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Indecomposable motivic cycles on K3K3 surfaces of degree 22

Ramesh Sreekantan    Ramesh Sreekantan
Abstract

In this paper we construct new indecomposable motivic cycles in the group H3(X,(2))H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2)) where XX is a degree 22 K3K3 surface. This generalizes our construction in [Sre22, Sre24] for Kummer surfaces of Abelian surfaces as well as the recent work of Ma and Sato [MS23] on degree 22 K3K3 surfaces.

1 Introduction

1.1 Degree 2 K3K3 surfaces

A degree 22 K3K3 surface XX is a K3K3 surface on which there is a line bundle {\mathcal{L}} such that 2=(.)=2{\mathcal{L}}^{2}=({\mathcal{L}}.{\mathcal{L}})=2. This is equivalent to the K3K3 surface being a double cover of 2{\mathds{P}}^{2} ramified at a sextic. The linear system |||{\mathcal{L}}| gives a map to 2{\mathds{P}}^{2} which is ramified at a sextic.

Conversely if SS is a sextic in 2{\mathds{P}}^{2} with at most isolated rational double point singularities, then the desingularisation of the double cover ramified at SS is a K3K3 surface of degree 22.

Generically the rank of the Neron-Severi group (the Picard number ρ(X)\rho(X)) is 11 - though there are some interesting special cases when the rank is much larger. If the sextic is a product of six lines, for instance, then the rank is 1616 and the moduli space of such K3K3 surfaces is four dimensional.

On this 44-fold there are two notable subvarieties. If the six lines are futher tangent to a conic, then the K3K3 surface is a Kummer surface of a principally polarised Abelian surface and the Picard number is 1717 [BW03]. If the six lines degenerate such that three of them are concurrent then Clingher and Malmendier show that the K3K3 surface is the Kummer surface of an Abelian surface with a polarization of type (1,2)(1,2) [CM17]. Other cases have been studied by Yu and Zheng [YZ23].

1.2 Motivic cycles

In this paper we construct elements in the motivic cohomology group H3(X,(2))H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2)) where XX is a degree 22 K3K3 surface. The group H3(X,(2))H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2)) has many avatars - it is usually defined as a graded piece of K1(X)K_{1}(X) with respect to the Adams filtration, but for us we will use the fact that it is the same as the Bloch higher Chow group CH2(X,1)CH^{2}(X,1).

The cycles we construct are generically indecomposable – namely they are non-trivial elements of the quotient of the motivic cohomology group by subgroup of cycles coming from lower graded pieces of the filtration. In a sense they are ‘new’ cycles.

In general it is not so easy to find indecomposable cycles and the discovery of them is a minor cause for celebration. They have a number of applications - from algebraicity of values of Greens functions [Mel08],[Sre22],[Sre24], [Ker13] to the Hodge-𝒟{\mathcal{D}}-conjecture [CL05], [Sre08],[Sre14] to torsion in co-dimension 22 [Mil92],[Spi99]. For varieties over number fields, the existence of indecomposable cycles is predicted by the Beilinson conjectures though there are only a few cases when these have been realised.

The method of construction is similar to that in [Sre22] where we studied the case of Abelian surfaces in some detail. The idea is to show the existence of certain rational curves on 2{\mathds{P}}^{2}. In this paper we show that the same construction can be generalised to this much larger class of varieties, The Kummer surfaces of principally polarised Abelian surfaces are special cases of K3K3 surfaces of degree 22.

As this paper was nearing completion we became aware of the preprint of Ma and Sato [MS23] where they also construct indecomposable motovic cycles in this case. Their methods of proof are quite different though. Their construction can be viewed as a special case when the rational curve is a line.

1.3 Acknowledgements

The history of this article is linked with the online seminar on K3K3 surfaces which has resulted in these proceedings. I spoke in the seminar on the construction in the article [Sre22] which was about Kummer surfaces of principally polarised Abelian surfaces, Prof. Armand Brumer was in the audience and he asked about the non-principally polarised case. When I dug into the literature I became aware of the work of Clingher and Malmendier [CM17] on the (1,2)(1,2) case and it was clear that the argument extends to that case. It soon became clear that the argument extends to the general degree 22 case as well. So I would first like to thank Devendra Tiwari and the rest of the organisers for inviting me to speak and second would like to thank Armand Brumer for his comment. I would also like to thank Shouhei Ma, Ken Sato and Subham Sarkar for their comments. Tom Graber and Ritwik Mukherjee for their help with questions on enumerative geometry and Arvind Nair for his remarks on orthogonal Shimura varieties. I would also like to thank the referee for their numerous comments and suggestions. Finally I would like to thank the Indian Statistical Institute for their support.

2 K3K3 surfaces of degree 2

2.1 K3K3 surfaces as double covers of 2{\mathds{P}}^{2} ramified at a sextic

Let XX be a K3K3 surface with a line bundle {\mathcal{L}} such that 2=2{\mathcal{L}}^{2}=2. The linear system |||{\mathcal{L}}| has no fixed points and maps to 2{\mathds{P}}^{2}. This is a double cover ramified at a sextic S=SXS=S_{X}. We call SXS_{X} the associated sextic of XX. The hyperplane section on 2{\mathds{P}}^{2} pulls back to a double cover of a line ramified at six points - hence is a genus 22 curve in |||{\mathcal{L}}| [May72]. On the complement of an infinite union of closed subvarieties, the Picard number ρ(X)\rho(X) of such K3K3 surfaces is 11 generated by this curve [Sha80]. Such K3K3 surfaces are called generic.

Conversely suppose SS is a sextic in 2{\mathds{P}}^{2} with only isolated double point singularities. Then the minimal desingularisation of the double cover ramified at SS is a K3K3 surface of degree 22. If there are double points on the sextic the Picard number of the K3K3 surfaces is larger as the exceptional cycles in the desingularization give new elements of the Neron-Severi group.

The compactification of the moduli space of smooth sextics was first studied by Shah [Sha80] and more recently Yu and Zheng [YZ23] have studied the singular sextic cases.

2.2 Lattices and the Moduli of K3K3 surfaces

In this section we state some results about the moduli space of K3K3 surfaces of degree 22. These results can be found in Bruinier [Bru08]. We have followed Peterson [Pet15].

If XX is a K3K3 surface, the group H2(X,)H^{2}(X,{\mathds{Z}}) is of rank 2222. As a lattice it is

H2(X,)=U3E8(1)2H^{2}(X,{\mathds{Z}})=U^{\oplus 3}\bigoplus E_{8}(-1)^{\oplus 2}

where UU is a unimodular lattice of rank 22 and signature (1,1)(1,1) and E8(1)E_{8}(-1) is the root lattice of the Lie algebra E8E_{8} with the (1)(-1) indicating that we take the negative of the standard positive definite quadratic form. Hence this is a lattice of signature (3,19)(3,19)

In H2(X,)H^{2}(X,{\mathds{Z}}) the class of {\mathcal{L}} gives us an element {\mathcal{L}} of square 22. Let L2L_{2} be the orthogonal complement {\mathcal{L}}^{\perp} of {\mathcal{L}} in H2(X,)H^{2}(X,{\mathds{Z}}). This is a lattice of signature (2,19)(2,19)

L2=<2>U2E8(1)3L_{2}=<-2>\bigoplus U^{\oplus 2}\bigoplus E_{8}(-1)^{\oplus 3}

where <2><-2> is the rank 1 lattice generated by an element ww such that (w,w)=2(w,w)=-2.

The moduli of K3K3 surfaces of degree 22 can be realised as an orthogonal Shimura variety associated to the lattice L2L_{2} as follows.

For a lattice LL let O(L)O(L) denote the group of isometries of LL. Let L^{\hat{L}} denote the dual lattice

L^={mL|(m,n) for all nL}{\hat{L}}=\{m\in L\otimes{\mathds{Q}}|(m,n)\in{\mathds{Z}}\text{ for all }n\in L\}

The discriminant group is DL=L^/LD_{L}={\hat{L}}/L. Let O~(L^)=Ker{O(L)O(DL)}{\tilde{O}}({\hat{L}})=\operatorname{Ker}\{O(L)\rightarrow O(D_{L})\}. Let O+(L){O^{+}}(L) denote the subgroup of O(L)O(L) of spinor norm 11 and O~+(L)=O~(L)O+(L){\tilde{O}^{+}}(L)={\tilde{O}}(L)\cap{O^{+}}(L).

