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Hodge numbers are not derived invariants in positive characteristic

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Abstract

We study a pair of Calabi–Yau threefolds X and M, fibered in non-principally polarized Abelian surfaces and their duals, and an equivalence \(D^b(X) \cong D^b(M)\), building on work of Gross, Popescu, Bak, and Schnell. Over the complex numbers, X is simply connected while \(\pi _1(M) = (\mathbf {Z}/3)^2\). In characteristic 3, we find that X and M have different Hodge numbers, which would be impossible in characteristic 0. In an appendix, we give a streamlined proof of Abuaf’s result that the ring \(\mathrm{H}^{*}({\mathscr {O}})\) is a derived invariant of complex threefolds and fourfolds. A second appendix by Alexander Petrov gives a family of higher-dimensional examples to show that \(h^{0,3}\) is not a derived invariant in any positive characteristic.

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Notes

  1. Some readers may be interested to know that this action of \(\mathbf {Z}/6 \times \mu _6\) is related to the Schrödinger representation of the Heisenberg group. For details see Gross and Popescu’s paper, or [11, Ch. 6] for a textbook account.

  2. We will confine our attention to characteristic 0 and 3, but the behavior in characteristic \(\ge 5\) seems to be the same as the behavior in characteristic 0, while the behavior in characteristic 2 is very different: for example, the singularities of Y are not isolated, and X is not smooth.

  3. In fact we expect that the birational map is an isomorphism, but to prove this, following Schnell’s argument in [47, Lem. 5.4], would require a detailed analysis of the singular fibers of \(X \rightarrow \mathbf {P}^1\) and \(M \rightarrow \mathbf {P}^1\).

  4. Oda denotes the Cartier operator by V rather than C; see [42, Def. 5.5].

  5. We remind the reader that we have chosen a particular threefold X in a family of threefolds parametrized by \(\mathbf {P}^3\). We do not claim that every smooth member of this family is weakly ordinary, only the one we have chosen, and thus a Zariski open set of them.

  6. A finite-length Dieudonné module is called semisimple torsion if the action of F is bijective, and nilpotent torsion if the action of F is nilpotent. A general finite-length Dieudonné module can be written uniquely as an extension of semisimple torsion by nilpotent torsion. For us the nilpotent torsion will always vanish.

  7. This follows from the compatibility of Hesselholt’s de Rham–Witt HKR isomorphism [25, Thm. C] and the usual HKR isomorphism. The essential verification is the compatibility under linearization of the operator \(\delta \) [25, Def. 1.4.3] and Connes’ B operator, which is [25, Prop. 1.4.6].

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Acknowledgements

We began this project at the conference “Derived categories and geometry in positive characteristic” in Warsaw in July 2019; we thank the organizers and IMPAN for their hospitality, and Ben Antieau for stimulating initial discussions. We thank Mark Gross for advice on [23], Richard Thomas and Adrian Langer for advice on framed sheaves, and Ben Young for computer time. Addington was supported by NSF grant no. DMS-1902213. Bragg was supported by NSF grant no. DMS-1902875.

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Appendices

Appendix A. A result of Abuaf

We give a simplified account of the proof of [1, Thm. 1.3(4)].

Theorem A.1

(Abuaf) Let X and Y be smooth complex projective varieties of dimension \(\le 4\). If \(D^b(X) \cong D^b(Y)\) then \(\mathrm{H}^{*}({\mathscr {O}}_X) \cong \mathrm{H}^{*}({\mathscr {O}}_Y)\) as algebras. In particular \(h^{0,j}(X) = h^{0,j}(Y)\) for all j.

This will follow from two preparatory results:

Proposition A.2

Let X and Y be as in the statement of Theorem A.1, and let \(\Phi :D^b(X) \rightarrow D^b(Y)\) be an equivalence. Then there is a line bundle L on X such that \({{\,\mathrm{rank}\,}}(\Phi L) \ne 0\).

Lemma A.3

Let X be a smooth complex projective variety, and let

$$\begin{aligned} {{\,\mathrm{Hdg}\,}}^{*}(X) := \textstyle \bigoplus _p \mathrm{H}^{2p}(X,\mathbf {Q}) \cap \mathrm{H}^{p,p}(X) \end{aligned}$$

be the ring of Hodge classes, endowed with with the Euler pairing

$$\begin{aligned} \chi (v,w) = \int _X (v_0 - v_2 + v_4 - \cdots ) \cup (w_0 + w_2 + w_4 + \cdots ) \cup {{\,\mathrm{td}\,}}(T_X), \end{aligned}$$

which makes \(\chi (E,F) = \chi ({{\,\mathrm{ch}\,}}(E),{{\,\mathrm{ch}\,}}(F))\).

