In 1958 Serre introduced the Witt-vector cohomology groups Hq(X,W)H^q(X,\mathscr{W}) of a variety XX over a perfect field of characteristic p>0p>0. He proved that for an abelian variety AA the group H1(A,WOA)H^1(A,W\mathcal{O}_A) is free of finite rank over the Witt ring WW, but his own counterexample, the product of two supersingular elliptic curves, showed that H2H^2 can fail to be finitely generated over WW. Later work converted this failure into a precise structure theory: Illusie and Raynaud proved that the failure of finite generation of the Hodge-Witt groups Hj(X,WΩi)H^j(X,W\Omega^i) is exactly measured by torsion numbers TijT^{ij}, that the VV-torsion submodule is, up to finite length, the Cartier module of a smooth connected unipotent formal group, and that ordinary varieties have all Hodge-Witt groups finitely generated. In modern terms, for an abelian variety AA of dimension gg the pp-primary torsion of the Brauer group decomposes as Br(A)[p∞]≃(Qp/Zp)r−ρ⊕U(k)\mathrm{Br}(A)[p^\infty]\simeq(\mathbb{Q}_p/\mathbb{Z}_p)^{r-\rho}\oplus U(k), where UU is a connected commutative unipotent group with dim⁡U=T0,2=h0,2−m0,2\dim U=T^{0,2}=h^{0,2}-m^{0,2} (Crew, extended to higher dimensions by Ekedahl). The fine structure of this torsion is the surviving open core: the isogeny class of UU, that is, the multiset of Witt groups WniW_{n_i} in its Serre isogeny decomposition, was determined for abelian varieties of dimension at most 33 by Yang (2025, for p≠2p\neq 2) but is open in general; the most recent treatment (Grammatica-Skorobogatov-Yang, 2025) proves that the pp-exponent of UU is at most g−1g-1 for p≠2p\neq 2, sharply, and poses this classification as its main open question. For supergeneral abelian varieties of dimension gg, Yang conjectures that UU is isogenous to ∏i=1g−1Wi\prod_{i=1}^{g-1}W_i; the conjectured value is realized by an exhibited supergeneral abelian variety in each dimension, but no proof or counterexample is known for the general statement, and the precise structure of UU up to isomorphism, even for supergeneral abelian threefolds, likewise remains open.

Background

Let kk be a perfect field of characteristic p>0p>0, and let W=W(k)W=W(k) be its ring of pp-adic Witt vectors, the complete discrete valuation ring with residue field kk and uniformizer pp. For a smooth projective variety XX over kk, Serre (1958) introduced the Witt-vector cohomology groups Hq(X,W)H^q(X,\mathscr{W}), the sheaf cohomology of the sheaf of Witt vectors, obtained as the inverse limit over nn of the cohomology of the sheaves WnOXW_n\mathcal{O}_X of length-nn truncated Witt vectors. These groups are a characteristic-pp analogue of pp-adic cohomology. Illusie (1979) embedded them into the de Rham-Witt complex WΩX∙W\Omega_X^\bullet, a system of differential graded algebras lifting the de Rham complex to all Witt-vector lengths; the cohomology groups Hj(X,WΩi)H^j(X,W\Omega^i) of its individual graded pieces are called Hodge-Witt cohomology, and Hq(X,W)H^q(X,\mathscr{W}) is the case i=0i=0. The groups Hj(X,WΩi)H^j(X,W\Omega^i) carry semilinear Frobenius and Verschiebung operators FF and VV, and they form the E1E_1 page of the slope spectral sequence converging to crystalline cohomology Hcris∙(X/W)H^\bullet_{\mathrm{cris}}(X/W), the pp-adic cohomology theory constructed by Berthelot and Grothendieck which for varieties that do not lift to characteristic zero plays the role that singular cohomology plays over the complex numbers.