Let

𝒟𝒟¯={z|(z,z)=0,(z,z¯)>0}(L){\mathcal{D}}\cup\overline{{\mathcal{D}}}=\{{\mathds{C}}z|\;(z,z)=0,(z,\bar{z})>0\}\subset{\mathds{P}}(L\otimes{\mathds{C}})

Choose a component 𝒟{\mathcal{D}}. The moduli space of K3K3 surfaces of degree 22 with transcendental lattice LL is

L=O~+(L)\𝒟{\mathcal{M}}_{L}={\tilde{O}^{+}}(L)\backslash{\mathcal{D}}

An alternative description is as a quotient of the Hermitian symmetric space of O(L)O(L). If LL is of signature (2,n)(2,n) this is

=O(2,n)O(2)×O(n){\mathds{H}}=\frac{O(2,n)}{O(2)\times O(n)}

The moduli space {\mathcal{M}} is

=O~+(L)\{\mathcal{M}}={\tilde{O}^{+}}(L)\backslash{\mathds{H}}

When LL is the lattice L2L_{2} this moduli space 2{\mathcal{M}}_{2} is a 1919 dimensional variety. If one considers singular sextics, the transcendental lattice becomes smaller as the exceptional fibres are elements of the Neron-Severi group. One interesting submoduli is when the sextic SS degenerates in to six lines. Here the Picard number is 1616 as the Neron-Severi is generated by the class of {\mathcal{L}} and the 1515 exceptional fibres over the nodes of SS. The transcendental lattice is hence of signature (2,4)(2,4) and the moduli space is 44 dimensional.

In this there is a particularly interesting divisor – if the six lines are tangent to a conic. Such K3K3 surfaces have Picard number 1717 and the transcendental lattice is of signature (2,3)(2,3). The new cycle is obtained as a component of the double cover of the conic. These K3K3 surfaces are the Kummer surfaces of principaly polarised abelian surfaces and the moduli is nothing but an alternative description of the Siegel modular threefold.

There are several other moduli corresponding to nodal sextics. These are described in Yu and Zheng. [YZ23]. Some of them correspond to K3K3 double covers of del Pezzo surfaces.

2.3 K3K3 surfaces with larger Picard number

As mentioned above, when the sextic has nodal singulaties, the corresponding K3K3 surface has additional elements in the Neron-Severi group coming from the exceptional fibres. In this section we will determine another condition under which there are new elements in the Neron-Severi group. In what follows we use {\mathcal{L}} to denote the class of the line bundle {\mathcal{L}} in the Neron-Severi group. Let DD be an element of NS(X)NS(X) which is not a multiple of {\mathcal{L}}. The moduli of those K3K3 surfaces of degree 22 where the Neron-Severi group is generated by {\mathcal{L}} and DD is a divisor on 2{\mathcal{M}}_{2}.

Recall that (,)=2({\mathcal{L}},{\mathcal{L}})=2. Consider the intersection matrix of the lattice generated by {\mathcal{L}} and DD,

A=(2(.D)(.D)(D.D))A=\begin{pmatrix}2&({\mathcal{L}}.D)\\ ({\mathcal{L}}.D)&(D.D)\end{pmatrix}

Let Δ=Δ(D)=det(A)=(.D)22D2\Delta=\Delta(D)=-\det(A)=({\mathcal{L}}.D)^{2}-2D^{2} and δ=(D.)mod2\delta=(D.{\mathcal{L}})\operatorname{mod}2, so δ={0,1}\delta=\{0,1\}. From the Hodge Index theorem we have that Δ(D)0\Delta(D)\geq 0 and Δ>0\Delta>0 if and only if DD is not a multiple of {\mathcal{L}}.

The irreducible Noether-Lefschetz divisor 𝒫Δ,δ{{\mathcal{P}}}_{\Delta,\delta} is the closure of the set of polarised K3K3 surfaces where the Picard lattice is a rank 22 lattice with discriminant Δ(D)=Δ\Delta(D)=\Delta and class δ\delta.

For number theoretic applications one considers Heegner divisors which are sums of these 𝒫Δ,δ{{\mathcal{P}}}_{\Delta,\delta} for certain choices of Δ\Delta. [Pet15]. Numbers determined by them are known to appear as coefficients of modular forms.

It is known that the Picard number of a Abelian surface with real multiplication is at least 22 which translates to the corresponding Kummer surface having Picard number at least 1818. Birkenhake-Wilhelm [BW03] showed, generalizing Humbert, that this corresponds to certain special rational curves on the associated 2{\mathds{P}}^{2}. Conversely, if one has special rational curves on 2{\mathds{P}}^{2} there are additional cycles in the corresponding K3K3 surface.

Along the lines of their argument, we have the following.

Proposition 2.1.

Let XX be a K3K3 surface of degree 22 and SXS_{X} the associated sextic in 2{\mathds{P}}^{2}. Let π:X2\pi:X\rightarrow{\mathds{P}}^{2} denote the double cover of 2{\mathds{P}}^{2} ramified at SXS_{X} induced by {\mathcal{L}}. Suppose there exists a rational curve QQ of degree d6d\neq 6 in 2{\mathds{P}}^{2} such that QQ meets SXS_{X} only at points of even multiplicity - including possibly nodes of SXS_{X}.

Then QQ determines an element in the Neron-Severi group of XX whose class is not a multiple of the class of {\mathcal{L}}. In particular, the moduli point of XX lies on 𝒫Δ,δ{{\mathcal{P}}}_{\Delta,\delta} for some Δ\Delta and δ\delta.

Proof.

The Picard number of 2{\mathds{P}}^{2} is 11 so the class of QQ is a multiple of the class of the hyperplane section HH. Since it is of degree dd, Q|dH|Q\in|dH|. π(H)=\pi^{*}(H)={\mathcal{L}} hence π1(Q)|d|\pi^{-1}(Q)\in|{\mathcal{L}}^{d}|. In particular, it is not a new element. So we cannot simply use the preimage of QQ.

Let C=π1(Q)C=\pi^{-1}(Q) be the double cover of QQ induced by the map π:X2\pi:X\rightarrow{\mathds{P}}^{2}. Let η:C~C\eta:\tilde{C}\longrightarrow C denote its normalization. The ramification points of π:CQ\pi:C\longrightarrow Q are the points SXQS_{X}\cap Q. By assumption SXS_{X} and QQ meet with even multiplicity. In the double cover CC these are nodal points. In the normalization C~\tilde{C}, these are no longer ramified. Since QQ is rational the normalization C~\tilde{C} is then an unramified double cover of 1{\mathds{P}}^{1}. This cannot be irreducible as 1{\mathds{P}}^{1} is simply connected and does not have an irreducible unramified double cover. Since it is a double cover it has two components, say C~1\tilde{C}_{1} and C~2\tilde{C}_{2}. Hence C=C1C2C=C_{1}\cup C_{2} for some possibly singular rational curves C1C_{1} and C2C_{2}.

We claim the class of C1C_{1} (or C2C_{2}) is not a multiple of the class of {\mathcal{L}}. To do this we have to compute Δ(C1)\Delta(C_{1}). Recall that if C1C_{1} is a multiple of {\mathcal{L}} then Δ(C1)=0\Delta(C_{1})=0.

Let ι\iota be the involution determined by the double cover. Then ι(C1)=C2\iota(C_{1})=C_{2}. On the other hand ι\iota acts trivially on the class of {\mathcal{L}}. If the class of C1C_{1} is a multiple of the class of {\mathcal{L}} then C1C_{1} and C2C_{2} are equivalent. Then

C12=(C1.C2)=3dC_{1}^{2}=(C_{1}.C_{2})=3d

as C1C_{1} and C2C_{2} meet at the 3d3d points of intersection lying over QSXQ\cap S_{X}.

Further C1+C2=π(dH)=dC_{1}+C_{2}=\pi^{*}(dH)={\mathcal{L}}^{d}. So

(C1.)=1d(C1.(C1+C2))=1d(2C12)=6(C_{1}.{\mathcal{L}})=\frac{1}{d}(C_{1}.(C_{1}+C_{2}))=\frac{1}{d}(2C_{1}^{2})=6

This gives Δ(C1)=2C12(C1.)2=6d36\Delta(C_{1})=2C_{1}^{2}-(C_{1}.{\mathcal{L}})^{2}=6d-36. On then other hand, it is 0. This implies d=6d=6. However, we have assumed d6d\neq 6.

