Weighted Hodge ideals of reduced divisors

Sebastian Olano

A. Introduction

In this paper, we continue the study of weighted Hodge ideals that started in [olano22a], where the focus was the -th weighted Hodge ideals, also called weighted multiplier ideals. We show that several results satisfied by the weighted multiplier ideals can be generalized under suitable conditions.

for all p≥0p\geq 0. Consequently, we can define the Hodge ideal Ip(D)I_{p}(D) by

The DX\mathscr{D}_{X}-module OX(∗D)\mathscr{O}_{X}(*D) is also endowed with a weight filtration W∙OX(∗D)W_{\bullet}\mathscr{O}_{X}(*D) by DX\mathscr{D}_{X}-submodules. The Hodge filtration of these submodules satisfies

and similarly we can define the weighted Hodge ideals by

The weighted Hodge ideals form a chain of inclusions

We can always understand the two extreme ideals in this chain. The first element in the list admits an easy description:

On the other end, the last ideal in this chain is the usual pp-th Hodge ideal, that is,

Unlike IpW0(D)I_{p}^{W_{0}}(D), for all the other degrees, the support of the scheme defined by IpWl(D)I_{p}^{W_{l}}(D) is contained in the singular locus of DD.

Birational definition We give an alternative description of the weighted Hodge ideals in terms of a resolution of singularities. Let f:Y→Xf:Y\to X be a resolution of singularities of the pair (X,D)(X,D) which is an isomorphism over X∖DX\setminus D, and let E:=(f∗D)redE:=(f^{*}D)_{\rm red}. This description stems from the birational definition of Hodge ideals in [hodgeideals]*§9, and uses right D\mathscr{D}-modules. The DY\mathscr{D}_{Y}-module ωY(∗E)\omega_{Y}(*E) admits a filtered resolution by DY\mathscr{D}_{Y}-modules given by

Similarly, using the weight filtration on the sheaves of logarithmic pp-forms (see (1.4)), we show that the complex

is filtered quasi-isomorphic to the DX\mathscr{D}_{X}-module Wn+lω(∗E)W_{n+l}\omega(*E) (see Proposition 4.1).

The DX\mathscr{D}_{X}-module ωX(∗D)\omega_{X}(*D) can be described using the filtered resolution of ωY(∗E)\omega_{Y}(*E) described above. More precisely, we can define the complex A∙A^{\bullet} by

placed in degrees −n,…,0-n,\ldots,0, and we have that,

(see [hodgeideals]*§9). To give the alternative description of the weighted Hodge ideals, we introduce the complex Cl,p−n∙C^{\bullet}_{l,p-n} defined as

is precisely Fp−nWn+lωX(∗D)=IpWl(D)⊗ωX((p+1)D)F_{p-n}W_{n+l}\omega_{X}(*D)=I^{W_{l}}_{p}(D)\otimes\omega_{X}((p+1)D) (see Proposition 4.3).

Let XX be a smooth complex variety and DD a reduced divisor defined by a regular function f∈OX(X)f\in\mathscr{O}_{X}(X). Then,

The proof is based on two ideas. First, we can relate the Hodge filtration of V1i+OXV^{1}i_{+}\mathscr{O}_{X} with that of OX(∗D)\mathscr{O}_{X}(*D) (see 5.2). Second, the weight filtration on the nearby cycles sheaf can be related to that of the local cohomology sheaf (Proposition 5.3). This is enough to understand all the weighted Hodge ideals in the case when DD only has isolated weighted-homogeneous singularities (see Remark 5.7).

The description in Theorem A is useful to relate the weighted Hodge ideals with some invariants of the singularities, like the minimal exponent. Recall that to the variety D⊆XD\subseteq X we can associate the Bernstein-Sato polynomial bD(s)b_{D}(s). The polynomial (s+1)(s+1) divides bD(s)b_{D}(s), and we denote bD~(s)=bD(s)/(s+1)\widetilde{b_{D}}(s)=b_{D}(s)/(s+1). The negative of the largest root of bD~(s)\widetilde{b_{D}}(s) is called the minimal exponent of a DD and is denoted αD~\widetilde{\alpha_{D}}. This invariant encodes important properties of the singularities of DD. For instance, it is a refined version of the log-canonical threshold, since lct(X,D)=min⁡{αD~,1}lct(X,D)=\min\{\widetilde{\alpha_{D}},1\}. In particular, this implies that (X,D)(X,D) is log-canonical if and only if αD~≥1\widetilde{\alpha_{D}}\geq 1. Moreover, it is a result of Saito that DD has rational singularities if and only if αD~>1\widetilde{\alpha_{D}}>1.

The notions of log-canonicity and rationality can be described in terms of weighted Hodge ideals. Recall that 0-th weighted Hodge ideals, or weighted multiplier ideals, form a sequence of ideals interpolating between the adjoint ideal and a multiplier ideal. This is the case, as I0W1(D)=adj⁡(D)I_{0}^{W_{1}}(D)=\operatorname{adj}(D) (see for instance [olano22a]*Theorem A) and I0(D)=J((1−ε)D)I_{0}(D)=\mathcal{J}((1-\varepsilon)D) for 0<ϵ≪10<\epsilon\ll 1 [budursaito05]. These two ideals identify if a singularity is respectively rational or log-canonical. We give an analogous description for the higher weighted Hodge ideals. The Hodge ideal Ip(D)I_{p}(D) is trivial if and only if αD~≥p+1\widetilde{\alpha_{D}}\geq p+1, in which case we say that (X,D)(X,D) is pp-log-canonical. Also, the weighted Hodge ideal IpW1(D)I_{p}^{W_{1}}(D) is trivial if and only if αD~>p+1\widetilde{\alpha_{D}}>p+1 (see Corollary 5.10), which some authors referred to as DD being pp-rational. The rest of the pp-weighted Hodge ideals filter and measure the “distance” between (X,D)(X,D) having pp-log-canonical singularities and DD being pp-rational.

Isolated singularities. Recall that the weighted Hodge ideals satisfy

The difference between the two ideals can be described by the coherent sheaf Fpgr⁡n+lWOX(∗D)F_{p}\operatorname{gr}^{W}_{n+l}\mathscr{O}_{X}(*D) (see (6.1)). If DD has isolated singularities, we give a description of the dimension of this sheaf at the singular points in terms of a resolution of singularities. For this, possibly after restricting to an open set, assume DD has one isolated singularity x∈Dx\in D. In this case, there exists a pure Hodge structure HlH_{l} for l≥2l\geq 2, such that the dimension of their Hodge pieces describes the desired dimension. More concretely,

(see §6 for more details). For this reason, to find the difference between two consecutive weighted Hodge ideals, it is enough to compute the dimensions of the spaces Gr⁡Fn−pHl\operatorname{Gr}_{F}^{n-p}H_{l}.

Let g:D~→Dg:\widetilde{D}\to D be a log-resolution of singularities that is an isomorphism outside of xx. Let G⊆D~G\subseteq\widetilde{D} be the exceptional divisor. Then

When p=0p=0 the second summand in the description of dim⁡(Gr⁡Fn−pH2)\dim(\operatorname{Gr}_{F}^{n-p}H_{2}) is 0 because the dimension of GG is n−2n-2, and therefore these dimensions are described as Hodge numbers of the middle cohomology of GG. For p≥1p\geq 1 we cannot expect this term to be 0 in general, but this dimension admits a geometric interpretation (see Remark 6.8).

Vanishing results. Weighted Hodge ideals satisfy global results under suitable conditions. Let XX be a smooth projective variety and DD an ample divisor with at most isolated singularities. Under this assumptions, when p=0p=0 we have that

for i≥1i\geq 1 and l≥2l\geq 2 [olano22a]*Theorem E. To generalize this result for all p≥1p\geq 1, we require the condition that Ip−1Wl(D)=OXI_{p-1}^{W_{l}}(D)=\mathscr{O}_{X}.