If \(\dim X \le 3\), then Chern characters of line bundles span \({{\,\mathrm{Hdg}\,}}^{*}(X)\).

If \(\dim X = 4\), then any non-zero \(v \in {{\,\mathrm{Hdg}\,}}^{*}(X)\) that is (left or right) \(\chi \)-orthogonal to all Chern characters of line bundles satisfies \(\chi (v,v) > 0\).

Proof of Lemma A.3

We omit the cases \(\dim X \le 1\).

If \(\dim X = n \ge 2\) then by the Lefschetz theorem on (1, 1)-classes we can choose irreducible divisors \(D_1, \dotsc , D_k \subset X\) such that their cohomology classes \([D_i]\) span \({{\,\mathrm{Hdg}\,}}^2(X)\). Suppose without loss of generality that \(D_1\) is ample, so \([D_1]^n = d \cdot [\text {pt}]\) for some \(d > 0\). Observe that

$$\begin{aligned} {{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_i}) = {{\,\mathrm{ch}\,}}({\mathscr {O}}_X) - {{\,\mathrm{ch}\,}}({\mathscr {O}}_X(-D_i)) = 0 + [D_i] + \cdots , \end{aligned}$$

and that any product of \({{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_i})\)s is a linear combination of Chern characters of line bundles.

If \(\dim X = 2\) then \({{\,\mathrm{Hdg}\,}}^{*}(X)\) is spanned by

$$\begin{aligned} {{\,\mathrm{ch}\,}}({\mathscr {O}}_X)&= 1 + \cdots \\ {{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_i})&= 0 + [D_i] + \cdots \\ {{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_1})^2&= 0 + 0 + d\cdot [\text {pt}]. \end{aligned}$$

If \(\dim X = 3\) then \({{\,\mathrm{Hdg}\,}}^4\) is spanned by \([D_1].[D_i]\) by the hard Lefschetz theorem, so \({{\,\mathrm{Hdg}\,}}^{*}\) is spanned by

$$\begin{aligned} {{\,\mathrm{ch}\,}}({\mathscr {O}}_X)&= 1 + \cdots \\ {{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_i})&= 0 + [D_i] + \cdots \\ {{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_1}) . {{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_i})&= 0 + 0 + [D_1].[D_i] + \cdots \\ {{\,\mathrm{ch}\,}}({\mathscr {O}}_{D_1})^3&= 0 + 0 + 0 + d\cdot [\text {pt}]. \end{aligned}$$

If \(\dim X = 4\) then in a similar way we can span

$$\begin{aligned} \mathrm{H}^0(X,\mathbf {Q}) \oplus \mathrm{H}^{1,1}(X,\mathbf {Q}) \oplus [D_1]. \mathrm{H}^{1,1}(X,\mathbf {Q}) \oplus \mathrm{H}^{3,3}(X,\mathbf {Q}) \oplus \mathrm{H}^4(X,\mathbf {Q}). \end{aligned}$$

If v is (left or right) \(\chi \)-orthogonal to this then \(v \in \mathrm{H}^{2,2}_{\mathrm{prim}}(X,\mathbf {Q})\), so if \(v \ne 0\) then \(\chi (v,v) = v_2.v_2 > 0\) by the Hodge–Riemann bilinear relations.

Proof of Proposition A.2

We have

$$\begin{aligned} {{\,\mathrm{rank}\,}}(\Phi L) = \chi (\Phi L, {\mathscr {O}}_y) = \chi (L, \Phi ^{-1} {\mathscr {O}}_y), \end{aligned}$$

where \({\mathscr {O}}_y\) is the skyscraper sheaf of some point \(y \in Y\). Suppose this rank is zero for all \(L \in {{\,\mathrm{Pic}\,}}(X)\), and let \(v={{\,\mathrm{ch}\,}}(\Phi ^{-1} {\mathscr {O}}_y) \in {{\,\mathrm{Hdg}\,}}^{*}(X)\). The Euler pairing on \({{\,\mathrm{Hdg}\,}}^{*}(X)\) is non-degenerate, so if \(\dim X \le 3\) then by Lemma A.3 we have \(v = 0\); but this contradicts the fact that \(\chi (\Phi ^{-1} {\mathscr {O}}_Y, \Phi ^{-1} {\mathscr {O}}_y) = \chi ({\mathscr {O}}_Y, {\mathscr {O}}_y) = 1\). If \(\dim X = 4\) then either \(v = 0\), which again is impossible, or \(\chi (v,v) > 0\), which contradicts the fact that \(\chi (\Phi ^{-1} {\mathscr {O}}_y, \Phi ^{-1} {\mathscr {O}}_y) = \chi ({\mathscr {O}}_y, {\mathscr {O}}_y) = 0\). \(\square \)