In fact the theorem likely holds for higher genus curves as well [BW03], Proposition 6.4. We will only be concerned with the case when the curve is rational in what follows and hence will restrict ourselves to that case.

The converse need not be true. Namely there exists 𝒫Δ,δ{{\mathcal{P}}}_{\Delta,\delta} such that the extra cycle need not be represented by a rational curve.

A rational curve QQ which meets the sextic SS at points of even multiplicity determines some nodes and orders of tangency, Let 𝒫Q{{\mathcal{P}}}_{Q} denote the component of 𝒫Δ(Q),δ{{\mathcal{P}}}_{\Delta(Q),\delta} where, for a K3K3 surface XX corresponding to a point on 𝒫Δ(Q),δ{{\mathcal{P}}}_{\Delta(Q),\delta}, there is a rational curve QXQ_{X} which meets SXS_{X} is exactly the same manner.

If SXS_{X} is smooth then the only possibility is that QXQ_{X} is tangent to SXS_{X} at some points. However, if SXS_{X} has nodes and components, PΔ(D),δP_{\Delta(D),\delta} could have more components. For instance, as mentioned above, nodal sextics correspond to interesting submoduli of the moduli of degree 22 K3K3 surfaces. In the case when the sextic is a union of six lines i\ell_{i} tangent to a conic it is known that the K3K3 surface XX is the Kummer surface of a principally polarized Abelian surface. Here the sextic has 1515 nodes qij=ijq_{ij}=\ell_{i}\cap\ell_{j} corresponding to the points of intersection of the lines. In this case Δ\Delta is called the Humbert invariant and corresponds to the moduli of Abelian surfaces with endomorphism ring containing [Δ]{\mathds{Z}}[\sqrt{\Delta}]. For a generic Kummer surface the Picard number is 1717 and on these Humbert surfaces the Picard number is at least 1818.

As an example, if there is a second conic passing thought 55 of the 1515 nodes - hence it meets five of the lines at these points and suppose it is tangent to the remaining line, then Δ=5\Delta=5 and 𝒫Δ(Q),δ{{\mathcal{P}}}_{\Delta(Q),\delta} is the moduli of Kummer surfaces of Abelian surfaces with real multiplication by (5){\mathds{Z}}({\sqrt{5}}). The conics passing through the five points q12,q23,q34,q45q_{12},q_{23},q_{34},q_{45} and q51q_{51} and tangent to 6\ell_{6} determine a component of 𝒫Δ(Q),δ{{\mathcal{P}}}_{\Delta(Q),\delta} and similarly, the conics passing through q12,q23,q34,q46,q61q_{12},q_{23},q_{34},q_{46},q_{61} and tangent to 5\ell_{5} will determine a different component. This special case of Kummer surfaces of simple Abelian surfaces was studied in some detail in [Sre22].

In the case when the sextic degenerates to six lines three of which are concurrent the K3K3 surface is the Kummer surface of an Abelian surface with polarization of type (1,2)(1,2) [CM17]. Once again the 𝒫Δ,δ{{\mathcal{P}}}_{\Delta,\delta} will correspond to Abelian surfaces with extra endomorphisms.

3 Motivic cycles

3.1 Presentation of cycles in H3(X,(2))H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2)).

Let XX be a surface over a field KK. The group H3(X,(2))H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2)) has the following presentation. It is generated by sums of the form

(Ci,fi)\sum(C_{i},f_{i})

where CiC_{i} are curves on XX and fif_{i} functions on them satisfying the co-cycle condition

div(fi)=0\sum\operatorname{div}(f_{i})=0

Equivalently these can be though of as codimensional 22 subvarieties ZZ of X×1X\times{\mathds{P}}^{1} such that

Z(X×{0}X×{})=0Z\cdot(X\times\{0\}-X\times\{\infty\})=0

The cycle given by the sum of the graphs of fif_{i} in X×1X\times{\mathds{P}}^{1} has this property.

Relations are given by the Tame symbol of a pair of functions. If ff and gg are two functions on XX, the Tame symbol of the pair

τ(f,g)=ZX1(Z,(1)ordg(Z)ordf(Z)fordg(Z)gordf(Z))\tau(f,g)=\sum_{Z\in X^{1}}\left(Z,(-1)^{\operatorname{ord}_{g}(Z)\operatorname{ord}_{f}(Z)}\frac{f^{\operatorname{ord}_{g}(Z)}}{g^{\operatorname{ord}_{f}(Z)}}\right)

satisfies the co-cycle condition and such cycles are defined to be 0 is the group. Here X1X^{1} is the set of irreducible codimensional one subvarieties.

One example of an element of this group is a cycle of the form (C,a)(C,a) where aa is a nonzero constant function and CC is a curve on XX. This trivially satisfies the cocycle condition. More generally, if L/KL/K is a finite extension and XL=X×Spec(K)Spec(L)X_{L}=X\times_{\operatorname{Spec}(K)}\operatorname{Spec}(L) then one has a product map

L/KH2(XL,(1))H1(XL,(1))L/KH3(XL,(2))NmL:KH3(X,(2))\bigoplus_{L/K}H^{2}_{{\mathcal{M}}}(X_{L},{\mathds{Q}}(1))\otimes H^{1}_{{\mathcal{M}}}(X_{L},{\mathds{Q}}(1))\longrightarrow\bigoplus_{L/K}H^{3}_{{\mathcal{M}}}(X_{L},{\mathds{Q}}(2))\stackrel{{\scriptstyle Nm_{L:K}}}{{\longrightarrow}}H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2))

The image of this is the group of decomposable cyles H3(X,(2))decH^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2))_{dec}. The group of indecomposable cycles is the quotient group

H3(X,(2))indec=H3(X,(2))/H3(X,(2))decH^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2))_{indec}=H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2))/H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2))_{dec}

In general it is not clear how to construct non-trivial elements of this group.

A way of constructing cycles in this group is as follows. Since we use it in the main construction we label it a proposition.

Proposition 3.1.

Let QQ be a nodal rational curve on XX with node PP. Let ν:Q~Q\nu:\tilde{Q}\rightarrow Q be its normalization in the blow up π:X~X\pi:\tilde{X}\longrightarrow X at PP The strict transform Q~\tilde{Q} meets the exceptional fibre EPE_{P} at two points P1P_{1} and P2P_{2}. Both Q~\tilde{Q} and EPE_{P} are rational curves. Let fPf_{P} be a function with div(fP)=P1P2\operatorname{div}(f_{P})=P_{1}-P_{2} on Q~\tilde{Q} and similarly let gPg_{P} be a function with div(gP)=P2P1\operatorname{div}(g_{P})=P_{2}-P_{1} on EPE_{P}. Then

Z~P=(Q~,fP)+(EP,gP)\tilde{Z}_{P}=(\tilde{Q},f_{P})+(E_{P},g_{P})

is an element of H3(X~,(2))H^{3}_{{\mathcal{M}}}(\tilde{X},{\mathds{Q}}(2)) and its pushforward ZP=π(Z~P)Z_{P}=\pi_{*}(\tilde{Z}_{P}) is an element of H3(X,(2))H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2)).

This is cycle is well defined up to decomposable cycles as the functions fPf_{P} and gPg_{P} are only defined up to scalars. To further determine the cycle we can choose a point on Q~\tilde{Q} and EPE_{P} each and require the value of fPf_{P} and gPg_{P} to be 11 a those points.

A priori it is not clear that if this cycle is indecomposable. We will show that is the case in many instances. For this we need to use the localization sequence in motivic cohomology.

3.2 The localization sequence

If 𝒳S{\mathcal{X}}\rightarrow S is a family of varieties over a base SS with XηX_{\eta} the generic fibre and XsX_{s} the fibre over a closed subvariety ss then one has a localization sequence relating the three.