Let XX be a smooth projective variety of dimension nn, and DD an ample reduced effective divisor with at most isolated singularities. Suppose that Ip−1W1(D)I_{p-1}^{W_{1}}(D) is trivial. Then

If Hj(X,ΩXn−j((p−j+1)D))=0H^{j}(X,\Omega_{X}^{n-j}((p-j+1)D))=0 for all 1≤j≤p1\leq j\leq p, then

When l=1l=1 and i=1i=1 the vanishing does not hold in general. For an example see Remark 7.2. A Kodaira-type vanishing result is also satisfied for all l≥1l\geq 1, and the proof is based on a vanishing result by Saito [saito90]*Proposition 2.33 (see Proposition 8.1).

for k≥(p+1)d−n−1k\geq(p+1)d-n-1 if l≥2l\geq 2, and k≥(p+1)d−nk\geq(p+1)d-n if l≥1l\geq 1.

This result gives a bound on a certain type of isolated singularities we describe next. For simplicity, suppose DD has at most one isolated singularity x∈Dx\in D, and assume αD~=p+1\widetilde{\alpha_{D}}=p+1. We describe first the case p=0p=0. This case corresponds to a log-canonical and not rational singularity. In this case, according to (0.1), the length of the scheme described by I0W1(D)I_{0}^{W_{1}}(D) is determined by Gr⁡F0(Hn−2(G))\operatorname{Gr}_{F}^{0}(H^{n-2}(G)), using the notation of Theorem B. Ishii proved that in this case, dim⁡(Gr⁡F0(Hn−2(G)))=1\dim(\operatorname{Gr}_{F}^{0}(H^{n-2}(G)))=1 [ishii85]*Proposition 3.7. This means that the ideal I0W1(D)I_{0}^{W_{1}}(D) is the maximal ideal of xx in XX, and that there exists exactly one degree l≥2l\geq 2 such that

while the dimension for the other degrees is 0. A log-canonical singularity is of type (0,n−l)(0,n-l) in this case [ishii85]*Definition 4.1.

for l≥2l\geq 2 and 0≤r≤p−10\leq r\leq p-1 by (0.1) and Theorem B. Moreover, by the same results, we know that there exists exactly one degree l≥2l\geq 2 such that

while the dimension for all the other degrees is 0. Related invariants in similar conditions have been studied by Friedman and Laza in [friedmanlaza22b]*Theorem 6.11 and Corollary 6.14.

Restriction theorem. Finally, we study the behavior of weighted Hodge ideals of a pair (X,D)(X,D) under the restriction of a hypersurface of XX. Let H⊆XH\subseteq X be a smooth hypersurface, and DHD_{H} the restriction of DD to HH. If DHD_{H} is reduced, then we can also consider the pair (H,DH)(H,D_{H}) and their respective weighted Hodge ideals.

Let XX be a smooth variety and DD an effective reduced divisor. Let H⊆XH\subseteq X be a smooth divisor such that H⊊Supp⁡(D)H\subsetneq\operatorname{Supp}(D) and D_{H}=D\big{|}_{H} is reduced. Then, for every p≥0p\geq 0 and l≥0l\geq 0 we have

Moreover, if HH is general, then we have an equality.

This is the analogue of the Restriction Theorem for Hodge ideals [mustatapopa18]*Theorem A, and for multiplier ideals [lazarsfeld2]*Theorem 9.5.1.

Acknowledgements. I would like to thank Mircea Mustaţă and Mihnea Popa for their constant support and many conversations during the project. I am also very grateful to the anonymous referees for their feedback on improving the presentation of the article and for suggesting a simpler proof of Lemma 5.4, explained in Remark 5.5.

B. Preliminaries

In this section, we recall some facts about mixed Hodge modules and set up the notation we use throughout this paper.

Let XX be a smooth variety of dimension nn. Mixed Hodge modules introduced by Saito in [saito88] are the main object used throughout this article. For a graded-polarizable mixed Hodge module MM, we denote the underlying left regular holonomic DX\mathscr{D}_{X}-module by M\mathcal{M}. In some contexts, it is more useful to use right DX\mathscr{D}_{X}-modules. Recall that if M\mathcal{M} is a left DX\mathscr{D}_{X}-module, the corresponding right DX\mathscr{D}_{X}-module is M⊗OXωX\mathcal{M}\otimes_{\mathscr{O}_{X}}\omega_{X}, where ωX\omega_{X} is the canonical sheaf. We mostly use left D\mathscr{D}-modules, and in case we are using right D\mathscr{D}-modules instead, we will say it explicitly.

A mixed Hodge module MM is endowed with a weight filtration, which we denote by W∙MW_{\bullet}M, and

is the quotient, which is a polarizable Hodge module of weight ll. We denote by F∙MF_{\bullet}\mathcal{M} the Hodge filtration. The de Rham complex is defined as:

and the Hodge filtration of M\mathcal{M} induces a filtration on this complex:

The pp-th subquotient of this filtration is the complex

(see for example [hodgeideals]*Lemma 2.2). Since EE is a simple normal crossings divisor, the weight filtration of the DY\mathscr{D}_{Y}-module OY(∗E)\mathscr{O}_{Y}(*E) can be described in terms of the intersections of its irreducible components. The lowest degree of the weight filtration is n=dim⁡Yn=\dim{Y}, that is:

The lowest piece corresponds to the canonical Hodge module of YY:

To describe the rest of the subquotients, we introduce the following very useful notation. Let

with EJ=⋂j∈JEjE_{J}=\displaystyle\bigcap_{j\in J}E_{j}, is a smooth and possibly disconnected variety. We denote il:E(l)→Yi_{l}:E(l)\to Y the map such that on each component is the inclusion. We have that

In order to describe the weight filtration of a pushforward of a projective morphism, a useful tool is to use the spectral sequence associated to the weight filtration:

which degenerates at E2E_{2}, and there is an isomorphism:

Finally, recall that the sheaf of pp-forms with logarithmic poles along EE denoted by ΩYp(log⁡E)\Omega^{p}_{Y}(\log{E}) are endowed with a weight filtration. This increasing filtration consists of subsheaves

such that if z1,…,znz_{1},\ldots,z_{n} are local coordinates on an open set VV, and EE is given by the equation

then in VV, WlΩp(log⁡E)W_{l}\Omega^{p}(\log{E}) is a OV\mathscr{O}_{V} module generated by elements of the form

with il≤ri_{l}\leq r and s≤ks\leq k (see [elzeinetal]*3.4.1.2 for more details). For I={i1,…,is}I=\{i_{1},\ldots,i_{s}\} and J={j1,…,jp−s}J=\{j_{1},\ldots,j_{p-s}\} we use the notation

C. Characterizations

In this section, we introduce weighted Hodge ideals using the theory of mixed Hodge modules.

A fundamental result by Saito about the Hodge filtration on OX(∗D)\mathscr{O}_{X}(*D) states that

(see [saito93]*Proposition 0.9). The definition of Hodge ideals follows from this result. These ideals are denoted by Ip(D)I_{p}(D), and are defined using the formula

(see [hodgeideals]*Definition 9.4). In this article, we study weighted Hodge ideals which are defined similarly using the weight filtration with which OX(∗D)\mathscr{O}_{X}(*D) is endowed. The Hodge filtration of the sub-DX\mathscr{D}_{X} modules Wn+lOX(∗D)W_{n+l}\mathscr{O}_{X}(*D) satisfies

Let XX be a smooth complex variety and DD a reduced divisor. For l≥0l\geq 0 and p≥0p\geq 0, we define the ideal sheaf IpWl(D)I_{p}^{W_{l}}(D) on XX by the formula

We call IpWl(D)I_{p}^{W_{l}}(D) the ll-th weighted pp-th Hodge ideal of DD.

for all p≥0p\geq 0. Indeed, the weight filtration of OX(∗D)\mathscr{O}_{X}(*D) is an increasing filtration, hence

Simple normal crossings divisor

Weighted Hodge ideals can be described completely when the reduced divisor DD has simple normal crossings. In this case, the Hodge filtration of OX(∗D)\mathscr{O}_{X}(*D) is fully understood, and from this information we can deduce the Hodge filtration of Wn+lOX(∗D)W_{n+l}\mathscr{O}_{X}(*D).

Let DD be a simple normal crossings divisor. In this case, the Hodge filtration of OX(∗D)\mathscr{O}_{X}(*D) admits a simple description:

if p≥0p\geq 0, and 0 otherwise. Using this, one obtains a local description of the Hodge ideals. Let x1,…,xnx_{1},\ldots,x_{n} be coordinates around z∈Xz\in X, such that DD is defined by (x1⋯xr=0)(x_{1}\cdots x_{r}=0). For every p≥0p\geq 0, the ideal Ip(D)I_{p}(D) is generated around zz by

[hodgeideals]*Proposition 8.2. Weighted Hodge ideals of DD admit a similar local description.