Proof of Theorem A.1

Because \({{\,\mathrm{rank}\,}}(\Phi L) \ne 0\), the natural map of algebra objects

$$\begin{aligned} {\mathscr {O}}_Y \rightarrow \mathrm{R}{{\,\mathrm{{\mathscr {H}}\!{ om}}\,}}_Y(\Phi L,\Phi L) \end{aligned}$$

is split by the trace map

$$\begin{aligned} \mathrm{R}{{\,\mathrm{{\mathscr {H}}\!{ om}}\,}}_Y(\Phi L,\Phi L) \rightarrow {\mathscr {O}}_Y, \end{aligned}$$

so it induces an injection

$$\begin{aligned} \mathrm{H}^{*}({\mathscr {O}}_Y) \hookrightarrow {{\,\mathrm{Ext}\,}}^{*}_Y(\Phi L, \Phi L) ={{\,\mathrm{Ext}\,}}^{*}_X(L,L) = \mathrm{H}^{*}({\mathscr {O}}_X). \end{aligned}$$

Symmetrically we get an injection \(\mathrm{H}^{*}({\mathscr {O}}_X) \hookrightarrow \mathrm{H}^{*}({\mathscr {O}}_Y)\). \(\square \)

We remark that this proof fails in characteristic p because an equivalence might take all line bundles to objects whose rank is a multiple of p.

Appendix B. A higher-dimensional example in any characteristic (by Alexander Petrov)

Let p be an arbitrary prime number. Denote \(\overline{{\mathbb {F}}}_p\) by k.

Theorem A.1

There exist smooth projective derived equivalent varieties \(X_1, X_2\) over k such that

$$h^{0,3}(X_1)\ne h^{0, 3}(X_2)$$

Moreover, for both \(i=1,2\) the variety \(X_i\) satisfies the following properties:

  1. (a)

    \(X_i\) can be lifted to a smooth formal scheme \({\mathfrak {X}}_i\) over W(k) such that Hodge cohomology groups \(H^r({\mathfrak {X}}_i,\Omega ^s_{{\mathfrak {X}}_i/W(k)})\) are torsion-free for all rs.

  2. (b)

    The Hodge-to-de Rham spectral sequence for \(X_i\) degenerates at the first page.

  3. (c)

    The crystalline cohomology groups \(H^n_{{{\,\mathrm{cris}\,}}}(X_i/W(k))\) are torsion-free for all n.

  4. (d)

    The Hochschild-Kostant-Rosenberg spectral sequence for \(X_i\) degenerates at the second page. That is, there exists an isomorphism \({{\,\mathrm{HH}\,}}_n(X_i/k)\simeq \bigoplus \limits _{s}H^s(X_i,\Omega ^{n+s}_{X_i/k})\) for every n.

  5. (e)

    \(X_i\) cannot be lifted to a smooth algebraic scheme over W(k).

The varieties \(X_1,X_2\) are both obtained as approximations of the quotient stack associated to a finite group acting on an abelian variety. The key to the construction is the appropriate choice of such finite group action that relies on complex multiplication and Honda-Tate theory.

Let \(G= \mathbf {Z}/l\mathbf {Z}\) be the cyclic group of order l where l is an arbitrary odd prime divisor of a number of the form \(p^{2r}+1\), for an arbitrary \(r\ge 1\).

Proposition A.2

There exists an abelian variety A over k equipped with an action of G by endomorphisms of A such that

$$\begin{aligned} \dim _k H^3(A,{\mathscr {O}}_A)^{G}\ne \dim _k H^3(\widehat{A},{\mathscr {O}}_{\widehat{A}})^G \end{aligned}$$
(B.1)

Here \(\widehat{A}\) denotes the dual abelian variety. Moreover, A can be lifted to a formal abelian scheme \({\mathfrak {A}}\) over W(k) together with an action of G.

