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).
{ωI=ωi1∧⋯∧ωia|I={i1,i2⋯,ia}, with1⩽
For 1 \leqslant i,j \leqslant r and a \geqslant 1, we define
One can consider \beta_{i}^{a} as taking the residual part of a log differential form along D_{i} , and \gamma_{j}^{a} is the restriction of the D_{i} regular log differential forms to D_{i} . Obviously, \beta_{i}^{a} and \gamma_{j}^{a} are surjective and independent of the coordinate system, respectively. For simplicity, we omit the upper symbol a .
Clearly, for any log connection \nabla , the composite map (\beta_{i} \otimes Id) \circ \nabla factors through \gamma_{i}
We call the second map the residue map of \nabla along D_{i} , and denote it as {\rm Res}_{i}\left( \nabla\right).
We can generalize morphisms above to the multi-indices case as follows. For a subset I = \left\lbrace j_{1},\cdots , j_{a}\right\rbrace \subseteq \left\lbrace 1,2,\cdots, r\right\rbrace with j_{1} < j_{2} < \cdots < j_{a} , set D_{I} = \cap_{i\in I} D_{i} , and define the residue ResI of the connection \nabla along D_{I} as follows:
• Assume IC_{r}^{*}(H,\nabla)(U_s) is defined. A section \beta \in {j_{s}}_{*} IC_{r}^{*}(H,\nabla) (U_s) belongs to IC_{r}^{*}(\varepsilon,\nabla)(U_{s-1}) when the following two conditions are satisfied:
① \beta has log pole along D|_{U_{s-1}} ;
② {{\rm{Res}}_{{D_J}}}\beta \in {\rm{Im}}({{\rm{Res}}_{{D_J}}}\nabla :\varepsilon {|_{{D_J}}} \to \varepsilon {|_{{D_J}}}) \otimes \varOmega _{{D_J}/S}^{l - n + s},\; \forall J \subset I with \left| J \right| = n - s.
Then we provide a geometric description of res-intersection complex in the sequel of this section. For any subset I of \mathcal{I}, let D_{I} = \cap_{i\in I} D_{i} , D_{I}^{*}=D_{I} - \cup_{j\notin I}\left( D_{i}\cap D_{I} \right) and let D_{\emptyset}^{*}= X-D . Set theoretically, we have X ={\coprod}_{I \subset {\mathcal{I}}} {D_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 {{\text{Res}}_i}(\nabla) are bundle morphisms for all i \in \left\lbrace 1,2,\cdots,r\right\rbrace , 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 \left\lbrace 1,2,\cdots,r\right\rbrace 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 {\cal{F}} be a coherent sheaf on X . Consider the function
where k(x) = {\cal{O}}_{x}/m_{x} is the residue field at point x . If \phi is constant, then {\cal{F}} is locally free.
Proof of Proposition 2.1. Consider the reduced scheme D_{I}^{*} and its associated coherent sheaf IC^{i}_{I} = IC_{r}^{i}\left( \mathit{X},\varepsilon \right)|_{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 \phi_{IC^{i}_{I}}(x) , is constant over D_{I}^{*} .
For each x \in D_{I}^{*} , IC_{r}^{*}\left( X,\varepsilon \right)(x) is an \varOmega_{X,x}^{*} module spanned by basis
\left\lbrace \overline{\rm {Res}}_{J}(\nabla)(e) \otimes {\rm dlog}\,t_{J}| e \text{ is the fibre of } \varepsilon \text{ and } J \text{ is a subset of } I \right\rbrace,
where \overline{\rm{Res}}_{J}(\nabla) represents the restriction of {\rm {Res}}_{J}(\nabla) on fibre. Due to that {\rm Res}_i(\nabla) \;\; \text{are bundle morphisms,}\;\; \phi_{IC^{i}_{I}} is constant if we restrict it to each degree i and stratum D_{I}^{*} . Therefore, IC_{r}^{*}\left( X,\varepsilon \right)|_{{D_{I}}^{*}} is a complex of locally free sheaves.
Proof of Lemma 2.1. It is a local problem, we may assume X = {\rm{Spec}} \, A and {\cal{F}} = {\tilde{M}} , where A is a reduced commutative local ring with maximal ideal \mathfrak{m} and M is a finite A-module.
We only have to show M is a free A-module. Assume that k({\mathfrak{m}}) vector space M/{\mathfrak{m}}M has dimension n. We use Nakayama’s lemma to lift the basis for M / {\mathfrak{m}}M into a set of generators {{m}_{1}},{{m}_{2}},\cdots ,{{m}_{n}} . It is sufficient to demonstrate that mi is linearly independent. Suppose that {\sum}_{i} a_{i} m_{i} = 0, where a_{i} \in A . In addition, ai must lie in {\mathfrak{m}} for all i, because the generators m_{i} form the basis of the fibre M / {\mathfrak{m}}M. Choose {\mathfrak{q}} \in {\rm{ Spec }}\, A arbitrarily; then, the images of m_{i} in M_{\mathfrak{q}} /{\mathfrak{q}}M_{\mathfrak{q}} generate vector space. In addition, \phi is constant, implying that they are, in fact, a basis, similarly to a_{i} \in {\mathfrak{q}} for all i .