Let x1,…,xnx_{1},\ldots,x_{n} be coordinates around z∈Xz\in X, such that DD is defined by (x1⋯xr=0)(x_{1}\cdots x_{r}=0). Then, for every p≥0p\geq 0 and l≤rl\leq r, IpWl(D)I_{p}^{W_{l}}(D) is generated around zz by

where I={1,…,r}I=\{1,\ldots,r\}. For l≥rl\geq r, IpWl(D)=Ip(D)I_{p}^{W_{l}}(D)=I_{p}(D) around zz.

The Hodge filtration of Wn+lOX(∗D)W_{n+l}\mathscr{O}_{X}(*D) also admits a simple description:

Indeed, this follows from the fact that gr⁡n+lWOX(∗D)≅il+OE(l)\operatorname{gr}^{W}_{n+l}\mathscr{O}_{X}(*D)\cong i_{l+}\mathscr{O}_{E(l)} with a Tate Twist, so that the analogous statement of (\refwsncgen0)(\ref{wsncgen0}) is true for il+OE(l)i_{l+}\mathscr{O}_{E(l)} (see e.g. [saito09]*Remark 1.1 iii.)

For the rest of the proof we use right D\mathscr{D}-modules. By [olano22a]*Proposition 4.1,

Around zz, WlωX(D)W_{l}\omega_{X}(D) is generated by

where ω\omega is the standard generator of ωX\omega_{X}. It is clear that WlωX(D)⋅FpDXW_{l}\omega_{X}(D)\cdot F_{p}\mathscr{D}_{X} is generated by

The result follows from the equation ωxj11+b1⋯xjl1+bl=ωxIp+1(xj1p−b1⋯xjlp−blxI∖Jp+1)\frac{\omega}{x_{j_{1}}^{1+b_{1}}\cdots x_{j_{l}}^{1+b_{l}}}=\frac{\omega}{x_{I}^{p+1}}(x_{j_{1}}^{p-b_{1}}\cdots x_{j_{l}}^{p-b_{l}}x_{I\setminus J}^{p+1}). The last statement follows from the fact that, if l>rl>r, around zz, WlωX(D)=ωX(D)W_{l}\omega_{X}(D)=\omega_{X}(D). ∎

Birational definition

Let XX be a smooth variety and DD a reduced divisor. Consider a log-resolution f:Y→Xf:Y\to X of the pair (X,D)(X,D), which is an isomorphism over X∖DX\setminus D, and denote E=(f∗D)redE=(f^{*}D)_{\rm red}. A birational definition is given for Hodge ideals in [hodgeideals]*§9. In this section, we give a similar equivalent definition for weighted Hodge ideals. For the rest of this section we use right D\mathscr{D}-modules, as it is more convenient for the construction. Recall that the right DX\mathscr{D}_{X}-module corresponding to OX(∗D)\mathscr{O}_{X}(*D) is ωX(∗D)\omega_{X}(*D), and

Consider the following complex which we denote by A∙A^{\bullet}:

placed in degrees −n,…,0-n,\ldots,0. The results in [hodgeideals]*§3 say that the complex A∙A^{\bullet} represents the object ωY(∗E)⊗LDYDY→X\omega_{Y}(*E)\overset{\mathbf{L}}{\otimes}_{\mathscr{D}_{Y}}\mathscr{D}_{Y\to X} in the derived category of filtered right f−1DXf^{-1}\mathscr{D}_{X}-modules. Moreover, R0f∗A∙≅ωX(∗D)R^{0}f_{*}A^{\bullet}\cong\omega_{X}(*D).

For p≥0p\geq 0 define the subcomplex Cp−n∙=Fp−nA∙C^{\bullet}_{p-n}=F_{p-n}A^{\bullet} of A∙A^{\bullet} by

The pushforward of this complex admits the following interpretation:

by [hodgeideals]*Remark 9.3, Corollary 12.1.

We prove similar results in order to obtain a birational definition. Consider the complex B∙B^{\bullet}:

is given by ω⊗P→dω⊗P+∑(dzi∧ω)⊗∂iP\omega\otimes P\to d\omega\otimes P+\sum{(dz_{i}\wedge\omega)\otimes\partial_{i}P}. The complex B∙B^{\bullet} is filtered quasi-isomorphic to the object ωY(∗E)\omega_{Y}(*E) in degree 0 [hodgeideals]*Proposition 3.1.

in degrees −n,…,0-n,\ldots,0 is quasi-isomorphic to Wn+lωY(∗E)W_{n+l}\omega_{Y}(*E).

We see first that the complex WlB∙W_{l}B^{\bullet} is exact in degrees −n,…,−1-n,\ldots,-1. Fix a degree −p-p. We need to see that

so that no ziz_{i} that appears in zIz_{I} divides CI,J,αβzβC^{\beta}_{I,J,\alpha}z^{\beta}. From this description, it follows that for each summand CI,J,αβzβdzIzI∧dzJ⊗∂αC^{\beta}_{I,J,\alpha}z^{\beta}\frac{dz_{I}}{z_{I}}\wedge dz_{J}\otimes\partial^{\alpha}, ∣I∣|I| determines the weight where the form CI,J,αβzβdzIzI∧dzJC^{\beta}_{I,J,\alpha}z^{\beta}\frac{dz_{I}}{z_{I}}\wedge dz_{J} lies.

Next, we write, ω=ω≤l+ω>l\omega=\omega_{\leq l}+\omega_{>l}, where the first term consists of the summands with ∣I∣≤l|I|\leq l, and the latter of the terms with ∣I∣>l|I|>l. Using the description of d′d^{\prime}, we see that d′ω≤ld^{\prime}\omega_{\leq l} is in the completion of WlΩYn−p(log⁡E)⊗DYW_{l}\Omega_{Y}^{n-p}(\log{E})\otimes\mathscr{D}_{Y}, and each summand of d′ω>ld^{\prime}\omega_{>l} is not. Indeed,

Since η∈ker⁡b^\eta\in\ker{\hat{b}}, d′ω>l=0d^{\prime}\omega_{>l}=0, and d′ω≤l=ηd^{\prime}\omega_{\leq l}=\eta, with ω≤l\omega_{\leq l} in the completion of WlΩYn−p−1(log⁡E)⊗DYW_{l}\Omega_{Y}^{n-p-1}(\log{E})\otimes\mathscr{D}_{Y}.

given by ωf⊗P→ωf⋅P\frac{\omega}{f}\otimes P\to\frac{\omega}{f}\cdot P. Fixing a degree of the Hodge filtration, and using the description of the Hodge filtration of Wn+lωY(∗E)W_{n+l}\omega_{Y}(*E) (see for example Proposition 3.3), we see that this map is surjective. That the kernel is the image of WlΩYn−1(log⁡E)⊗OYDYW_{l}\Omega^{n-1}_{Y}(\log{E})\otimes_{\mathscr{O}_{Y}}\mathscr{D}_{Y} follows from [hodgeideals]*Proposition 3.1 and an argument similar to the one above.

We have that WlA∙=WlB∙⊗DYDY→XW_{l}A^{\bullet}=W_{l}B^{\bullet}\otimes_{\mathscr{D}_{Y}}\mathscr{D}_{Y\to X}, where DY→X=OY⊗f−1OXf−1DX\mathscr{D}_{Y\to X}=\mathscr{O}_{Y}\otimes_{f^{-1}\mathscr{O}_{X}}f^{-1}\mathscr{D}_{X} is the transfer module. Note that when we see it as an OY\mathscr{O}_{Y} module, we simply write f∗DXf^{*}\mathscr{D}_{X}.

The complex WlA∙W_{l}A^{\bullet} represents Wn+lωY(∗E)⊗LDYDY→XW_{n+l}\omega_{Y}(*E)\overset{\mathbf{L}}{\otimes}_{\mathscr{D}_{Y}}\mathscr{D}_{Y\to X} in the derived category of filtered right f−1DXf^{-1}\mathscr{D}_{X}-modules.