H3(Xη,(2)sS1H2(Xs,(1))H4(𝒳,(2))\cdots\rightarrow H^{3}_{{\mathcal{M}}}(X_{\eta},{\mathds{Q}}(2)\stackrel{{\scriptstyle\partial}}{{\longrightarrow}}\bigoplus_{s\in S^{1}}H^{2}_{{\mathcal{M}}}(X_{s},{\mathds{Q}}(1))\longrightarrow H^{4}_{{\mathcal{M}}}({\mathcal{X}},{\mathds{Q}}(2))\rightarrow\cdots

where S1S^{1} denotes the set of irreducible closed subvarieties of codimension 11. The boundary map of an element Z=i(Cη,i,fη,i)Z=\sum_{i}(C_{\eta,i},f_{\eta,i}) is given as follows. Let 𝒞{\mathcal{C}} denote the closure of CηC_{\eta} in 𝒳{\mathcal{X}}. Then

(Z)=idiv𝒞i(fη,i)\partial(Z)=\sum_{i}\operatorname{div}_{{\mathcal{C}}_{i}}(f_{\eta,i})

The cocycle condition idivCη,i(fη,i)=0\sum_{i}\operatorname{div}_{C_{\eta,i}}(f_{\eta,i})=0 implies that the ‘horizontal’ divisors cancel out and only the components in some of the fibres survive.

Let 𝒳{\mathcal{X}} be a family of K3K3 surfaces. To check for indecomposability one can use the boundary map \partial. Over the algebraic closure of the base field, a decomposable cycle in H3(Xη,(2))H^{3}_{{\mathcal{M}}}(X_{\eta},{\mathds{Q}}(2)) is given by (Cη,aη)(C_{\eta},a_{\eta}) where CηC_{\eta} is a curve on XηX_{\eta} and aηa_{\eta} a constant (that is, a function on the base SS).

The boundary map is particularly simple to compute in the case of a decomposable element

((Cη,aη))=ords(aη)Cs\partial((C_{\eta},a_{\eta}))=\sum\operatorname{ord}_{s}(a_{\eta})C_{s}

where CsC_{s} is the restriction of the closure 𝒞{\mathcal{C}} of CηC_{\eta} to the fibre over ss. Hence in the boundary of decomposable elements one can obtain only those cycles in the special fibres which are the restrictions of cycles in the generic fibre. In particular, if ZηZ_{\eta} is a motivic cycle and the boundary contains cycles which are not the restriction of cyces in the generic fibre then the motivic cycle is necessarily indecomposable. We will show that that is the case for our cycles.

An alternate way, as is done in Chen-Lewis [CL05], Ma-Sato [MS23] or Sato [Sat23], is to compute the Beilinson regulator and show that, when evaluated against a particular transcendental (1,1)(1,1) form, this is non-zero. In the case when the base is the ring of integers of a glabal field or a local field, the boundary map can be thought of as a non-Archimedean regulator map and the idea is essentially the same. The transcendental form is represented by a new algebraic cycle in the special fibre. Evaluation against this form corresponds to intersecting with the new cycle. That being non-zero implies that the component of the boundary in the direction of the new cycle is non-zero. This also fits in to the philosophy espoused by Manin [Man91] that the Archimedean component of an arithmetic variety can be viewed as the ‘special fibre at \infty’.

4 Construction of the cycles on the generic K3K3 surface of degree 22.

We use Proposition 3.1 to construct infinitely many distinct cycles in the generic K3K3 surface of degree 22. Recall that if XX is a K3K3 surface whose moduli point ss lies on 𝒫Q{{\mathcal{P}}}_{Q}, there is a rational curve QQ meeting SXS_{X} at 3d3d double points. Assuming this moduli is non-empty, we construct a motivic cycle defined in a Zariski open set in the complement of this space.

To apply Proposition 3.1 we need a suitable rational curve in the generic K3K3 surface. The idea is to ‘deform’ the curve QQ which exists on the fibres over 𝒫Q{{\mathcal{P}}}_{Q} to a rational curve which exists everywhere but meets the sextic at fewer points.

4.1 A Theorem in Enumerative Geometry

There is a well known theorem in enumerative geometry [Zin05] which states the following:

Theorem 4.1.

Let NdN_{d} denote the number of rational curves of degree dd passing through 3d13d-1 points in 2{\mathds{P}}^{2} in general position. Then NdN_{d} is finite and non-zero.

Proof.

A proof of this can be found in the book by Dusa McDuff and Dieter Salamon [MS12], page 213. ∎

The numbers N1=1N_{1}=1, N2=1N_{2}=1, N3=12N_{3}=12 are classical. The precise number NdN_{d} is the celebrated theorem of Kontsevich-Manin [KM94] and Ruan-Tian [RT95].

Recall that 𝒫Q{{\mathcal{P}}}_{Q} is the submoduli of the moduli of K3K3 surfaces XX of degree 22 where there is a rational curve QQ of degree dd which meets the sextic SXS_{X} at points of even multiplicity. Since QQ is of degree dd it meets SXS_{X} at 6d6d points. However, since they meet at either ordinary double points of the sextic or points of even multiplicity, there are at most 3d3d distinct points of intersection.

If we discard one of the double points of QSXQ\cap S_{X}, we determine 3d13d-1 points. Hence the theorem above suggests that perhaps for any SXS_{X} we can find a rational curve of degree dd passing through these 3d13d-1 points.

In general it is not clear if 𝒫Q{{\mathcal{P}}}_{Q} is non-empty but we will give several examples when such submoduli exist.

We need some definitions. Let Σ6\Sigma_{6} be the space of sextic curves in 2{\mathds{P}}^{2} and let Σ6(n)\Sigma_{6}(n) be the subspace with nn nodes. A singular type ΣT\Sigma_{T} [YZ23], Section 3, is an irreducible component of Σ6(n)\Sigma_{6}(n). A sextic in ΣT\Sigma_{T} is said to be of type TT. For zΣTz\in\Sigma_{T} there are nn nodes p1(z),,pn(z)p_{1}(z),\dots,p_{n}(z) smoothly varying with zz.

We have the following theorem, the proof of which was suggested to me by Tom Graber. The proof is easier as we assume that for some XX there exists a rational curve meeting SXS_{X} at the correct number of points.

Theorem 4.2.

Consider pairs (S,Q)(S,Q) where SS is a sextic in 2{\mathds{P}}^{2} in ΣT\Sigma_{T} of singular type TT with nn nodes and QQ is a rational curve of degree dd. In general they will meet at 6d6d points. We make the following assumption:

Assumption: For some z0z_{0} in ΣT\Sigma_{T}, there exists a sextic Sz0S_{z_{0}} of type TT and and a nodal rational curve Qz0Q_{z_{0}} of degree dd such that Sz0S_{z_{0}} and Qz0Q_{z_{0}} meet at 3d+1\leq 3d+1 points of the following type

  1. 1.

    kk nodes of Sz0S_{z_{0}}, say pi1(z0),,pik(z0)p_{i_{1}}(z_{0}),\dots,p_{i_{k}}(z_{0}).

  2. 2.

    3d1k3d-1-k other points tangent to Sz0S_{z_{0}} (which could coincide to be of even multiplicity).

  3. 3.

    22 other points (which could coincide and be of one of the above types).

Then, for any sextic SzS_{z} corresponding to a point zz in ΣT\Sigma_{T}, there exists a nodal rational curves QzQ_{z} of degree dd meeting the sextic at 3d13d-1 points of even multiplicity and two other points. There are two possibilities - either 3d1k3d-1-k points of tangency and passing through the kk nodes pi1(z),,pik(z)p_{i_{1}}(z),\dots,p_{i_{k}}(z) or meeting the sextic at 3dk3d-k points of tangency and passing thought k1k-1 nodes - and both exist.

Proof.

Let d{\mathcal{M}}_{d} be the space of degree dd nodal rational curves in 2{\mathds{P}}^{2} and let ΣT\Sigma_{T} be the space of sextic curves of singular type TT. It is known that the dimension dimd=3d1\operatorname{dim}{\mathcal{M}}_{d}=3d-1. Let =d(k){\mathcal{M}}={\mathcal{M}}_{d}(k) be the subspace of d{\mathcal{M}}_{d} of rational curves passing through kk points in general position. This is of dimension 3dk13d-k-1.

