completes our proof.
4.
Surface case
In this section, we provide an explicit calculation for the surface case and present an example to the main theorem without bundle morphism conditions.
Let X ={\rm{ Spec }}(k[t_{1},t_{2}]) be a surface and let D=D_{1}+D_{2} defined by t_{1}t_{2}=0 . The divisor gives rise to a stratification the surface as X=D_{\emptyset}^{*} \coprod D_{1}^{*} \coprod D_{2}^{*} \coprod D_{12}^{*}. With the help of the coordinates t_{i} , we can write \nabla=\nabla_{1} {\rm dlog} \, t_{1} + \nabla_{2} {\rm dlog} \, t_{2}.
① IC_{r}^{0}\left( X,\varepsilon \right) = IC^{0}\left( X,\varepsilon \right), because both are equal to \varepsilon.
② In the one-degree term, note that the sections of the sheaf IC^{1}\left( X,\varepsilon \right) are of the form:
Let s \in IC\left( X,\varepsilon \right)^{1}(X). To verify s\in IC_{c}^{1}\left( X,\varepsilon \right), we aim to find e_{1} and e_{2} . By definition, s satisfies \beta_{i}(s) \in {\rm Im}\left( {\rm Res}_{D_{i}} \right): Consider a commutative diagram
The first vertical arrow is surjective, so we can find a section e_{1} \in \varepsilon such that s-\nabla(e_{1}){\rm dlog}\,t_1 in the kernel of the second vertical, which is \varepsilon \otimes \varOmega_{X}^{1} \left( {\rm log} \left( D_{2} \right) \right), replacing 1 with 2 , and we obtain a section e_{2} of \varepsilon, by the exact sequence (4), s_{1} = s-( \nabla_{1}(e_{1}) {\rm dlog} \, t_{1}+\nabla_{2}(e_{2}) {\rm dlog} \,t_{2}) is of weight zero. In other words, it is regular, which allows us to write:
s = \nabla_{1}(e_{1}) {\rm dlog}\, t_{1}+\nabla_{2}(e_{2}) {\rm dlog}\,t_{2}+f_{1}{\rm d}t_{1}+f_{2}{\rm d}t_{2},
where e_{1},e_{2},f_{1},f_{2} \in \varepsilon(\mathit{U}).
③ Using the same pattern, a section \omega in IC^{2}\left( X,\varepsilon \right)(X) is of the form
by definition. For any section s \in IC_{r}^2(X, \varepsilon )(X), we aim to get section e_{12}, e_{1}, e_{2}, f. By (5), we have the following commutative diagram:
where both vertical arrows are surjective, we obtain e_{12} \in \varepsilon such that s_{1}: = s - ( \nabla(e_{12}) ) \omega_{12} \in \ker \varepsilon\otimes \beta_{12}, which is of weight one by short exact sequence (4).
Then consider diagram (5) and set a = 2 , I = \left\lbrace1,2 \right\rbrace. Using the same argument as above, we obtain \tilde{e}_{1} \text{ and } \tilde{e}_{1} \in \varepsilon \otimes \varOmega_{X}^{1}, such that s_{1}- \nabla_{1}(e_{1}) {\rm dlog}\,t_{1} \wedge {\rm d}t_{2}-\nabla_{2}(e_{2}) {\rm dlog}\,t_{2}\wedge {\rm d}t_{1} in \ker ( \beta_{2} \;\oplus\; \beta_{2}) , which is exactly \varOmega_{X}^{2}\otimes \varepsilon by (4). Therefore, e_{12},e_{1},e_{2},f are the section we want. This completes our proof.
In the sequel of the section we will present an example, which is provided by Zebao Zhang, to show that the main theorem will be wrong if the residue morphisms are not assumed to be bundle morphisms. Let k be a perfect field of character p , (X,D) is as above. Define logarithmic connection over
One can see that {\rm{Res}}_{1}(\nabla) has torsion at t_{2}=0 , hence it is not a bundle morphism. By definition, we have IC^{2}=(t_{2}^{p} \cdot {\rm{dlog}}\, t_{1} \wedge {\rm{d}}t_{2}) {\cal{O}}_{X} + ({\rm{d}}t_{1} \wedge {\rm{d}}t_{2})\cal{O}_{X}. Consider the section t_{2}^{p} {\rm dlog }\,t_{1} \wedge {\rm dlog }\,t_{2}, it is a section in IC_{r}^{2} but not in IC^{2} .
Acknowledgements
I would especially like to thank Prof. Mao Sheng for his suggestions. And I would also like to thank Dr. Zebao Zhang for correcting the article.
Conflict of interest
The author declares that he has no conflict of interest.
Conflict of Interest
The authors declare that they have no conflict of interest.
We provide an intrinsic definition of intersection subcomplex via these residues.
We present its explicit geometric description.
Sheng M, Zhang Z. On the decomposition theorem for intersection de Rham complexes. [2021-11-10]. https://arxiv.org/abs/1904.06651.
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Kashiwara M, Kawai T. Poincare lemma for a variation of polarized Hodge structure. In: Hodge Theory. Berlin: Springer, 1987.
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Cattani E, Kaplan A, Schmid W. L2 and intersection cohomologies for a polarizable variation of Hodge structure. Inventiones Mathematicae,1987, 87: 217–252. DOI: 10.1007/BF01389415
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Peters C, Steenbrink J. Mixed Hodge Structures. Berlin: Springer, 2008.
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Sheng M, Zhang Z. On the decomposition theorem for intersection de Rham complexes. [2021-11-10]. https://arxiv.org/abs/1904.06651.
[2]
Hartshorne R. Algebraic Geometry. Berlin: Springer, 1975.
[3]
Schmid W. Variation of Hodge structure: The singularities of the period mapping. Inventiones Mathematicae,1973, 22 (3): 211–319. DOI: 10.1007/BF01389674
[4]
Kashiwara M, Kawai T. Poincare lemma for a variation of polarized Hodge structure. In: Hodge Theory. Berlin: Springer, 1987.
[5]
Cattani E, Kaplan A, Schmid W. L2 and intersection cohomologies for a polarizable variation of Hodge structure. Inventiones Mathematicae,1987, 87: 217–252. DOI: 10.1007/BF01389415
[6]
Peters C, Steenbrink J. Mixed Hodge Structures. Berlin: Springer, 2008.
[7]
Voisin C. Hodge Theory and Complex Algebraic Geometry I. Cambridge, UK: Cambridge University Press, 2003.