It is enough to show that the elements WlBkW_{l}B^{k} are acyclic with respect to −⊗DYDY→X-\otimes_{\mathscr{D}_{Y}}\mathscr{D}_{Y\to X}. For any kk consider the following spectral sequence:

[weibel]*Theorem 5.6.6. As DY\mathscr{D}_{Y} is a locally free OY\mathscr{O}_{Y}-module, then E2p,q=0E_{2}^{p,q}=0 for q≠0q\neq 0. Therefore,

for p≠0p\neq 0, where the last equality follows from the fact that f∗DXf^{*}\mathscr{D}_{X} is locally free.

whose image is Wn+lωX(∗D)W_{n+l}\omega_{X}(*D). Moreover, the complex Cp−n∙C_{p-n}^{\bullet} described above corresponds to the Fp−n(ωY(∗E)⊗LDYDY→X)F_{p-n}(\omega_{Y}(*E)\overset{\mathbf{L}}{\otimes}_{\mathscr{D}_{Y}}\mathscr{D}_{Y\to X}) using the identification

whose image is Fp−nωX(∗D)=Ip(D)⊗ωX((p+1)D)F_{p-n}\omega_{X}(*D)=I_{p}(D)\otimes\omega_{X}((p+1)D) (see [hodgeideals]*Sections 4, 9, and 12).

Similarly, we define Cl,p−n∙C^{\bullet}_{l,p-n} by

which corresponds to Fp−n(Wn+lωY(∗E)⊗LDYDY→X)F_{p-n}(W_{n+l}\omega_{Y}(*E)\overset{\mathbf{L}}{\otimes}_{\mathscr{D}_{Y}}\mathscr{D}_{Y\to X}) under the identification

whose image is Fp−nH0f+Wn+lωX(∗D)F_{p-n}H^{0}f_{+}W_{n+l}\omega_{X}(*D) (see for instance [hodgeideals]*§4). Taking the composition

and using strictness in the middle morphism (since it underlies a morphism of mixed Hodge modules), the image corresponds to Fp−nWn+lωX(∗D)=IpWl(D)⊗ωX((p+1)D).F_{p-n}W_{n+l}\omega_{X}(*D)=I^{W_{l}}_{p}(D)\otimes\omega_{X}((p+1)D). ∎

The description in Proposition 4.3 for I0Wl(D)I_{0}^{W_{l}}(D) coincides with the description in [olano22a]*Proposition 3, since f∗WlωY(E)→f∗ωY(E)f_{*}W_{l}\omega_{Y}(E)\to f_{*}\omega_{Y}(E) is an inclusion. The complex Cl,1−n∙C^{\bullet}_{l,1-n} also has a simple description. Recall that by definition

is injective [hodgeideals]*Lemma 3.4. Using the fact that WlΩYn−1(log⁡E)↪ΩYn−1(log⁡E)W_{l}\Omega^{n-1}_{Y}(\log{E})\hookrightarrow\Omega^{n-1}_{Y}(\log{E}) and WlωY(E)⊗f∗F1DX↪ωY(E)⊗f∗F1DXW_{l}\omega_{Y}(E)\otimes f^{*}F_{1}\mathscr{D}_{X}\hookrightarrow\omega_{Y}(E)\otimes f^{*}F_{1}\mathscr{D}_{X} are injective (since F1DXF_{1}\mathscr{D}_{X} is a locally free OX\mathscr{O}_{X}-module), we obtain that the differential in Cl,1−n∙C^{\bullet}_{l,1-n} is also an inclusion. Let Fl,1\mathcal{F}_{l,1} be the cokernel. This means that

This map can be interpreted by using the complex C1−n∙C^{\bullet}_{1-n}. Indeed, let F1\mathcal{F}_{1} be the cokernel of the differential in C1−n∙C^{\bullet}_{1-n}. We have an induced map Fl,1→F1\mathcal{F}_{l,1}\to\mathcal{F}_{1}. Since f∗F1=I1(D)⊗ωX(2D)f_{*}\mathcal{F}_{1}=I_{1}(D)\otimes\omega_{X}(2D),

Note that since weighted Hodge ideals were defined in terms of the Hodge and weight filtrations of OX(∗D)\mathscr{O}_{X}(*D), the constructions presented in this section are independent of the resolution of singularities.

Weighted Hodge ideals and V𝑉V-filtration

Let XX be a smooth variety and DD be an effective reduced divisor defined by the global equation f∈OX(X)f\in\mathscr{O}_{X}(X). The Hodge ideals Ip(D)I_{p}(D) can be described using the VV-filtration of i+OXi_{+}\mathscr{O}_{X}, where ii is the graph embedding defined by ff. Namely,

where Qj(x)=∏i=0j−1(x+i)Q_{j}(x)=\prod_{i=0}^{j-1}(x+i), [mustatapopa20b]*Theorem A’. An equivalent description is obtained using the following map:

The map τ\tauThe map τ\tau corresponds to τ1\tau_{1} in the notation of [mustatapopa20]. See §1 for the discussion about the reduced case. is a surjective morphism of DX\mathscr{D}_{X}-modules, and

see [mustatapopa20]*Proposition 5.4 and Lemma 5.1. Moreover, the map τ\tau induces a map

Indeed, it is enough to see that τ(V>1i+OX)⊆OX\tau(V^{>1}i_{+}\mathscr{O}_{X})\subseteq\mathscr{O}_{X}. This follows from the fact that V>1i+OX=V1+αi+OX=t⋅Vαi+OXV^{>1}i_{+}\mathscr{O}_{X}=V^{1+\alpha}i_{+}\mathscr{O}_{X}=t\cdot V^{\alpha}i_{+}\mathscr{O}_{X}, with α>0\alpha>0, and that if j>0j>0, tu∂tjδ=fu∂tjδ−ju∂tj−1δtu\partial_{t}^{j}\delta=fu\partial_{t}^{j}\delta-ju\partial_{t}^{j-1}\delta, and tuδ=fuδtu\delta=fu\delta. For v=∑j=0pvj∂tjδ∈V>1i+OXv=\sum_{j=0}^{p}v_{j}\partial_{t}^{j}\delta\in V^{>1}i_{+}\mathscr{O}_{X}, there exists u=∑j=0puj∂tjδ∈Vαi+OXu=\sum_{j=0}^{p}u_{j}\partial_{t}^{j}\delta\in V^{\alpha}i_{+}\mathscr{O}_{X} such that, tu=vtu=v. Hence,

The DX\mathscr{D}_{X}-module gr⁡V1i+OX\operatorname{gr}^{1}_{V}i_{+}\mathscr{O}_{X} underlies the mixed Hodge module ψf,1OX\psi_{f,1}\mathscr{O}_{X} and its weight filtration can be described in terms of the nilpotent operator t∂tt\partial_{t}. In order to complete the description in Theorem 5.6, we first need to show that the map τˉ\bar{\tau} also preserves the weight filtration.

The map τˉ\bar{\tau} sends the weight and Hodge pieces to the same image as the map τDX\tau_{\mathscr{D}_{X}} that underlies a morphism of mixed Hodge modules

The map τˉ\bar{\tau} is surjective and using its description, we observe that its kernel is the image of the map ∂tt−1\partial_{t}t-1 on gr⁡V1i+OX\operatorname{gr}^{1}_{V}i_{+}\mathscr{O}_{X}. The same is true for the map τDX\tau_{\mathscr{D}_{X}}. Indeed, the map ∂tt−1\partial_{t}t-1 underlies the composition Var∘canVar\circ can on ψf,1OX\psi_{f,1}\mathscr{O}_{X}. As can:ψf,1OX→ϕf,1OXcan:\psi_{f,1}\mathscr{O}_{X}\to\phi_{f,1}\mathscr{O}_{X} is surjective because i+OXi_{+}\mathscr{O}_{X} has strict support (see for instance [schnellsurvey]*§11), the cokernel of Var∘canVar\circ can coincides with the cokernel of

The cokernel of VarVar is isomorphic to iD∗H1iD!OXi_{D*}\mathcal{H}^{1}i_{D}^{!}\mathscr{O}_{X}, where iD:D→Xi_{D}:D\to X is the inclusion [saito90]*Corollary 2.24. Moreover, iD∗H1iD!OXi_{D*}\mathcal{H}^{1}i_{D}^{!}\mathscr{O}_{X} is isomorphic to HD1(OX)\mathcal{H}^{1}_{D}(\mathscr{O}_{X}) [saito09]*§2.2. This means that τˉ\bar{\tau} and τDX\tau_{\mathscr{D}_{X}} could only differ by a DX\mathscr{D}_{X}-automorphism of HD1(OX)\mathcal{H}^{1}_{D}(\mathscr{O}_{X}) and the result is a consequence of Lemma 5.4. ∎

A DX\mathscr{D}_{X}-automorphism of HD1(OX)\mathcal{H}^{1}_{D}(\mathscr{O}_{X}) preserves the Hodge and weight filtration.