Let 𝒳{\mathcal{X}} be the locus in ×ΣT{\mathcal{M}}\times\Sigma_{T} parametrizing pairs (Qz,Sz)(Q_{z},S_{z}) where QzQ_{z} meets SzS_{z} at (3d1)(3d-1) double points of which kk are the nodes pi1(z),,pik(z)p_{i_{1}}(z),\dots,p_{i_{k}}(z) of SzS_{z} and two other points. 𝒳{\mathcal{X}} is non-empty as by assumption (Sz0,Qz0)(S_{z_{0}},Q_{z_{0}}) corresponds to a point on 𝒳{\mathcal{X}}. There is a morphism

π:×ΣT6d2k\pi:{\mathcal{M}}\times\Sigma_{T}\longrightarrow{\mathcal{H}}_{6d-2k}
π(Q,S)(QS)\{pi1,,pik}\pi(Q,S)\longrightarrow(Q\cap S)\backslash\{p_{i_{1}},\dots,p_{i_{k}}\}

where 6d2k{\mathcal{H}}_{6d-2k} is the Hilbert scheme of 6d2k6d-2k points in 2{\mathds{P}}^{2}.

Let ZZ be the stratum of 6d2k{\mathcal{H}}_{6d-2k} parametrizing subschemes of 3dk13d-k-1 double points \cup 22 reduced points. Then 𝒳{\mathcal{X}} is just π1(Z)\pi^{-1}(Z). The closure Z¯\bar{Z} is an irreducible codimension (3dk1)(3d-k-1) subscheme of 6d2k{\mathcal{H}}_{6d-2k} as it is determined by choosing 3dk+13d-k+1 points - which is 6d2k+26d-2k+2 dimensional - and then 3dk13d-k-1 tangents at 3d1k3d-1-k of those points - which makes it 9d2k+19d-2k+1 dimensional. Further 6d2k{\mathcal{H}}_{6d-2k} is 12d4k12d-4k dimensional. Since 6d2k{\mathcal{H}}_{6d-2k} is smooth every irreducible component of π1(Z¯)\pi^{-1}(\bar{Z}) has codimension at most (3dk1)(3d-k-1).

From our assumption we know that for some z0z_{0} in ΣT\Sigma_{T} there is a pair (Qz0,Sz0)(Q_{z_{0}},S_{z_{0}}) in π1(Z¯)\pi^{-1}(\bar{Z}). Equivalently, the local dimension of 𝒳(×{Sz0}){\mathcal{X}}\cap({\mathcal{M}}\times\{S_{z_{0}}\}) is 0\geq 0. Looking at π\pi near (Qz0,Sz0)(Q_{z_{0}},S_{z_{0}}), since dim(𝒳)dim(ΣT)\operatorname{dim}({\mathcal{X}})\geq\operatorname{dim}(\Sigma_{T}), the map π:𝒳Z\pi:{\mathcal{X}}\rightarrow Z is flat ([Har77],Chapter III, Theorem 9.9) and the fact that the local fibre dimension is 0\geq 0 at (Qz0,Sz0)(Q_{z_{0}},S_{z_{0}}) implies all nearby fibre dimensions are 0\geq 0 . This is equivalent to the fact that there is such a pair (Qz,Sz)(Q_{z},S_{z}) for every zz in a Zariski open neighborhood of z0z_{0}. Since ΣT\Sigma_{T} is irreducible, this holds for all pairs (Qz,Sz)(Q_{z},S_{z}) with zz in ΣT\Sigma_{T}.

Remark 4.3.

In fact, we expect that the dimension is 0 - namely there are a finite non-zero number of rational curves QQ for each SS of type TT when there is a special rational curve of the same type. There are instances when the special rational curve cannot exist - for instance, one cannot have a nodal cubic meeting six lines only at points of tangency.

In general it is not clear if there exists pairs (St0,Qt0)(S_{t_{0}},Q_{t_{0}}) of the type we require, though in several special cases they are known to exist. For instance if k=0k=0 and d=2d=2, so generically SS is a smooth sextic and QQ is a conic. We know that for the Kummer surface of a principally polarised Abelian surface there is a conic tangent to the sextic (which in this case is the union of six lines) at the six lines. In particular, at five lines. Hence from the theorem above, it says that in a Zariski neigbourhood of the moduli point of the Kummer surface of an Abelian surface there exists a conic tangent to a sextic at five points. In fact, it is a theorem of Gathmann [Gat05] (Corollary 3.6) that there are 7095670956 conics tangent to a sextic at five points

If SS has nodes, for instance if SS is the union of six lines and has 1515 nodes, then the theorems of Birkenhake and Lange ([BW03], Theorems 7.1-7.4) show that for Δ\Delta of the form 2d22k+72d^{2}-2k+7 or 2d22k+82d^{2}-2k+8 there exists rational curves of degree dd passing through kk nodes and meeting the remaining lines at points of even multiplicity. In particular, there exists a rational curve of the type required passing through kk nodes and 3d1k3d-1-k points of even multiplicity.

If SS has nn-nodes with n8n\leq 8 then Yu and Zheng [YZ23] show that the desingularization of the double cover of 2{\mathds{P}}^{2} branched at SS in ΣT\Sigma_{T} is a del Pezzo surface. So this argument extends to certain families of K3K3 double covers of del Pezzo surfaces.

A related case when there is a similar theorem is 1×1{\mathds{P}}^{1}\times{\mathds{P}}^{1}. Here minimal desingularization of the double cover of ×{{\mathds{P}}\times{\mathds{P}}} ramified at a curve of degree (4,4)(4,4) is also a K3K3 surface. Here the analogous statement would be that if there existed a rational curve QQ of degree (1,n)(1,n) or (n,1)(n,1) meeting the curve at 2n+12n+1 double points then in a Zariski open set there exists such a curve.

In the special case that the curve is consists of two pairs of four parallel lines, the double cover is the Kummer surface of a product of elliptic curves, say E1E_{1} and E2E_{2}. If E1E_{1} and E2E_{2} are isogenous by an isogeny of degree nn then image of the graph of the isogeny provides a example of the special curve [Sre24].

4.2 Motivic cycles

4.2.1 Construction

We now use Theorem 4.2 to construct a motivic cycle.

Construction 4.4.

Let 𝒫Q{{\mathcal{P}}}_{Q} as above be the moduli of degree 22 K3K3 surfaces XX for which there is a rational curve QQ of degree dd meeting the associated sextic SXS_{X} at 3d3d points of even multiplicity. Let TT be a singular type and assume 𝒫QΣT{{\mathcal{P}}}_{Q}\cap\Sigma_{T} is non-empty and that for z0z_{0} in this intersection, Qz0Q_{z_{0}} meets Sz0S_{z_{0}} at kk of its nodes. Then there exists a motivic cycle

ZQzH3(Xz,(2))Z_{Q_{z}}\in H^{3}_{{\mathcal{M}}}(X_{z},{\mathds{Q}}(2))

where XzX_{z} is the K3K3 surface of degree 22 corresponding to a zz in V=ΣT\𝒫QV=\Sigma_{T}\backslash{{\mathcal{P}}}_{Q}.

This construction can be extended to get a cycle ZUZ_{U} defined in the motivic cohomology over a Zariski open set UU lying over VV in an étale cover of ΣT\Sigma_{T}.

Proof.

Let XzX_{z} denote the K3K3 surface corresponding to a point zz. Let Sz=SXzS_{z}=S_{X_{z}} be the associated sextic. Let X¯z\bar{X}_{z} denote the surface which is obtained by blowing down the exceptional cycles of XzX_{z} lying over the nodes of SzS_{z} - so X¯z\bar{X}_{z} is a double cover of 2{\mathds{P}}^{2} ramified at SzS_{z}.

If z0z_{0} lies on 𝒫QΣT{{\mathcal{P}}}_{Q}\cap\Sigma_{T}, the curve Qz0Q_{z_{0}} determines 3d3d points QSz0Q\cap S_{z_{0}}. From Theorem 4.2 above, for any zΣTz\in\Sigma_{T}, there exists a rational curve QzQ_{z} which meets SzS_{z} at 3d13d-1 points of the type determined by Qz0Sz0Q_{z_{0}}\cap S_{z_{0}}. QzQ_{z} will meet SzS_{z} at two other points szs_{z} and tzt_{z} which are not points of even multiplicity.