Proof

Take \(A={\mathfrak {Z}}\times _{W(k')}k\) with \({\mathfrak {Z}}\), \(k'\) provided by [44], Proposition 3.1. The inequality (B.1) follows because there are G-equivariant isomorphisms \(H^3(\widehat{A},{\mathscr {O}})\simeq \Lambda ^3H^1(\widehat{A},{\mathscr {O}}_{\widehat{A}})\simeq \Lambda ^3 (H^0(A,\Omega ^1_{A/k})^{\vee })\simeq H^0(A,\Omega ^3_{A/k})^{\vee }\) (the last isomorphism exists even if \(p=3\)) and \(\dim _k H^0(A,\Omega ^3_{A/k})^G=\dim _k (H^0(A,\Omega ^3_{A/k})^{\vee })^G\) as the order of G is prime to p. \(\square \)

This proposition is specific to positive characteristic. For an abelian variety B equipped with an action of a finite group \(\Gamma \) over a field F of characteristic zero there must exist \(\Gamma \)-equivariant isomorphisms \(H^i(B,\Omega ^{j}_{B/F})\simeq H^i(\widehat{B},\Omega ^j_{\widehat{B}/F})^{\vee }\) for all ij as follows either from Hodge theory or thanks to the existence of a separable \(\Gamma \)-invariant polarization on B.

A more subtle feature of this construction is that it is impossible to find an abelian variety B with an action of a finite group \(\Gamma \) with \(p\not \mid |\Gamma |\) that would have \(\dim _k H^i(B,{\mathscr {O}}_B)^{\Gamma }\ne \dim _k H^i(\widehat{B},{\mathscr {O}}_{\widehat{B}})^{\Gamma }\) for \(i=1\) or \(i=2\). This can be deduced from Corollary 2.2 of [44] applied to an approximation of the stack \([{\mathfrak {B}}/G]\) where \({\mathfrak {B}}\) is a formal \(\Gamma \)-equivariant lift of B that exists by Grothendieck-Messing theory combined with the fact that the order of \(\Gamma \) is prime to p.

Proof of Theorem A.1

Let A be the abelian variety provided by Proposition A.2. By Proposition 15 of [48] there exists a smooth complete intersection Y of dimension 4 over k equipped with a free action of G. The diagonal action of G on the product of \(A\times Y\) is free as well.

Define \(X_1=(A\times Y)/G\) and \(X_2=(\widehat{A}\times Y)/G\) where \(\widehat{A}\) is the dual abelian variety of A equipped with the induced action of G. In both cases the quotient is taken with respect to the free diagonal action. The equivalence of \(D^b(X_1)\) and \(D^b(X_2)\) will follow from the Mukai equivalence between derived categories of an abelian scheme and its dual. Indeed, consider \(X_1\) and \(X_2\) as abelian schemes over Y/G. The base changes of both \({{\,\mathrm{Pic}\,}}^0_{Y/G}(X_1)\) and \(X_2\) along \(Y\rightarrow Y/G\) are isomorphic to \(\widehat{A}\times Y\) compatibly with the G-action. By étale descent, \({{\,\mathrm{Pic}\,}}^0_{Y/G}(X_1)\simeq X_2\) as abelian schemes over Y/G. Proposition 6.7 of [9] implies that \(D^b(X_1)\simeq D^b(X_2)\).

Next, we compare the Hodge numbers of \(X_1\) and \(X_2\). By Théorème 1.1 of Exposé XI [18] we have \(H^i(Y,{\mathscr {O}}_Y)=0\) for \(1\le i\le 3\). Hence, there are G-equivariant identifications \(H^3(A\times Y,{\mathscr {O}}_{A\times Y})\simeq H^3(A,{\mathscr {O}}_A)\) and \(H^3(\widehat{A}\times Y,{\mathscr {O}}_{\widehat{A}\times Y})\simeq H^3(\widehat{A},{\mathscr {O}}_{\widehat{A}})\). Since G acts freely on both \(A\times Y\) and \(\widehat{A}\times Y\), the projections \(A\times Y\rightarrow X_1\) and \(\widehat{A}\times Y\rightarrow X_2\) are étale G-torsors and, since the order of G is prime to p, we have \(H^3(X_1,{\mathscr {O}}_{X_1})\simeq H^3(A\times Y,{\mathscr {O}}_{A\times Y})^G\) and \(H^3(X_2,{\mathscr {O}}_{X_2})\simeq H^3(\widehat{A}\times Y,{\mathscr {O}}_{\widehat{A}\times Y})^G\).

The inequality (B.1) therefore says that \(h^{0,3}(X_1)\ne h^{0,3}(X_2)\). Condition (a) can be fulfilled as it is possible to choose Y that lifts to a smooth projective scheme over W(k) together with an action of G, by Proposition 4.2.3 of [46]. Denote by \({\mathfrak {X}}_1\) and \({\mathfrak {X}}_2\) the resulting formal schemes over W(k) lifting \(X_1\) and \(X_2\). Since \({\mathfrak {X}}_i\) for \(i=1,2\) can be presented as a quotient by a free action of G of a product of an abelian scheme with a complete intersection, the Hodge cohomology modules \(H^r({\mathfrak {X}}_i,\Omega ^s_{{\mathfrak {X}}_i/W(k)})\) are free for all rs.