We are very grateful to Mircea Mustaţă for suggesting the argument of Lemma 5.4.

A consequence of the result above, is that we can write a description of the weighted Hodge ideals in a similar way to (5.1). Let WlV1i+OXW_{l}V^{1}i_{+}\mathscr{O}_{X} be the submodule of V1i+OXV^{1}i_{+}\mathscr{O}_{X} which maps to Wn+l−2gr⁡V1i+OXW_{n+l-2}\operatorname{gr}^{1}_{V}i_{+}\mathscr{O}_{X} via the canonical projection.

It follows from Proposition 5.3 that τ(Fp+1WlV1i+OX)=FpWn+lOX(∗D)=IpWl(D)⊗OX((p+1)D).\tau(F_{p+1}W_{l}V^{1}i_{+}\mathscr{O}_{X})=F_{p}W_{n+l}\mathscr{O}_{X}(*D)=I_{p}^{W_{l}}(D)\otimes\mathscr{O}_{X}((p+1)D). ∎

The result above can be simplified even more using the description of the weight filtration of ψf,1OX\psi_{f,1}\mathscr{O}_{X}, and that is the statement of Theorem A.

First, we note that if v∈V1i+OXv\in V^{1}i_{+}\mathscr{O}_{X}, then τ(t∂tv)=0\tau(t\partial_{t}v)=0. Indeed, let v=∑j=0pvj∂tjδ∈V1i+OXv=\sum_{j=0}^{p}v_{j}\partial_{t}^{j}\delta\in V^{1}i_{+}\mathscr{O}_{X}, then

The weight filtration of ψf,1OX\psi_{f,1}\mathscr{O}_{X} admits the following description for k≥0k\geq 0:

(see [saito94]*2.7 and for the monodromy filtration see e.g. [variationsofmhsi]*Remark 2.3). The only piece that is not an image of (t∂t)(t\partial_{t}) is ker⁡(t∂t)k+1\ker{(t\partial_{t})^{k+1}}. That means that the subset ker⁡(t∂t)l⊆WlV1i+OX\ker{(t\partial_{t})^{l}}\subseteq W_{l}V^{1}i_{+}\mathscr{O}_{X} has the same image as WlV1i+OXW_{l}V^{1}i_{+}\mathscr{O}_{X} via τ\tau. ∎

Let (X,D)(X,D) be a pair such that DD has at most isolated weighted homogeneous singularities. Theorem A gives a complete description of the weighted Hodge ideals using the description of the VV-filtration in [saito09]. Using the notation above, in this case, (t∂t)2u∈V>1i+OX(t\partial_{t})^{2}u\in V^{>1}i_{+}\mathscr{O}_{X} for all u∈V1i+OXu\in V^{1}i_{+}\mathscr{O}_{X}. For this reason, IpW2(D)=Ip(D)I_{p}^{W_{2}}(D)=I_{p}(D), for all p≥0p\geq 0. An argument without the use of the VV-filtration in the case of p=0p=0 is described in [olano22a]*§10.

A direct application of Theorem A is that we can recover the following result proved in [hodgeideals]*Theorem C. The proof we give differs from the one in [hodgeideals] and is also much shorter.

Let XX be a smooth variety and DD an effective reduced divisor. Then

Recall that adj⁡(D)=I0W1(D)\operatorname{adj}(D)=I_{0}^{W_{1}}(D) [olano22a]*Theorem A. Moreover, as Ip(D)⊆I1(D)I_{p}(D)\subseteq I_{1}(D) [hodgeideals]*Proposition 13.1, it is enough to prove that I1(D)⊆I0W1(D).I_{1}(D)\subseteq I_{0}^{W_{1}}(D).

Let u∈I1(D)u\in I_{1}(D). By (5.1), u=u0f+u1u=u_{0}f+u_{1}, where ff is defining equation of DD, and u0δ+u1∂tδ∈V1i+OXu_{0}\delta+u_{1}\partial_{t}\delta\in V^{1}i_{+}\mathscr{O}_{X}. We also have that

Finally, as δ∈V>0i+OX\delta\in V^{>0}i_{+}\mathscr{O}_{X}, then u0fδ=t(u0δ)∈V>1i+OX⊆W1V1i+OXu_{0}f\delta=t(u_{0}\delta)\in V^{>1}i_{+}\mathscr{O}_{X}\subseteq W_{1}V^{1}i_{+}\mathscr{O}_{X}. This means that u0fδ+u1δ∈W1V1i+OXu_{0}f\delta+u_{1}\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X}, hence u0f+u1∈I0W1(D).u_{0}f+u_{1}\in I_{0}^{W_{1}}(D). ∎

Using these ideas, we obtain the following result for the 1st weighted Hodge ideals.

Suppose first that αf~>p+1\widetilde{\alpha_{f}}>p+1. Then, by Lemma 5.9, ∂tpδ∈V1i+OX\partial_{t}^{p}\delta\in V^{1}i_{+}\mathscr{O}_{X}. Moreover, there exists α∈(0,1]\alpha\in(0,1] such that αf~≥p+1+α\widetilde{\alpha_{f}}\geq p+1+\alpha. Again, by Lemma 5.9, ∂tp+1δ∈W1V1i+OX\partial_{t}^{p+1}\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X}, and therefore, IpW1(D)=OXI_{p}^{W_{1}}(D)=\mathscr{O}_{X}.

Suppose now that IpW1(D)=OXI_{p}^{W_{1}}(D)=\mathscr{O}_{X}. Then, Ip(D)=OXI_{p}(D)=\mathscr{O}_{X}, and in particular δ,∂tδ,…,∂tpδ∈V1i+OX\delta,\partial_{t}\delta,\ldots,\partial_{t}^{p}\delta\in V^{1}i_{+}\mathscr{O}_{X}. Moreover, there exists v=∑j=0pvj∂tjδ∈W1V1i+OXv=\sum_{j=0}^{p}v_{j}\partial_{t}^{j}\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X} such that ∑j=0pQj(1)fp−jvj=1\sum_{j=0}^{p}Q_{j}(1)f^{p-j}v_{j}=1. It is enough to show that ∂tpδ∈W1V1i+OX\partial_{t}^{p}\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X}. Indeed, by Proposition 5.6 and the injectivity of t:gr⁡V0i+OX→gr⁡V1i+OXt:\operatorname{gr}_{V}^{0}i_{+}\mathscr{O}_{X}\to\operatorname{gr}_{V}^{1}i_{+}\mathscr{O}_{X} (see e.g. [schnellsurvey]*§11), this means that ∂tp+1δ∈Vαi+OX\partial_{t}^{p+1}\delta\in V^{\alpha}i_{+}\mathscr{O}_{X} with α∈(0,1]\alpha\in(0,1], and therefore, αf~≥p+1+α>p+1\widetilde{\alpha_{f}}\geq p+1+\alpha>p+1. We argue by induction. Suppose p=0p=0. Then v=v0δv=v_{0}\delta and by the second condition, v0=1v_{0}=1. Hence, δ∈W1V1i+OX\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X}. By the induction hypothesis, we assume now that ∂tkδ∈W1V1i+OX\partial_{t}^{k}\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X} for k=0,…,p−1k=0,\ldots,p-1. It follows from the description of vv that

The result follows if we show that f∂tpδ∈W1V1i+OXf\partial_{t}^{p}\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X}, and this is a consequence of f∂tpδ=t∂t(∂tp−1δ)+p∂tp−1δ∈W1V1i+OXf\partial_{t}^{p}\delta=t\partial_{t}(\partial_{t}^{p-1}\delta)+p\partial_{t}^{p-1}\delta\in W_{1}V^{1}i_{+}\mathscr{O}_{X}.