Let π:CzQz\pi:C_{z}\longrightarrow Q_{z} be the double cover of QzQ_{z} in X¯z\bar{X}_{z}. The normalization of CzC_{z} is a double cover of 1{\mathds{P}}^{1} ramified at two points - namely the points szs_{z} and tzt_{z} and so is an irreducible rational curve. The curve CzC_{z} has nodes at the points CzSzC_{z}\cap S_{z} and there are 3d13d-1 such nodes.

Let PzP_{z} be one of the nodes. If it is a node of SzS_{z} as well then from Proposition 3.1, using the function fPzf_{P_{z}} on the strict transform C~z\tilde{C}_{z} of CzC_{z} along with the function gPzg_{P_{z}} on the exceptional fibre EPzE_{P_{z}}, we obtain a cycle

ZQz=(C~Pz,fPz)+(EPz,gPz)H3(X¯z,(2))Z_{Q_{z}}=(\tilde{C}_{P_{z}},f_{P_{z}})+(E_{P_{z}},g_{P_{z}})\in H^{3}_{{\mathcal{M}}}(\bar{X}_{z},{\mathds{Q}}(2))

If PzP_{z} is not a node of SzS_{z} then let b:XPzXzb:X_{P_{z}}\longrightarrow X_{z} be the blow up of XzX_{z} at PzP_{z}. We can construct a function on the strict transform of CzC_{z} in XPzX_{P_{z}} as above to obtain a cycle in H3(XPz,(2))H^{3}_{{\mathcal{M}}}(X_{P_{z}},{\mathds{Q}}(2)) and push that down using bb_{*} to obtain a cycle ZQzH3(Xz,(2))Z_{Q_{z}}\in H^{3}_{{\mathcal{M}}}(X_{z},{\mathds{Q}}(2)).

We further determine ZQzZ_{Q_{z}} by requiring the function fPzf_{P_{z}} satisfy

fPz(sz)=1f_{P_{z}}(s_{z})=1

Monodromy around 𝒫Q{{\mathcal{P}}}_{Q} might take one of the points in the strict transform of CzC_{z} lying over PzP_{z} to the other, so the function ff may not be defined over the generic fibre. To rectify this, we have to go to an étale cover of the moduli space where all the sections are defined. This results in a cycle ZQUZ_{Q_{U}} define in the fibres over a Zariski open set UU which meets 𝒫Q{{\mathcal{P}}}_{Q} and one has sections PU,1P_{U,1} and PU,2P_{U,2} defined over UU which map to a node PUP_{U}.

For instance, consider the case of the conics meeting the sextic tangentially. As remarked above, Gathmann [Gat05] showed there always exists a conic meeting the sextic tangentially at five points. This conic meets the sextic at two other points. The normalisation of the double cover of this conic ramified at all the points of intersection is a double cover of 1{\mathds{P}}^{1} ramified at two points - namely tzt_{z} and szs_{z} - hence is an irreducible smooth rational curve. Using this we can construct a motivic cycle on the complement of the moduli of K3K3 surfaces where the conic meets the sextic at six points of tangency.

However, we do not have to use the theorem of Gathmann. We can instead use the fact that in the 2{\mathds{P}}^{2} corresponding to the Kummer surface of a simple principally polarized Abelian surface there is a conic meeting the six lines tangentially. Hence at least in a Zariski open neighbourhood of Kummer surfaces of Abelian surfaces there exists a conic meeting the sextic tangentially at 55 points.

In the special case when the sextic degenerates to a product of six lines - so the moduli space is 44 dimensional. The K3K3 surface is obtained by blowing up the nodes of the double cover of 2{\mathds{P}}^{2} ramified at these 66 lines. There are 1515 nodes. The generic Picard number of the degree 22 K3K3 surface XX corresponding to this type of a sextic is 1616. 1515 of those come from the exceptional fibres and one more coming from the hyperplane section.

The conic above will be tangent to 55 of the six lines and will meet the remaining line at 22 points. If these points coincide then the conic is tangent to the six lines and then one knows that corresponding K3K3 surface is the Kummer surface of an Abelian surface. And further, the Picard number is 1717 - one more cycle comes from a component of the double cover of the conic.

This is an example of the above situation - on the 44 dimensional moduli of double covers of degenerate sextics, there is a motivic cycle supported in the fibres over the complement of the moduli of Kummer surfaces. This is distinct from the cycles constructed in [Sre22] or [MS23].

In the construction we have made some choices. We chose a point to discard to obtain 3d13d-1 points and we also chose the node PUP_{U}. A different choice of point to discard results in a different rational curve QUQ_{U} but the support of the boundary is the same. Another choice of PUP_{U} will result in a different function fPUf_{P_{U}}. In the next section we show that all these choices will result in cycles with the same boundary. Interestingly, Sato [Sat23] shows that in the case of products of elliptic curves, the Archimedean regulator does depend on the choice of PUP_{U}.

As things stand, we do not know that the cycle is non zero. Our computation of the boundary will show that the cycle is generically indecomposable. In particular, that will show that it is generically non-trivial.

4.2.2 Indecomposability

We now claim that ZQUZ_{Q_{U}} in H3(XU,(2))H^{3}_{{\mathcal{M}}}(X_{U},{\mathds{Q}}(2)) is in fact an indecomposable cycle.

Recall that over 𝒫Q{{\mathcal{P}}}_{Q} the conic CUC_{U} gains a new node RQR_{Q} since sUs_{U} and tUt_{U} coincide. As a result it breaks up in to two components.

There are cycles C~𝒫Q,1\tilde{C}_{{{\mathcal{P}}}_{Q},1} and C~𝒫Q,2\tilde{C}_{{{\mathcal{P}}}_{Q},2} in the universal K3K3 surface over 𝒫Q{{\mathcal{P}}}_{Q} such that

𝒞~|𝒫Q=C~𝒫Q,1+C~𝒫Q,2+ERQ\tilde{\mathcal{C}}|_{{{\mathcal{P}}}_{Q}}=\tilde{C}_{{{\mathcal{P}}}_{Q},1}+\tilde{C}_{{{\mathcal{P}}}_{Q},2}+E_{R_{Q}}

where 𝒞~\tilde{\mathcal{C}} denotes the closure of C~U\tilde{C}_{U} in the universal K3K3 surface over the moduli space (or its blow up at PUP_{U}) and ERQE_{R_{Q}} the exceptional fibre over the node RQR_{Q}.

As explained in Section 3.2, if a cycle is decomposable, then the boundary under the connecting homomorphism of the localization sequence is the restriction of a generic cycle. If we show that the boundary is not the restriction of a generic cycle then it is is necessarily indecomposable.

Theorem 4.5.

The boundary of the cycle ZQUZ_{Q_{U}} is supported in the fibres over 𝒫Q{{\mathcal{P}}}_{Q} and

(ZQU)=C~𝒫Q,1C~𝒫Q,2.\partial(Z_{Q_{U}})=\tilde{C}_{{{\mathcal{P}}}_{Q},1}-\tilde{C}_{{{\mathcal{P}}}_{Q},2}.

The cycle C~𝒫Q,1C~𝒫Q,2\tilde{C}_{{{\mathcal{P}}}_{Q},1}-\tilde{C}_{{{\mathcal{P}}}_{Q},2} is not the restriction of a cycle in the generic fibre and hence the cycle ZQUZ_{Q_{U}} is indecomposable

Proof.

Let ZQU=(C~U,fPU)+(EPU,gPU)Z_{Q_{U}}=(\tilde{C}_{U},f_{P_{U}})+(E_{P_{U}},g_{P_{U}}) be the cycle in the generic fibre constructed in Theorem 4.4.

div(fPU)=PU,1PU,2\operatorname{div}(f_{P_{U}})=P_{U,1}-P_{U,2}

where PU,1P_{U,1} and PU,2P_{U,2} are the two points lying over PUP_{U}. We have further assumed that fPU(sU)=1f_{P_{U}}(s_{U})=1, where sUs_{U} is one of the non-singular ramified points.

The double cover π:XUKU2\pi:X_{U}\rightarrow{\mathds{P}}^{2}_{K_{U}} induces an involution ι\iota on CUC_{U} which fixes the ramified points. This involution lifts to the normalization C~U\tilde{C}_{U}. If PU,1P_{U,1} and PU,2P_{U,2} are two points lying over a singular ramified point PUP_{U}, then ι(PU,1)=PU,2\iota(P_{U,1})=P_{U,2}. Further ι\iota stabilizes the exceptional fibre: ι(EPU)=EPU\iota(E_{P_{U}})=E_{P_{U}} for any node PUP_{U}.