Both properties (b) and (d) would be immediate if we had \(\dim _k X_i\le p\) but this is not always possible to achieve. Instead, we can argue using the lifts \({\mathfrak {X}}_i\). For (b), consider the Hodge-Tate complex . By Proposition 4.15 of [10] there is a morphism in the derived category of \({\mathfrak {X}}_i\) that induces an isomorphism on first cohomology. Taking n-th tensor power of s and precomposing it with the antisymmetrization map \(\Omega ^n_{{\mathfrak {X}}_i/W(k)}\rightarrow (\Omega ^{1}_{{\mathfrak {X}}_i/W(k)})^{\otimes n}\) we obtain maps that induce a quasi-isomorphism . In particular, the differentials in the Hodge-Tate spectral sequence vanish modulo torsion. But, as we established above, the Hodge cohomology of \({\mathfrak {X}}_i\) has no torsion, so the Hodge-Tate spectral sequence degenerates at the second page. Therefore the conjugate spectral sequence for \(X_i\) degenerates at the second page as well and, equivalently, the Hodge-to-de Rham spectral sequence degenerates at the first page.

Similarly, for (d) consider the Hochschild-Kostant-Rosenberg spectral sequence \(E_2^{r,s}=H^r({\mathfrak {X}}_i,\Omega ^{-s}_{{\mathfrak {X}}_i/W(k)})\) converging to \({{\,\mathrm{HH}\,}}_{-r-s}({\mathfrak {X}}_i/W(k))\). There exist maps \(\varepsilon _n:\Omega ^n_{{\mathfrak {X}}_i/W(k)}[n]\rightarrow {{\,\mathrm{HH}\,}}({\mathfrak {X}}_i/W(k))\) into the Hochschild complex inducing multiplication by n! on the n-th cohomology: \(\varepsilon _n=n!:\Omega ^n_{{\mathfrak {X}}_i/W(k)}\rightarrow {\mathscr {H}}^{-n}({{\,\mathrm{HH}\,}}({\mathfrak {X}}_i/W(k)))\simeq \Omega ^n_{{\mathfrak {X}}_i/W(k)}\). Therefore, the HKR spectral sequence always degenerates modulo torsion, hence degenerates at the second page in our case. Passing to the mod p reduction gives (d).

The property (c) follows from (a) and (b) as \(H^n_{{{\,\mathrm{cris}\,}}}(X_i/W(k))\simeq H^n_{{{\,\mathrm{dR}\,}}}({\mathfrak {X}}_i/W(k))\).

Finally, to prove (e), note that by the same computation as above one sees that \(h^{0,3}(X_1)=h^{3,0}(X_2)\ne h^{0,3}(X_2)=h^{3,0}(X_1)\) so both \(X_1\) and \(X_2\) violate Hodge symmetry. Denote by K the fraction field of W(k). If \({\mathscr {X}}_i\) is a smooth scheme over W(k) lifting \(X_i\) then we have

$$\begin{aligned} \dim _{K}H^r({\mathscr {X}}_{i,K},\Omega ^s_{{\mathscr {X}}_{i,K}/K})\le \dim _k H^r(X_i,\Omega ^s_{X_i/k}) \end{aligned}$$
(B.2)

for all rs by semi-continuity while \(\dim _K H^n_{{{\,\mathrm{dR}\,}}}({\mathscr {X}}_{i,K}/K)=\dim _k H^n_{{{\,\mathrm{dR}\,}}}(X_i/k)\) because \(H^n_{{{\,\mathrm{dR}\,}}}({\mathscr {X}}_i/W(k))\simeq H^n_{{{\,\mathrm{cris}\,}}}(X_i/W(k))\) is torsion-free for all n. Since Hodge-to-de Rham spectral sequences for \(X_i\) and \({\mathscr {X}}_{i,K}\) degenerate at the first page, we deduce that \(\sum \limits _{r,s}\dim _{K}H^r({\mathscr {X}}_{i,K},\Omega ^s_{{\mathscr {X}}_{i,K}/K}) =\sum \limits _{r,s}\dim _k H^r(X_i,\Omega ^s_{X_i/k})\) so (B.2) is in fact equality for all rs. But this means that the smooth proper algebraic variety \({\mathscr {X}}_{i,K}\) over a field of characteristic zero violates Hodge symmetry which is impossible. \(\square \)

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Addington, N., Bragg, D. & Petrov, A. Hodge numbers are not derived invariants in positive characteristic. Math. Ann. 387, 847–878 (2023). https://doi.org/10.1007/s00208-022-02474-w

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