In general, we cannot obtain more information about the other pp-weighted Hodge ideals. In [olano22a]*§13, the case of isolated log-canonical singularities, that are not rational, is discussed. This case corresponds to αf~=1\widetilde{\alpha_{f}}=1. By the discussion above, it is clear that I0(D)=OXI_{0}(D)=\mathscr{O}_{X} and that I0W1(D)I_{0}^{W_{1}}(D) is not trivial. For l=2,…,n−1l=2,\ldots,n-1, there are examples of ff where the weighted multiplier ideals I0Wl(D)I_{0}^{W_{l}}(D) are trivial, and other examples where they are non-trivial [ishii85]*Theorem 5.2.

D. Local study

There is a short exact sequence that arises from the definition of the weight filtration on OX(∗D)\mathscr{O}_{X}(*D):

Applying FpF_{p}, we obtain the short exact sequence

When DD has at most isolated singularities and l≥2l\geq 2, gr⁡n+lWOX(∗D)\operatorname{gr}^{W}_{n+l}\mathscr{O}_{X}(*D) is supported on the singular points. To simplify the notation, we use the following definition.

Suppose DD has at most one isolated singularity x∈Dx\in D, and let ix:{x}↪Xi_{x}:\{x\}\hookrightarrow X. For l≥2l\geq 2, we denote by HlH_{l} the complex pure Hodge structure of weight n+ln+l such that

In order to describe the dimension of Fp(ix)+HlF_{p}(i_{x})_{+}H_{l}, it is enough to describe the dimension of Gr⁡Fn−kHl\operatorname{Gr}_{F}^{n-k}H_{l} for 0≤k≤p0\leq k\leq p. This is a consequence of the local description of the Hodge filtration of (ix)+Hl(i_{x})_{+}H_{l}. Let x1,…,xnx_{1},\ldots,x_{n} be a set of coordinates around the point x∈Xx\in X. We have the following description of the pushforward of HlH_{l} as a D\mathscr{D}-module:

where ∂i=∂∂xi\partial_{i}=\frac{\partial}{\partial_{x_{i}}}, and

where ∂ν=∂1ν1⋯∂nνn\partial^{\nu}=\partial_{1}^{\nu_{1}}\cdots\partial_{n}^{\nu_{n}}, ∣ν∣=ν1+…+νn|\nu|=\nu_{1}+\ldots+\nu_{n}, and FkHl=F−kHlF_{k}H_{l}=F^{-k}H_{l}. Since the lowest degree of the Hodge filtration of OX(∗D)\mathscr{O}_{X}(*D) is 0, and DR⁡((ix)+Hl)≅(ix)∗Hl\operatorname{DR}((i_{x})_{+}H_{l})\cong(i_{x})_{*}H_{l}, that is, the push-forward of the pure Hodge structure HlH_{l} is a skyscraper sheaf, then the highest degree of the Hodge filtration of HlH_{l} is nn, in other words, Fn+1Hl=0F^{n+1}H_{l}=0. Using this, we obtain, for instance, that

Since Fp(ix)+HlF_{p}(i_{x})_{+}H_{l} is a skyscraper sheaf, we denote by dim⁡(Fp(ix)+Hl)\dim(F_{p}(i_{x})_{+}H_{l}) the dimension of the complex vector space JpJ_{p} that satisfies Fp(ix)+Hl=(ix)∗JpF_{p}(i_{x})_{+}H_{l}=(i_{x})_{*}J_{p}. From the discussion above, we obtain that

The dimension of Gr⁡Fn−kHl\operatorname{Gr}_{F}^{n-k}H_{l} is described in Theorem B.

We can and will assume that XX is a projective variety. Indeed, there is an open set around xx which has a smooth projective compactification Xˉ\bar{X}. Let Dˉ\bar{D} be the closure of DD in Xˉ\bar{X}. Consider a log-resolution of (Xˉ∖x,Dˉ∖x)(\bar{X}\smallsetminus x,\bar{D}\smallsetminus x) given by a sequence of blow ups with centers over the singular locus of Dˉ∖x\bar{D}\smallsetminus x. By blowing up the same sequence of centers over Xˉ\bar{X}, we obtain a map X1→XˉX_{1}\to\bar{X}. Let D1D_{1} be the strict transform of Dˉ\bar{D}. By construction, the map is an isomorphism over (X,D)(X,D), and D1D_{1} has only one isolated singularity corresponding to x∈Dx\in D. We replace (X,D)(X,D) with (X1,D1)(X_{1},D_{1}).

First, we prove that these dimensions do not depend on the log-resolution of singularities that is an isomorphism outside of {x}\{x\}. Since for a pair of resolution of singularities one can find a third one that dominates the two of them, it is enough to show that the dimensions are equal if we have two resolutions of singularities g1:D1→Dg_{1}:D_{1}\to D and g2:D2→Dg_{2}:D_{2}\to D such that there is a morphism h:D1→D2h:D_{1}\to D_{2} such that g1=g2∘hg_{1}=g_{2}\circ h. Let Gi⊆DiG_{i}\subseteq D_{i} be the exceptional divisor of gig_{i}. Consider the exact sequence of mixed Hodge structures

(see [PS]*Proof of Theorem 6.15). For l≥3l\geq 3, applying Hp,n−l−pH^{p,n-l-p}, we obtain that

For l=2l=2, applying Hp,n−p−2H^{p,n-p-2} and Hn−p−1,p+1H^{n-p-1,p+1}, and noting that hp,n−p−2(Di)=hn−p−1,p+1(Di)h^{p,n-p-2}(D_{i})=h^{n-p-1,p+1}(D_{i}), we obtain that

Let f:Y→Xf:Y\to X be a log-resolution that is an isomorphism outside of xx, and E:=f−1(D)redE:=f^{-1}(D)_{red}. This resolution defines a log-resolution of singularities g:D~→Dg:\widetilde{D}\to D by restriction, that is an isomorphism outside of xx. We use the spectral sequence (1.3) for the constant map from XX to a point. In this case, it says

Moreover, the degeneration of the Hodge-to-de-Rham spectral sequence says that

(see for example [hodgeideals]*Example 4.2).

Applying gr⁡−n+pF\operatorname{gr}^{F}_{-n+p}, using (6.7), and the E2E_{2}-degeneration of the spectral sequence, we obtain that

where the last isomoprhism follows from Poincaré duality (see [PS]*Theorem 6.23). Using the long exact sequence of the pair (X,D)(X,D), we obtain that

as Hn−1(X)H^{n-1}(X) and Hn(X)H^{n}(X) have pure Hodge structures. Finally, as gg has {x}\{x\} as discriminant, we have a long exact sequence,

As this is a sequence of mixed Hodge structures, we obtain

Consider now l=2l=2. In this case, the maps

where β=gr⁡−n+pFβ~\beta=\operatorname{gr}^{F}_{-n+p}\widetilde{\beta} and γ=gr⁡−n+pFγ~\gamma=\operatorname{gr}^{F}_{-n+p}\widetilde{\gamma}, we obtain that

Indeed, this follows from the descriptions of E2n−2+s,n+2E_{2}^{n-2+s,n+2} for s=0,1,2s=0,1,2 and Poincaré duality. More precisely, we have three short exact sequences

and also that Gr⁡Fn−pE2n−1,n+2≅Hp,n−p−2(Hcn−1(U))∗\operatorname{Gr}_{F}^{n-p}E_{2}^{n-1,n+2}\cong H^{p,n-p-2}(H^{n-1}_{c}(U))^{*}. Using the long exact sequence associated to the pair (X,D)(X,D) to relate these three sequences, we obtain

Finally, using that the map gg has {x}\{x\} as discriminant, we obtain that

In general, the term hn−p−1,p+1(Hn(G))h^{n-p-1,p+1}(H^{n}(G)) might not be 0. Consider for instance n=4n=4 and p=1p=1. In this case, h2,2(H4(G))=kh^{2,2}(H^{4}(G))=k where kk is the number of irreducible components of GG. Using similar computations as above, we also see that

that is, the failure of Poincaré duality. Still, in the case p=0p=0, the term hn−p−1,p+1(Hn(G))h^{n-p-1,p+1}(H^{n}(G)) is always 0, as GG is (n−2)(n-2)-dimensional (see [olano22a]*Theorem B).

