Abstract
Let \({\mathscr {X}} \rightarrow C\) be a non-isotrivial and generically ordinary family of K3 surfaces over a proper curve C in characteristic \(p \ge 5\). We prove that the geometric Picard rank jumps at infinitely many closed points of C. More generally, suppose that we are given the canonical model of a Shimura variety \({\mathcal {S}}\) of orthogonal type, associated to a lattice of signature (b, 2) that is self-dual at p. We prove that any generically ordinary proper curve C in \({\mathcal {S}}_{{\overline{{\mathbb {F}}}}_p}\) intersects special divisors of \({\mathcal {S}}_{{\overline{{\mathbb {F}}}}_p}\) at infinitely many points. As an application, we prove the ordinary Hecke orbit conjecture of Chai–Oort in this setting; that is, we show that ordinary points in \({\mathcal {S}}_{{\overline{{\mathbb {F}}}}_p}\) have Zariski-dense Hecke orbits. We also deduce the ordinary Hecke orbit conjecture for certain families of unitary Shimura varieties.
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Notes
Note that the Picard lattice of a K3 surface is equipped with a non-degenerate quadratic form arising from the intersection pairing. The discriminant of the Picard lattice is defined to be the discriminant of this quadratic form.
The special divisors Z(d) and \(Z(m^2d)\) are in the same Hecke orbit.
The conjecture was made in the PEL case, but is expect to hold for Hodge type Shimura varieties too, which includes the case of PEL Shimura varieties.
Being \(\mu \)-ordinary means that this point lies in the open Newton stratum of \({\mathcal {S}}_{{\bar{{\mathbb {F}}}}_p}\) and it means ordinary if the ordinary locus in \({\mathcal {S}}_{{\bar{{\mathbb {F}}}}_p}\) is nonempty, which will be the case for us in the rest of the paper.
We drop the ones which do not make sense. For instance, if p is invertible in T, we drop \({\mathrm {cris}}\); if \(T_{\mathbb {Q}}=\emptyset \), we drop B.
By [24, Lem. 4.2.4], this definition of being supersingular is equivalent to that the corresponding Kuga–Satake abelian variety is supersingular.
We note that our notation differs from Ogus’ by a Tate twist, so our \(F^1_{\text {con}}\) corresponds to Ogus’ \(F^2_{\text {con}}\)
By [39, p. 327], \(t_P/2\) is the Artin invariant if \(A_P\) is the Kuga–Satake abelian variety associated to a K3 surface.
All empty entries in the matrix are 0.
Comparing to [33, §3], §3.2.1 in loc. cit. is a special case of the split even dimensional case, §3.2.2 in loc. cit. is a special case of the non-split even dimensional case, and §3.3 in loc. cit. is a special case of the odd dimensional case.
We would like to thank the anonymous referee for pointing out this reference to us.
For more details, see [33, Proof of Thm. 5.1.2 assuming Prop. 5.1.3].
Here we have \(p^{r+2}\) instead of \(p^{r+1}\) is due to the fact that \({{\,\mathrm{Span}\,}}_W\{e_i,f_i, e'_j, f'_j\}\ne {\mathbb {L}}\) but we still have \({{\,\mathrm{Span}\,}}_W\{e_i,f_i, e'_j, f'_j\}\supset p {\mathbb {L}}\).
Note that we also consider B(x) and \(K_i\) as the zeroth \(\sigma \)-twist of themselves.
Here and also in the statement of Theorem 5.15, by the Newton stratum associated to \(\nu \) in Kottwitz’s set, we mean the closed subscheme in the Shimura variety parametrizing points whose Newton points/polygons \(\nu '\le \nu \) with respect to the partial order in Kottwitz’s set; equivalently, this closed subscheme is the Zariski closure of the locally closed subscheme parametrizing points whose Newton points/polygons are exactly \(\nu \). We refer to this locally closed subscheme as the open Newton stratum.
There is another possible choice with \(\lambda \) replaced by \(-\lambda \); given the computation is the same for both cases, we will just work with the first case.
Indeed, by [46, Lem. 4.7], every \(m\gg 1\) is representable since L is maximal.
Here we follow the convention in [32, §3.1] that we use an embedding into the group of symplectic similitudes of a symplectic space over \({\mathbb {Q}}\) which admits a self-dual \({\mathbb {Z}}\)-lattice; this embedding may be different from the one in Sect. 2.2, but can be constructed from the one in Sect. 2.2 using Zarhin’s trick as explained in [32, p. 442].
In [32] there is a twist by \(2\pi i\) which we are suppressing.
Note that by definition in [32, §2.1.11], \({\mathbf {B}}_{K_n}\otimes {\mathbb {Z}}[1/\ell ]\) is independent of n for our \(K_n\).
Here we call \({\mathbf {H}}^*\) in [32, §2.1.22] the rational closure of the cone \({\mathbf {H}}\).
This means that \([-,-]\) induces an isomorphism between \({{\,\mathrm{Span}\,}}_{{\mathbb {Z}}}\{\zeta ,\omega \}\) and \({{\,\mathrm{Hom}\,}}(I,{\mathbb {Z}})\) with \(\zeta ,\omega \) mapping to the basis dual to \(\{z,w\}\); the existence of such a basis is given by [51, Def. 2.1, Lem. 2.2].
because \({\mathcal {S}}_{{\mathbb {F}}_p}^{\mathrm {BB}}\) is projective by [32, Thm. 3]
More precisely, as explained on [2, p. 434] that \({\mathcal {Z}}(m)_{{\mathbb {Q}}}\) is a finite disjoint union of GSpin Shimura varieties associated to quadratic spaces isomorphic to \((v^\perp , Q|_{v^\perp })\subset (V,Q)\), where \(v\in L\) with \(Q(v)=m\); since \(p\not \mid m\), then \((v^\perp , Q|_{v^\perp })\) is self-dual at p and the embedding \(v^\perp \subset V\) also induces a hyperspecial level for the Shimura variety associated to \(v^\perp \). By [2, Prop. 4.4.2] (or [31, Cor. 6.23]), \({\mathcal {Z}}(m)\) is normal and flat and thus is the disjoint union of canonical integral models of the GSpin Shimura varieties associated to isomorphism classes of \(v^\perp \) with \(Q(v)=m\).
Even though [7] works with principal polarization case, since we work with hyperspecial level at p, the description also applies to our case here.
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Acknowledgements
We thank George Boxer, Ching-Li Chai, Johan de Jong, Kai-Wen Lan, Keerthi Madapusi Pera, Frans Oort, Arul Shankar, Andrew Snowden, Salim Tayou, and Tonghai Yang for helpful discussions, as well as Arthur and D.W. Read for additional assistance. A.S. has been partially supported by the NSF Grant DMS-2100436 and Y.T. has been partially supported by the NSF Grant DMS-1801237. Y.T. was a chargée de recherche at CNRS and Université Paris-Saclay from February 2020 to June 2021. We would like to thank the referee for a careful and thorough reading, and for valuable suggestions which vastly improved the exposition of the paper.
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Maulik, D., Shankar, A.N. & Tang, Y. Picard ranks of K3 surfaces over function fields and the Hecke orbit conjecture. Invent. math. 228, 1075–1143 (2022). https://doi.org/10.1007/s00222-022-01097-x
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DOI: https://doi.org/10.1007/s00222-022-01097-x