Serre proved that for an abelian variety AA over kk the group H1(A,WOA)H^1(A,W\mathcal{O}_A) is a free WW-module of finite rank (his result is reproduced as Proposition 2.19 in Illusie's 1979 paper), and that the ordinary Hodge cohomology H∙(A,OA)H^\bullet(A,\mathcal{O}_A) is an exterior algebra on H1(A,OA)H^1(A,\mathcal{O}_A). In the same paper he showed, however, that finite generation fails in degree 22: if E1E_1 and E2E_2 are elliptic curves over kk with Hasse invariant 00, equivalently supersingular elliptic curves (elliptic curves whose formal Brauer group has the maximal height 22, or equivalently whose Newton polygon is a single segment of slope 1/21/2), then for the abelian surface X=E1×E2X=E_1\times E_2 the group H2(X,WOX)H^2(X,W\mathcal{O}_X) is not a finitely generated WW-module. Illusie and Raynaud (1983) later established the general facts behind this phenomenon: Hj(X,WΩi)H^j(X,W\Omega^i) is finitely generated over WW modulo its VV-torsion, the VV-torsion submodule is annihilated by a power of pp, and it is, up to a module of finite length, the Cartier module of a smooth connected unipotent formal group (the Cartier module of a formal group is the WW-module equipped with the Verschiebung operator VV that is equivalent to the formal group); moreover Hj(X,WΩi)H^j(X,W\Omega^i) is finitely generated over WW if and only if the torsion number TijT^{ij}, the invariant measuring its VV-torsion, vanishes, and a variety is called Hodge-Witt when all these groups are finitely generated. They also proved that ordinary varieties (those whose Hodge-de Rham spectral sequence degenerates with Frobenius acting bijectively on each Hj(X,Ωi)H^j(X,\Omega^i); for abelian varieties this is equivalent to the p-rank being maximal) are Hodge-Witt, which affirmatively settles the finiteness question under ordinary hypotheses. Crew (1985), in work extended to higher dimensions by Ekedahl, made the size of the torsion numerical: writing mijm_{ij} for the Hodge-Newton numbers, the slope-weighted multiplicities mij=∑i≤λ<i+1(i+1−λ)mλ+∑i−1≤λ<i(λ−i+1)mλm_{ij}=\sum_{i\leq\lambda<i+1}(i+1-\lambda)m_\lambda+\sum_{i-1\leq\lambda<i}(\lambda-i+1)m_\lambda of the crystalline Frobenius slopes, where mλm_\lambda is the multiplicity of the slope λ\lambda of Hcrisi+jH^{i+j}_{\mathrm{cris}} (in the degree-two case this is m0,2=∑0≤λ<1(1−λ)mλm^{0,2}=\sum_{0\leq\lambda<1}(1-\lambda)m_\lambda), the dimension of the unipotent part is the difference hij−mijh^{ij}-m_{ij} of the Hodge number and the Hodge-Newton number, and for surfaces T0,2T^{0,2} is upper semicontinuous in smooth proper families.

The modern form of the question passes to the Brauer group. The Brauer group Br(X)\mathrm{Br}(X) is the torsion part of the flat (fppf) cohomology group Hfl2(X,Gm)H^2_{\mathrm{fl}}(X,\mathbb{G}_m), and its pp-primary part in characteristic pp is governed by Hodge-Witt cohomology through the formal Brauer group, the Artin-Mazur formal group (the formal group pro-representing the functor sending an Artinian local kk-algebra RR to ker⁡(H2(X⊗R,Gm)→H2(X,Gm))\ker(H^2(X\otimes R,\mathbb{G}_m)\to H^2(X,\mathbb{G}_m))) and its flat variant, whose Cartier module is H2(X,WOX)H^2(X,W\mathcal{O}_X). For an abelian variety AA of dimension gg over an algebraically closed field kk, one has a decomposition Br(A)[p∞]≃(Qp/Zp)r−ρ⊕U(k)\mathrm{Br}(A)[p^\infty]\simeq(\mathbb{Q}_p/\mathbb{Z}_p)^{r-\rho}\oplus U(k), where rr is the multiplicity of slope 11 in Hcris2(A/W)H^2_{\mathrm{cris}}(A/W), ρ\rho is the Picard number (the rank of the Néron-Severi group), and UU is a connected commutative unipotent algebraic group over kk with dim⁡U=T0,2=h0,2−m0,2\dim U=T^{0,2}=h^{0,2}-m^{0,2} and h0,2=(g2)h^{0,2}=\binom{g}{2} (Yang, Theorem 2.4.2, building on the work of Crew and Ekedahl). A unipotent group is an algebraic group admitting a filtration with successive quotients isomorphic to the additive group Ga\mathbb{G}_a; a theorem of Serre says that every connected commutative unipotent group UU in characteristic pp is isogenous to (surjects onto, with finite kernel) a product of Witt vector groups ∏iWni\prod_i W_{n_i}, where WnW_n is the group of length-nn Witt vectors, and the multiset of integers nin_i, called the isogeny class of UU, is uniquely determined by, and determines, the dimensions of the finite subgroup schemes U[pn]U[p^n] killed by pnp^n for all nn. Determining the isogeny class of UU therefore amounts to computing the integers dim⁡U[pn]\dim U[p^n].