Therefore, a_{i} lies in the intersection of the prime ideals of A , which is the nilradical of A , and thus a_{i} = 0 because A is assumed to be reduced. This completes this proof.
It is interesting to investigate the case where (\varepsilon,\nabla) 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 (\varepsilon,\nabla) equipped with a flat connection via a Riemann-Hilbert correspondence over X-D . There is a canonical extension of \varepsilon to a vector bundle with a logarithmic flat connection over X , with the residue of the connection along divisor D_{i} being the log of the monodromy of the divisor (up to a scalar), which we denote as N_{i}. It can be observed that N_{i} is topologically defined.
In Refs. [4, 5], the intermediate extension complex can be fibre-wisely expressed as follows: for x \in D_I^* and a set of coordinates z_{i} , the fibre of intermediate extension complex at x is an \varOmega _{{X,x}}^{*} sub-module generated by the sections \tilde v{ \wedge _{j \in J}}\dfrac{{{\rm{d}}{z_j}}}{{{z_j}}} for v \in {N_J} \varepsilon and J \subset I. The differential map of the complex at fibre is defined as
Note that the residue of the connection \nabla_{I} is exactly (up to a scalar) the endomorphism N_{I} if it is restricted to the stratum D_{I} . 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, \varepsilon be as in the previous section. Given a coordinate system
due to that the set \left\lbrace {\rm dlog}\,t_{i} ,{\rm d}t_{k}|i \leqslant r,r+1 \leqslant k \leqslant n\right\rbrace forms a basis of the log sheaf. For subset I =\left\lbrace j_{1},\cdots , j_{a}\right\rbrace \subseteq \cal{I} with j_{1} < j_{2} < \cdots < j_{a} , let \nabla_{I}= \nabla_{j_{1}} \circ \nabla_{j_{2}} \circ \cdots \circ \nabla_{j_{a}}. We can generalize diagram (1) as follows:
In Ref. [1], the intersection complex is defined as follows:
Definition 3.1.IC^{*}\left( X,{\varepsilon} \right) is an \varOmega^{*}_{U} graded submodule of {\varOmega}_{X}^{*}\left( {\rm log} \, D \right) \otimes {\varepsilon} generated by the abelian subsheaf
where U is an open subset of X, and M = \left\lbrace 1,\;2,\;\cdots,r \right\rbrace .
Our main theorem is as as follows:
Theorem 3.1. If {\rm Res}_{i}(\nabla): \varepsilon|_{D_{i}} \rightarrow \varepsilon|_{D_{i}} are bundle morphisms for all i \in \cal{I} , then IC_r^*\left( {{{X}},\varepsilon } \right) = I{C^*}\left( {{{X}},\varepsilon } \right).
This proof makes essential use of the weight filtration of the log complex.
Definition 3.2. Weight filtration \mathit{W}_{\cdot} of the logarithmic complex is defined as follows:
where D_{(m)} is the disjoint union over subset K \subset I of cardinal m of D_{K}: = \cap_{i\in K}D_{i} , and \alpha_{m} is the natural immersion D_{(m)} \rightarrow X .
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 \nabla_{I}\omega_{I}(\varepsilon\otimes \varOmega_{X}^{a-|I|}) is contained in W^{\left| I \right|}\varOmega_{X}^{a}\left( {\rm log}\,D \right) \otimes \varepsilon. It is straightforward because the source the map \varepsilon \otimes \varOmega_{X} ^{a-|I|} is weight zero and the map \nabla_{I} \omega_{I} is of weight |I| .
Note that we have \beta_{I}( W_{\left| I \right|}\varOmega_{X}^{a}\left( {\rm log}\, D \right)) = \varOmega_{D_{I}}^{a-|I|}, hence the vertical arrow on the right is well-defined. The commutativity of the diagram follows from restricting diagram (1) on subbundle \varepsilon\otimes \varOmega_{X}^{a-|I|} \subset \varepsilon \otimes \varOmega_{D_{I}/S}({\rm log }((D-\sum_{i\in I}D_{i})|_{D_{1}}). 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
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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Schmid W. Variation of Hodge structure: The singularities of the period mapping. Inventiones Mathematicae,1973, 22 (3): 211–319. DOI: 10.1007/BF01389674
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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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Voisin C. Hodge Theory and Complex Algebraic Geometry I. Cambridge, UK: Cambridge University Press, 2003.
Yaseen, B., Gangwar, C., Nayak, R. et al. Cannabis sativa mediated palladium nanoparticles as an effective nanodrug against multi-drug resistant bacteria and A549 lung cancer cells. Inorganic Chemistry Communications, 2023.
DOI:10.1016/j.inoche.2023.111254
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.
Yaseen, B., Gangwar, C., Nayak, R. et al. Cannabis sativa mediated palladium nanoparticles as an effective nanodrug against multi-drug resistant bacteria and A549 lung cancer cells. Inorganic Chemistry Communications, 2023.
DOI:10.1016/j.inoche.2023.111254