E. Vanishing Theorems

Let XX be a smooth projective variety of dimension nn, and DD an ample divisor. Let U=X∖DU=X\smallsetminus D. As UU is smooth and affine, Hi+n(U)=0H^{i+n}(U)=0 for i>0i>0 (see for instance [lazarsfeld2]*Theorem 3.1.1). In this setting we have the following result.

In [olano22a]*Proof of Proposition 12.1, using the spectral sequences

corresponding to the map E1−n−k−1,i+n+k→E1−n−k,i+n+kE^{-n-k-1,i+n+k}_{1}\to E_{1}^{-n-k,i+n+k}. Then we have the following short exact sequence:

As E2−n−l,n+l+i=0E_{2}^{-n-l,n+l+i}=0, using the analysis above, we obtain a short exact sequence

When p=0p=0, the result above is enough to obtain that

for l≥2l\geq 2 and i≥1i\geq 1. Indeed, as 0 is the lowest degree of the Hodge filtration on OX(∗D)\mathscr{O}_{X}(*D), we have

This is no longer the case when we consider gr⁡−n+pF\operatorname{gr}^{F}_{-n+p} for p≥1p\geq 1 instead. Nonetheless, following the idea in [hodgeideals]*Proof of Theorem F, we give conditions in Theorem C to obtain an analogue vanishing theorem.

Since Ip−1Wl(D)=OXI_{p-1}^{W_{l}}(D)=\mathscr{O}_{X}, we have the following short exact sequence

Using the long exact sequence of cohomologies and Kodaira-vanishing, we note that it is enough to prove that

The complex C∙C^{\bullet} can be identified with the complex

concentrated in degrees −p-p to , since F0Wn+lOX(∗D)=OX(D)F_{0}W_{n+l}\mathscr{O}_{X}(*D)=\mathscr{O}_{X}(D) and gr⁡kFWn+lOX(∗D)≅OD((k+1)D)\operatorname{gr}^{F}_{k}W_{n+l}\mathscr{O}_{X}(*D)\cong\mathscr{O}_{D}((k+1)D) for k≤p−1k\leq p-1 (see §1 for the definition of gr⁡pFDR⁡)\operatorname{gr}^{F}_{p}\operatorname{DR}).

Suppose now that DD has at most isolated singularities. By Lemma 7.1, we obtain that

for i≥1i\geq 1 and l≥2l\geq 2. In particular, this means that

for the same indices, by the Hodge-to-de-Rham degeneration. Next, we use the exact sequence

then E1−1,q=0E_{1}^{-1,q}=0 if q≥2q\geq 2 by Nakano vanishing. Moreover, E1−1,1=0E_{1}^{-1,1}=0 by our hypothesis.

We continue with a similar analysis in the higher pages of the spectral sequence. More precisely, we show that the hypothesis implies that Er−r,q+r−1=0E_{r}^{-r,q+r-1}=0 for all r≥2r\geq 2. Note that this is enough to complete the proof. Indeed, if this is the case, we obtain that

for q≥1q\geq 1, where the last equality follows from the established equality with C∙C^{\bullet}.

for r≥pr\geq p. Indeed, this is clear for the strict inequality by the degrees on which C∙C^{\bullet} is concentrated, and

If q≥2q\geq 2, then this spaces vanishes by Nakano vanishing, and if q=1q=1, it vanishes by our assumption. Finally, for r≤p−1r\leq p-1, we have

This space fits the a long exact sequence

If q≥2q\geq 2, then the two other terms vanish by Nakano vanishing, and if q=1q=1, they vanish by the assumption. ∎

This result does not hold in general for l=1l=1 (see [olano22a]*Remark 9).

Kodaira-type vanishing

Using a similar idea to the one in the proof of Theorem C, we obtain a vanishing theorem for weighted Hodge ideals. This is the analogue result to [hodgeideals]*Theorem F.

Let XX be a smooth projective variety of dimension nn, and DD a reduced effective divisor. Let LL be a line bundle such that L(kD)L(kD) is ample for 0≤k≤p0\leq k\leq p, and assume Ip−1W1(D)I_{p-1}^{W_{1}}(D) is trivial. Then

If Hj(X,ΩXn−j⊗L((p−j+1)D))=0H^{j}(X,\Omega_{X}^{n-j}\otimes L((p-j+1)D))=0 for all 1≤j≤p1\leq j\leq p, then

Since Ip−1Wl(D)=OXI_{p-1}^{W_{l}}(D)=\mathscr{O}_{X}, we have the following short exact sequence

By Kodaira-vanishing, it is enough to prove

for i≥1i\geq 1 and l≥1l\geq 1 as a consequence of a vanishing result by Saito [saito90]*Proposition 2.33. To complete the proof, we use the same spectral sequence as in the proof of Theorem C. ∎

Applications

In this section, we combine the local study and the vanishing results. To obtain applications, we use the vanishing theorems of the previous sections. A class varieties where the vanishing condition in Theorem C and Proposition 8.1 is satisfied, is toric varieties. In this case, the Bott-Danilov-Steenbrink vanishing theorem says that if AA is an ample line bundle on the toric variety XX, then

The result follows from passing to cohomology and applying Theorem C. ∎

Suppose the pair (X,D)(X,D) is pp-log-canonical, and has at most isolated singularities. If p=0p=0, the pair is log-canonical and in this case, I0W1(D)I_{0}^{W_{1}}(D) is the maximal ideal at each isolated singularity that is not rational, by a result of Ishii (see [olano22a]*§5.3). For simplicity, let x∈Dx\in D be the only singularity and i:{x}↪Xi:\{x\}\hookrightarrow X the inclusion, and suppose that it is log-canonical singularity and not rational. The result above means that if we denote

for l≥2l\geq 2, there exists exactly one degree ll such that dim⁡(gr⁡−nFHl)=1\dim(\operatorname{gr}^{F}_{-n}H_{l})=1, and the rest are 0. In this case, using [olano22a]*Theorem B, we say that the singularity is of type (0,n−l)(0,n-l) [ishii85]*Definition 4.1. There is a similar picture for the cases p≥1p\geq 1 we describe next.

Non-rational log-canonical singularities correspond to the case where the minimal exponent at the singularity is 1. We then consider singularities with minimal exponent p+1p+1, in which case Ip(D)=OXI_{p}(D)=\mathscr{O}_{X} and IpW1(D)I_{p}^{W_{1}}(D) is non-trivial by Corollary 5.10. These singularities generalize the example of non-rational log-canonical singularities in the following sense.

Suppose DD has at most one isolated singularity x∈Dx\in D, and αD~=p+1\widetilde{\alpha_{D}}=p+1. Then,

Suppose that DD is defined by f∈OXf\in\mathscr{O}_{X}. Recall from the proof of Corollary 5.10, that as αf~=p+1\widetilde{\alpha_{f}}=p+1, then δ,∂tδ,…,∂tpδ∈V1Bf\delta,\partial_{t}\delta,\ldots,\partial_{t}^{p}\delta\in V^{1}B_{f}. Moreover, we also know that δ,∂tδ,…,∂tp−1δ∈W1V1Bf\delta,\partial_{t}\delta,\ldots,\partial_{t}^{p-1}\delta\in W_{1}V^{1}B_{f}. It is then enough to show that g∂tpδ∈W1V1Bfg\partial_{t}^{p}\delta\in W_{1}V^{1}B_{f} if and only if g∈mxg\in\mathfrak{m}_{x}. As DD has an isolated singularity, we have that

We also know that ∂tpδ∈V1Bf∖W1V1Bf\partial_{t}^{p}\delta\in V^{1}B_{f}\smallsetminus W_{1}V^{1}B_{f}, and this means that ∂tp+1δ∈V0Bf∖V>0Bf\partial_{t}^{p+1}\delta\in V^{0}B_{f}\smallsetminus V^{>0}B_{f}. In particular, the class of ∂tp+1δ\partial_{t}^{p+1}\delta in Gr⁡pFgr⁡V0Bf\operatorname{Gr}^{F}_{p}\operatorname{gr}_{V}^{0}B_{f} is not zero. Using the result above, for any g∈mxg\in\mathfrak{m}_{x}, the class of g∂tp+1δg\partial_{t}^{p+1}\delta in Gr⁡pFgr⁡V0Bf\operatorname{Gr}^{F}_{p}\operatorname{gr}_{V}^{0}B_{f} is zero. This means that g∂tp+1δ∈V>0Bfg\partial_{t}^{p+1}\delta\in V^{>0}B_{f}, and equivalently, g∂tpδ∈W1V1Bfg\partial_{t}^{p}\delta\in W_{1}V^{1}B_{f}. Using the description of Theorem A, we obtain that g∈IpW1(D)g\in I_{p}^{W_{1}}(D) for any g∈mxg\in\mathfrak{m}_{x}, and we know that the ideal is not trivial, hence we have an equality. ∎

In other words, if DD has one isolated singularity x∈Dx\in D, and αD~=p+1\widetilde{\alpha_{D}}=p+1, then

by Theorem B, that is, there is exactly one l≥2l\geq 2 such that

and the rest are 0. Moreover, by the same result, ∑l≥2dim⁡(Gr⁡Fn−rHl)=1\sum_{l\geq 2}{\dim(\operatorname{Gr}_{F}^{n-r}H_{l})}=1, for 0≤r≤p−10\leq r\leq p-1.