Let fι=fιf^{\iota}=f\circ\iota. Then fPUιf^{\iota}_{P_{U}} has divisor

div(fPUι)=PU,2PU,1=div(fPU)\operatorname{div}(f^{\iota}_{P_{U}})=P_{U,2}-P_{U,1}=-\operatorname{div}(f_{P_{U}})

hence

fPUι=cUfPUf^{\iota}_{P_{U}}=\frac{c_{U}}{f_{P_{U}}}

for some constant (function on the base) cUc_{U}. Since we have further assumed that f(sU)=1f(s_{U})=1 and ι(sU)=sU\iota(s_{U})=s_{U} we have cU1c_{U}\equiv 1.

The closure 𝒞Q{\mathcal{C}}_{Q} of C~U\tilde{C}_{U} has two components over 𝒫Q{{\mathcal{P}}}_{Q}, C~𝒫Q,1\tilde{C}_{{{\mathcal{P}}}_{Q},1} and C~𝒫Q,2\tilde{C}_{{{\mathcal{P}}}_{Q},2} and the involution ι\iota interchanges them. The closure of one of the points lying over PUP_{U} will lie on C~𝒫Q,1\tilde{C}_{{{\mathcal{P}}}_{Q},1} and the other on C~𝒫Q,2\tilde{C}_{{{\mathcal{P}}}_{Q},2}. Let P𝒫Q,iP_{{{\mathcal{P}}}_{Q},i} denote the closures of PU,iP_{U,i}. We can assume P𝒫Q,iP_{{{\mathcal{P}}}_{Q},i} lies on C~𝒫Q,i\tilde{C}_{{{\mathcal{P}}}_{Q},i}.

The closure of points sUs_{U} and tUt_{U} meet over 𝒫Q{{\mathcal{P}}}_{Q} at a point RQR_{Q} hence 𝒞Q{\mathcal{C}}_{Q} has a node at RQR_{Q}. Let 𝒞~Q\tilde{\mathcal{C}}_{Q} be the blow up of 𝒞Q{\mathcal{C}}_{Q} at RQR_{Q}. This has fibre

C~𝒫Q,1+C~𝒫Q,2+ERQ\tilde{C}_{{{\mathcal{P}}}_{Q},1}+\tilde{C}_{{{\mathcal{P}}}_{Q},2}+E_{R_{Q}}

over 𝒫Q{{\mathcal{P}}}_{Q}. The involution stabilizes ERQE_{R_{Q}} as well.

The boundary map in the localization sequence is

(ZQU)=div𝒞~Q(fPU)+divEPU(gPU).\partial(Z_{Q_{U}})=\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f_{P_{U}})+\operatorname{div}_{E_{P_{U}}}(g_{P_{U}}).

The first term is

div𝒞~Q(fPU)=+a1C~𝒫Q,1+a2C~𝒫Q,2+a3ERQ\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f_{P_{U}})={\mathcal{H}}+a_{1}\tilde{C}_{{{\mathcal{P}}}_{Q},1}+a_{2}\tilde{C}_{{{\mathcal{P}}}_{Q},2}+a_{3}E_{R_{Q}}

where {\mathcal{H}} is the closure of the ‘horizontal’ divisor div(fPU)\operatorname{div}(f_{P_{U}}). We then recall that

div𝒞~Q(fPUι)=ι(div(fPU)) and fPUι=1fPU\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f^{\iota}_{P_{U}})=\iota(\operatorname{div}(f_{P_{U}}))\text{ and }f^{\iota}_{P_{U}}=\frac{1}{f_{P_{U}}}

Therefore, on one hand

div𝒞~Q(fPUι)=ι(+a1C~𝒫Q,1+a2C~𝒫Q,2+a3ERQ)=+a1C~𝒫Q,2+a2C~𝒫Q,1+a3ERQ\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f^{\iota}_{P_{U}})=\iota({\mathcal{H}}+a_{1}\tilde{C}_{{{\mathcal{P}}}_{Q},1}+a_{2}\tilde{C}_{{{\mathcal{P}}}_{Q},2}+a_{3}E_{R_{Q}})=-{\mathcal{H}}+a_{1}\tilde{C}_{{{\mathcal{P}}}_{Q},2}+a_{2}\tilde{C}_{{{\mathcal{P}}}_{Q},1}+a_{3}E_{R_{Q}}

and on the other

div𝒞~Q(fPUι)=divC~¯PU(fPU)=a1C~𝒫Q,1a2C~𝒫Q,2a3ERQ.\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f^{\iota}_{P_{U}})=-\operatorname{div}_{\overline{\tilde{C}}_{P_{U}}}(f_{P_{U}})=-{\mathcal{H}}-a_{1}\tilde{C}_{{{\mathcal{P}}}_{Q},1}-a_{2}\tilde{C}_{{{\mathcal{P}}}_{Q},2}-a_{3}E_{R_{Q}}.

This implies a1=a2a_{1}=-a_{2} and a3=a3a_{3}=-a_{3}. Hence a3=0a_{3}=0. Let a=a1a=a_{1}. We have

div𝒞~Q(fPU)=+a(C~𝒫Q,1C~𝒫Q,2).\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f_{P_{U}})={\mathcal{H}}+a(\tilde{C}_{{{\mathcal{P}}}_{Q},1}-\tilde{C}_{{{\mathcal{P}}}_{Q},2}).

To show a0a\neq 0 we suppose a=0a=0. Then

div𝒞~Q(fPU)=\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f_{P_{U}})={\mathcal{H}}

Since div𝒞~Q(fPU)\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(f_{P_{U}}) does not contain C~𝒫Q,1\tilde{C}_{{{\mathcal{P}}}_{Q},1} it restricts to a function on C~𝒫Q,1\tilde{C}_{{{\mathcal{P}}}_{Q},1} and so

deg(divC~𝒫Q,1(fPU)|C~𝒫Q,1)=0.\operatorname{deg}(\operatorname{div}_{\tilde{C}_{{{\mathcal{P}}}_{Q},1}}(f_{P_{U}})|_{\tilde{C}_{{{\mathcal{P}}}_{Q},1}})=0.

However,

divC~𝒫Q,1(fPU)|C~𝒫Q,1)=.C~𝒫Q,1=P1,𝒫Q\operatorname{div}_{\tilde{C}_{{{\mathcal{P}}}_{Q},1}}(f_{P_{U}})|_{\tilde{C}_{{{\mathcal{P}}}_{Q},1}})={\mathcal{H}}.\tilde{C}_{{{\mathcal{P}}}_{Q},1}=P_{1,{{\mathcal{P}}}_{Q}}

which has degree 11. This is a contradiction, hence a0a\neq 0.

Finally, divEP(gP)=\operatorname{div}_{E_{P}}(g_{P})=-{\mathcal{H}} as E𝒫QE_{{{\mathcal{P}}}_{Q}} remains irreducible when zz lies on 𝒫Q{{\mathcal{P}}}_{Q}. Hence

(ZQU)=a(C~𝒫Q,1C~𝒫Q,2).\partial(Z_{Q_{U}})=a\left(\tilde{C}_{{{\mathcal{P}}}_{Q},1}-\tilde{C}_{{{\mathcal{P}}}_{Q},2}\right).

for some a0a\neq 0. In particular, since C~𝒫Q,1C~𝒫Q,2\tilde{C}_{{{\mathcal{P}}}_{Q},1}-\tilde{C}_{{{\mathcal{P}}}_{Q},2} is not the restriction of a cycle in the generic fibre, the cycle ZQZ_{Q} is indecomposable.