Concrete tools are available. A formula of Skorobogatov (proved in Yang's thesis for p≠2p\neq 2) identifies Br(A)[pn]\mathrm{Br}(A)[p^n] with the symmetric part Hom(A[pn],A∨[pn])sym\mathrm{Hom}(A[p^n],A^\vee[p^n])^{\mathrm{sym}} of the homomorphism group between the pnp^n-torsion group schemes of AA and its dual A∨A^\vee, modulo the image of Hom(A,A∨)sym\mathrm{Hom}(A,A^\vee)^{\mathrm{sym}}; and Yang's Theorem 4.1.2 computes dim⁡U[p]\dim U[p] from the Ekedahl-Oort type of AA (the elementary sequence classifying the Dieudonné module of A[p]A[p], equivalently the isomorphism type of the pp-torsion group scheme with its Verschiebung). Using these, and assuming p≠2p\neq 2, Yang classified the isogeny class of UU for all abelian threefolds: UU is trivial or a product of copies of Ga\mathbb{G}_a in all cases except the supergeneral ones, supersingular abelian threefolds with aa-number 11 (the aa-number is dim⁡kHom(αp,A)\dim_k\mathrm{Hom}(\alpha_p,A), where αp\alpha_p is the kernel of Frobenius on Ga\mathbb{G}_a), where UU is isogenous to Ga×W2\mathbb{G}_a\times W_2. The most recent treatment, by Grammatica, Skorobogatov, and Yang (2025), republishes the threefold classification, proves that the pp-exponent of UU (the least mm with pmU=0p^mU=0) is at most g−1g-1 for p≠2p\neq 2, with equality for one exhibited supergeneral abelian variety in each dimension gg, and shows that the isogeny class of UU is not an invariant of the isogeny class of AA; the classification in dimension g≥4g\geq 4 and the structure of UU up to isomorphism remain open.

Problem Statement

Let AA be an abelian variety of dimension gg over an algebraically closed field kk of characteristic p>0p>0, let W=W(k)W=W(k), and let UU be the connected commutative unipotent algebraic group appearing in the decomposition Br(A)[p∞]≃(Qp/Zp)r−ρ⊕U(k)\mathrm{Br}(A)[p^\infty]\simeq(\mathbb{Q}_p/\mathbb{Z}_p)^{r-\rho}\oplus U(k) of the pp-primary torsion of the Brauer group; equivalently, UU is the group whose Cartier module is, up to finite length, the VV-torsion submodule of the Hodge-Witt cohomology group H2(A,WOA)H^2(A,W\mathcal{O}_A). The dimension of UU is known in general (dim⁡U=T0,2=h0,2−m0,2\dim U=T^{0,2}=h^{0,2}-m^{0,2}, h0,2=(g2)h^{0,2}=\binom{g}{2}), its pp-exponent is known to be at most g−1g-1 for p≠2p\neq 2 (a sharp bound), and the isogeny class of UU is known for g≤3g\leq 3 (for p≠2p\neq 2). The problem is to determine the fine structure of this torsion in general:

(1a) For the abelian varieties not already covered by the known p≠2p\neq 2 classification, namely those of dimension g≥4g\geq 4 (for any prime pp) and those of dimension g≤3g\leq 3 in characteristic p=2p=2, determine the isogeny class of UU, i.e. the multiset of positive integers (ni)(n_i) such that UU is isogenous to the product of Witt vector groups ∏iWni\prod_i W_{n_i}, as a function of standard invariants of AA (Newton polygon, Ekedahl-Oort type, aa-number), or prove that the isogeny class is not determined by any function of these invariants; whether the isogeny class of UU is determined by such invariants at all is part of the question, since it is not an invariant of the isogeny class of AA. Equivalently, compute the dimensions dim⁡U[pn]\dim U[p^n] for all n≥1n\geq 1.

(1b) Prove or refute Yang's Conjecture 5.2.1: if AA is supergeneral (supersingular with aa-number 11) of dimension gg, then UU is isogenous to ∏i=1g−1Wi\prod_{i=1}^{g-1}W_i; the conjectured value is known to hold for one exhibited supergeneral abelian variety in each dimension gg, but no proof or counterexample is known in general. This sub-question is required independently of (1a): a proof that the standard invariants do not determine the isogeny class of UU does not settle the supergeneral case, and a proof of the supergeneral case does not settle the general classification.

(2) Determine the structure of UU up to isomorphism, not merely up to isogeny; this is open even for supergeneral abelian threefolds, where the isogeny class (UU is isogenous to Ga×W2\mathbb{G}_a\times W_2) is known but the precise structure is not.

More generally, in Hodge-Witt terms: for a non-ordinary (in particular supersingular) abelian variety AA, determine the VV-torsion submodule of each Hodge-Witt cohomology group Hj(A,WΩi)H^j(A,W\Omega^i) with Tij≠0T^{ij}\neq 0 as a module over the Dieudonné-type operators FF and VV on the Witt ring. The degree-22 case above, where the torsion is incarnated as the unipotent group UU, is the central and most concretely formulated instance, and the task is to settle (1a) — the isogeny class of UU for the abelian varieties not already covered by the known p≠2p\neq 2 classification, namely dimension g≥4g\geq 4 for any prime pp and dimension g≤3g\leq 3 in characteristic p=2p=2, whether in terms of Ekedahl-Oort-type data as Yang did for g≤3g\leq 3 (for p≠2p\neq 2) or by establishing that no such invariants suffice — together with (1b), Yang's Conjecture 5.2.1 in every dimension gg, and (2), the structure of UU up to isomorphism; the determination of the VV-torsion submodule of every Hj(A,WΩi)H^j(A,W\Omega^i) with Tij≠0T^{ij}\neq 0 is the general Hodge-Witt formulation of the same question, not a separate requirement.

References

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