Friedman and Laza have studied related invariants of singularities in similar conditions in [friedmanlaza22b]*Theorem 6.11 and Corollary 6.14.

Let x∈Dx\in D be an isolated singularity such that αD~x=p+1\widetilde{\alpha_{D}}_{x}=p+1, that is an isolated pp-log-canonical that is not pp-rational. Let ll be the degree such that dim⁡(Gr⁡Fn−pHl)=1\dim(\operatorname{Gr}_{F}^{n-p}H_{l})=1. Then, we say that the singularity is of type (p,n−l−p)(p,n-l-p).

Definition 9.3 is analogous to the definition of isolated log-canonical singularities of type (0,s)(0,s) [ishii85]*Definition 4.1, when x∈Dx\in D is an isolated singularity and DD is a hypersurface of a smooth variety.

Ishii defined these singularities more generally for normal isolated 1-Gorenstein log-canonical singularities. It is an open question how to generalize this definition for non-hypersurface singularities.

The possible types are (p,p),(p,p+1),…(p,n−2−p)(p,p),(p,p+1),\ldots(p,n-2-p). This is a consequence of the fact that the nilpotency order of the vanishing cohomology is bounded by Briançon-Skoda exponent [scherk80]*Main Theorem. This nilpotency order gives a bound for the nilpotency order of (∂tt)(\partial_{t}t) on gr⁡V0Bf\operatorname{gr}_{V}^{0}B_{f}, which in turn gives a bound for the order of (t∂t)(t\partial_{t}) on gr⁡V1Bf\operatorname{gr}_{V}^{1}B_{f}. The Briançon-Skoda exponent is bounded by n−2p−1n-2p-1 (see for instance [jksy22b]), which means that n−l−p≥pn-l-p\geq p.

where 1=(1,…,1)\mathbf{1}=(1,\ldots,1), and for any g∈Og\in\mathscr{O}, g=∑gAxAg=\sum g_{A}x^{A},

Suppose α~f=p+1\widetilde{\alpha}_{f}=p+1, which implies that ∂tpδ∈V1i+OX\partial^{p}_{t}\delta\in V^{1}i_{+}\mathscr{O}_{X}. Using the description of the microlocal VV-filtration (see [saito94]*Proposition 3.2), we see that if

then (t∂t)r+1∂tpδ∈V>1i+OX(t\partial_{t})^{r+1}\partial_{t}^{p}\delta\in V^{>1}i_{+}\mathscr{O}_{X}, or equivalently,

In general, r+1r+1 is not the degree with Gr⁡Fn−pHl≠0\operatorname{Gr}_{F}^{n-p}H_{l}\neq 0.

Let Δ0\Delta_{0} be the compact face that contains 1p+11\frac{1}{p+1}\mathbf{1} in its relative interior, and let s=dim⁡Δ0s=\dim{\Delta_{0}}. Assume also that the Newton polyhedron is simplicial. The number rr defined above satisfies that s=n−rs=n-r. Let ll be the degree such that Gr⁡Fn−pHl≠0\operatorname{Gr}_{F}^{n-p}H_{l}\neq 0. Then l≤r+1=n−s+1l\leq r+1=n-s+1, if s>0s>0, and l≤nl\leq n is s=0s=0.

If p=0p=0, the previous inequalities are equalities (without the simplicial assumption) by a result of Watanabe that says that the singularities are log-canonical of type (0,s−1)(0,s-1) if s>0s>0, and (0,0)(0,0) if s=0s=0, which is equivalent to the equalities [watanabe86]*Corollary 3.14.

By Proposition 9.1, the scheme ZZ is defined by the ideal IpWl(D)I_{p}^{W_{l}}(D). Therefore, the result follows from Corollary D.

F. Restriction Theorem

Let (M,F)(\mathcal{M},F) be a filtered right D\mathscr{D}-module underlying a mixed Hodge module MM on XX. Let H⊆XH\subseteq X be a smooth hypersurface and i:H↪Xi:H\hookrightarrow X the inclusion. In this section, we change the notation of the VV-filtration by Vk=V−kV_{k}=V^{-k}, which is the notation used in [mustatapopa18]. There exists a canonical morphism

with the filtrations induced by the filtrations on M\mathcal{M} (see [mustatapopa18]*§2). Moreover, on an open set U⊆XU\subseteq X where HH is given by a local equation tt, this map corresponds to

between the vanishing and nearby cycles along HH.

In the proof of [mustatapopa18]*Theorem A the authors defined for all kk a morphism

such that for u∈FkV−1Mu\in F_{k}V_{-1}\mathcal{M}, η(u)\eta(u) is the class of uu in FkM⊗OXOHF_{k}\mathcal{M}\otimes_{\mathscr{O}_{X}}\mathscr{O}_{H}. This map is well defined, as on an open set UU where HH is defined by an equation tt, the VV-filtration satisfies

and FkM⋅tF_{k}\mathcal{M}\cdot t maps to 0 in FkM⊗OXOHF_{k}\mathcal{M}\otimes_{\mathscr{O}_{X}}\mathscr{O}_{H}. The map η\eta induces a map on FkH1i!MF_{k}\mathcal{H}^{1}i^{!}\mathcal{M}. Indeed, since locally σ\sigma is right multiplication by tt, the image of σ\sigma is mapped to 0 by η⊗OX(H)\eta\otimes\mathscr{O}_{X}(H).

Let M=Wn+lωX(∗D)\mathcal{M}=W_{n+l}\omega_{X}(*D). For every kk we have the canonical morphism (9.8):

Applying the functor i!i^{!} and taking cohomology we obtain an exact sequence

as H0i!ωX(∗D)=0\mathcal{H}^{0}i^{!}\omega_{X}(*D)=0. As gr⁡iWC=0\operatorname{gr}^{W}_{i}\mathcal{C}=0 for i<n+l+1i<n+l+1,

by [saito90]*Proposition 2.26. Therefore, we obtain a short exact sequence

(see [schnellsurvey]*§23), there is a split map

The source of this maps admits the following interpretation:

Taking the corresponding piece of the Hodge filtration in (9.9) and composing it with (9.8), we obtain a morphism

Using the morphism above and switching kk to k−nk-n, we obtain a map

Composing this map with IkWl(D)⊗OH→IkWl(D)⋅OH,I_{k}^{W_{l}}(D)\otimes\mathscr{O}_{H}\to I_{k}^{W_{l}}(D)\cdot\mathscr{O}_{H}, we obtain a morphism

By construction, this map is compatible with restriction to open sets. Let V=H∖DHV=H\setminus D_{H} be the complement. When restricted to VV, this map is the identity on OV\mathscr{O}_{V}, and therefore it is an inclusion.

For the last statement, we note that a general HH is in particular non-characteristic with respect to ωX(∗D)\omega_{X}(*D). By the description of the VV-filtration in this case [saito88]*Lemma 3.5.6, the map σ\sigma is the zero map, and therefore (9.8) is a surjection. Moreover, in this case

where the first equality is the definition of M\mathcal{M} and the isomorphism is a result of Saito [saito90]*Lemma 2.25. Hence, in this case (9.10) is an isomorphism. ∎

A similar result can be obtained when HH is an intersection of several general hyperplane sections. For more details, see [olano22a]*Remark 12.