To compute aa we do the following. Let hh be a function on the base with divisor div(h)=𝒫QaDD\operatorname{div}(h)={{\mathcal{P}}}_{Q}-\sum a_{D}D and such that Supp(D)𝒫Q=Supp(D)\cap{{\mathcal{P}}}_{Q}=\emptyset. Such a function exists as H1H^{1} of the moduli spaces is 0 so homological and rational equivalence are the same. Let (C~U,h)(\tilde{C}_{U},h) be the decomposable cycle in H3(XU,(2))H^{3}_{{\mathcal{M}}}(X_{U},{\mathds{Q}}(2)). Then

((C~U,h))=C~𝒫Q,1+C~𝒫Q,2+ERQaD𝒞~Q,D\partial((\tilde{C}_{U},h))=\tilde{C}_{{{\mathcal{P}}}_{Q},1}+\tilde{C}_{{{\mathcal{P}}}_{Q},2}+E_{R_{Q}}-\sum a_{D}\tilde{\mathcal{C}}_{Q,D}

where 𝒞~Q,D\tilde{\mathcal{C}}_{Q,D} is the 𝒞~Q|D\tilde{\mathcal{C}}_{Q}|_{D}. These fibres are irreducible and have no intersection with cycles in the fibres over 𝒫Q{{\mathcal{P}}}_{Q}.

The function hafPUh^{-a}f_{P_{U}} has divisor

div𝒞~Q(hafPU)=+a(C~𝒫Q,1C~𝒫Q,2)a(C~𝒫Q,1+C~𝒫Q,2+ERQaD𝒞~Q,D)\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(h^{-a}f_{P_{U}})={\mathcal{H}}+a\left(\tilde{C}_{{{\mathcal{P}}}_{Q},1}-\tilde{C}_{{{\mathcal{P}}}_{Q},2}\right)-a\left(\tilde{C}_{{{\mathcal{P}}}_{Q},1}+\tilde{C}_{{{\mathcal{P}}}_{Q},2}+E_{R_{Q}}-\sum a_{D}\tilde{\mathcal{C}}_{Q,D}\right)
=2aC~𝒫Q,2aERQ+aaD𝒞~Q,D={\mathcal{H}}-2a\tilde{C}_{{{\mathcal{P}}}_{Q},2}-aE_{R_{Q}}+a\sum a_{D}\tilde{\mathcal{C}}_{Q,D}

so does not have C~𝒫Q,1\tilde{C}_{{{\mathcal{P}}}_{Q},1} in its support. We can therefore restrict the function hafPUh^{-a}f_{P_{U}} to it and

deg(div(hafPU)|C~𝒫Q,1)=0\operatorname{deg}(\operatorname{div}(h^{-a}f_{P_{U}})|_{\tilde{C}_{{{\mathcal{P}}}_{Q},1}})=0

On the other hand one has

deg(div(hafPU)|C~𝒫Q,1)=(div𝒞~Q(hafPU),C~𝒫Q,1)\operatorname{deg}(\operatorname{div}(h^{-a}f_{P_{U}})|_{\tilde{C}_{{{\mathcal{P}}}_{Q},1}})=(\operatorname{div}_{\tilde{\mathcal{C}}_{Q}}(h^{-a}f_{P_{U}}),\tilde{C}_{{{\mathcal{P}}}_{Q},1})

Since (,C~𝒫Q,1)=1({\mathcal{H}},\tilde{C}_{{{\mathcal{P}}}_{Q},1})=1, (C~𝒫Q,2,C~𝒫Q,1)=0(\tilde{C}_{{{\mathcal{P}}}_{Q},2},\tilde{C}_{{{\mathcal{P}}}_{Q},1})=0, (ERQ,C~𝒫Q,1)=1(E_{R_{Q}},\tilde{C}_{{{\mathcal{P}}}_{Q},1})=1 and (𝒞~Q,D,C~𝒫Q,1)=0(\tilde{\mathcal{C}}_{Q,D},\tilde{C}_{{{\mathcal{P}}}_{Q},1})=0 for all DD, this implies

0=1a0=1-a

Therefore a=1a=1.

5 Applications

There are some immediate consequences of the existence of such indecomposable motivic cycles. In the case of the base being a local ring, Spiess [Spi99] shows that it has some consequences for torsion in codimension 22. Here we give a rough outline of possible other applications.

5.1 Mumford’s conjecture.

Mumford conjectured that there are infinitely many rational cures on a K3K3 surface. Mori and Mukai [MM83] showed this in the complex case and Bogomolov, Hassett and Tschinkel [BHT11] showed this in the case of mixed characteristics using a delicate deformation argument deforming rational curves in special fibres to the generic fibre.

A byproduct of the construction above is that there are infinitely many rational curves on the general degree 22 K3K3 surface. The motivic cycles we have are made up of rational curves. Since the motivic cycles have boundaries on distinct moduli, the corresponding rational curves are distinct.

5.2 Hodge-𝒟{\mathcal{D}}-conjecture for K3K3 surfaces over a local field

Let XX be a variety over a local field KK with residue field kk. Let XkX_{k} denote the special fibre of a regular proper model 𝒳{\mathcal{X}} over 𝒪K{\mathcal{O}}_{K}. The Hodge 𝒟{\mathcal{D}}-conjecture asserts that the map

H3(X,(2))H2(𝒳k,(1))H^{3}_{{\mathcal{M}}}(X,{\mathds{Q}}(2))\stackrel{{\scriptstyle\partial}}{{\longrightarrow}}H^{2}_{{\mathcal{M}}}({\mathcal{X}}_{k},{\mathds{Q}}(1))

is surjective. This is equivalent to showing that for any cycle in the Neron-Severi group there is a motivic cycle bounding it.

In several cases, if XX is a surface, the rank of the Neron-Severi of the special fibre is greater than that of the general fibre. In these cases, For instance, in the case of a product of elliptic curves without CMCM, in the special fibre the Frobenius induces complex multiplication and the graph of the Frobenius is a new cycle.

In some instances, the enumerative geometry argument might work directly in mixed characteristic (at least for odd primes). For instance, the statement that there is a conic tangent to 55 lines general position is purely algebraic and extends to the mixed characteristic case.

5.3 Relations with modular forms

The Heegner divisors on the moduli space of Abelian surfaces are intimately connected with modular forms, as in the case of the theorems of Gross-Zagier [GZ86], Hirzebruch-Zagier [HZ76], van der Geer [vdG82] and Hermann [Her95].

The theorems state that Heegner divisors give rise to coefficients of modular forms. Borcherds [Bor99] showed that all these theorems can be proved in a similar manner. The idea is that to show a certain power series is a modular form of a certain weight kk, it suffies to show its coefficients satisfy relations between coefficients of modular forms of that weight. The space of ‘relations between coefficients of modular forms of weight kk’ is the space of weakly holomorphic modular forms of weight 2k2-k.

So an approach to this theorem is to relate weakly holomorphic modular forms of weight 2k2-k with ‘relations between Heegner divisors’. Borcherds did so by showing that his lift of weakly holomorphic modular forms gave rise to functions with divisoral support on Heegner divisors - or in other words a relation of rational equivalence among Heegner divisors.

There are similar theorems expected for higher codimension Heegner cycles in the universal families over these Shimura varieties. Gross and Zagier [GZ86] that Heegner divisors on a modular curve are related to modular forms of weight 32\frac{3}{2}. Zhang [Zha97] showed that Heegner cycles on self product of the universal family are related to higher weight modular forms. For instance if one consideres the threefold which is compactification of self-product the universal elliptic curve, then the Heegner cycles are related to coefficients of weight 52\frac{5}{2}.

It it intriguing to speculate if these can be proved along the lines of Borcherds thereom. The modular form formalism extends without any problem. Relations among Heegner cycles are given by elements of the motivic cohomology group so the question becomes ‘Can one construct motivic cycles from weakly holomorphic modular forms?’. Borcherds theorem is an example of this as functions are elements of the motivic cohomology group H1(Sη,(1))H^{1}_{{\mathcal{M}}}(S_{\eta},{\mathds{Q}}(1)) where SηS_{\eta} is generic point of the modular variety.

Borcherds lifts are functions, so one cannot expect it to directly work for higher codimensions. However, given a motivic cycle in the generic fibre of the the universal family one can consider its regulator. This is a current on certain forms and for a suitable choice of form varying over the family computing the regulator on it gives a function on the base. Hence one can ask whether a certain Borcherds lift of weakly holomorphic forms is the regulator of a motivic cycle. In [Sre22] and [Sre24] we provide some evidence of this for codimension 22.

In this paper what we construct are relations among codimension two cycles in the universal family of K3K3 surfaces of degree 22 and one might expect that once again there is a relation between the regulator of these cycles and Borcherds lifts of modular forms.

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