On K3 surfaces and lattices
By a lattice we mean a finite dimensional free \(\mathbb {Z}\)-module L together with a symmetric bilinear form \((-,-)\). The basic invariants of a lattice are its rank and signature. A lattice is even if \((x,x) \in 2\mathbb {Z}\) for every \(x \in L\). The direct sum
of two lattices \(L_1\) and \(L_2\) is always assumed to be orthogonal, which will be denoted by
. For a lattice \(M \subset L\), \(M_L^{\perp }\) denotes the orthogonal complement of M in L. Given two lattices L and \(L'\) and a lattice embedding \(L \hookrightarrow L'\), we call it a primitive embedding if
is torsion free.
We shall use the following lattices: the (negative definite) root lattices \(A_n\) (\(n \geqslant 1\)), \(D_m\) (\(m \geqslant 4\)), \(E_r\) (\(r = 6,7,8\)) and the hyperbolic plane U. Given a lattice L, L(n) denotes the lattice with the same underlying \(\mathbb {Z}\)-module as L but with the bilinear form multiplied by n.
Notation 3.1
Given any even lattice L, we define:
-
, the dual lattice;
-
, the discriminant group endowed with the induced quadratic form
;
-
: the determinant of the Gram matrix (i.e. the intersection matrix) with respect to an arbitrary \(\mathbb {Z}\)-basis of L;
-
O(L): the group of isometries of L;
-
\(O(q_L)\): the automorphisms of \(A_L\) that preserve the quadratic form \(q_L\);
-
\(O_{-}(L)\): the group of isometries of L of spinor norm 1 (see [29, Section 3.6]);
-
\(\widetilde{O}(L)\): the group of isometries of L that induce the identity on \(A_L\);
-
\(O^*(L) = O_{-}(L) \cap \widetilde{O}(L)\);
-
\(\Delta (L)\): the set of roots of L (\(\delta \in L\) is a root if
);
-
W(L): the Weyl group, i.e. the group of isometries generated by reflections \(s_{\delta }\) in root \(\delta \), where
.
For a surface X, the intersection form gives a natural lattice structure on the torsion-free part of \(H^2(X, \mathbb {Z})\) and on the Néron–Severi group
. For a K3 surface S, we have
, and hence
. Both \(H^2(S, \mathbb {Z})\) and
are torsion-free and the natural map
is a primitive embedding. Given any K3 surface S, \(H^2(S,\mathbb {Z})\) is isomorphic to
, the unique even unimodular lattice of signature (3, 19). We shall use \(O(S),\Delta (S),W(S)\), etc. to denote the corresponding objects of the lattice
. We also denote by \(\Delta ^+(S)\) and \(V^+(S)\) the set of effective \((-2)\) divisor classes in
and the Kähler cone of S respectively.
In our context, a polarization for a K3 surface is the class of a nef and big divisor H (and not the most restrictive notion of ample divisor, we follow the terminology in [17]) and \(H^2\) is its degree. More generally there is a notion of lattice polarization. We shall consider the period map for (lattice) polarized K3 surfaces and use the standard facts on K3 surfaces: the global Torelli theorem and the surjectivity of the period map. We also need the following theorem (see [24, p. 40] or [17, Theorem 4.8, Proposition 4.9]).
Theorem 3.2
Let H be a nef and big divisor on a K3 surface S. The linear system |H| has base points if and only if there exists a divisor D such that
and \(D^2=0\).
The K3 surfaces associated to a generic triple
We first consider the K3 surfaces arising as a double cover of
branched at a smooth quartic curve C and two different lines \(L_1\) and \(L_2\) such that \(C+L_1+L_2\) has simple normal crossings. We shall show that these K3 surfaces are naturally polarized by a certain lattice.
Denote by \(\overline{S}_{(C,L_1,L_2)}\) the double cover of
branched along \(C+L_1+L_2\). Let \(S_{(C,L_1,L_2)}\) be the K3 surface obtained as the minimal resolution of the nine singular points of \(\overline{S}_{(C,L_1,L_2)}\). Let
be the natural morphism. Note that
also factors as the composition of the blow-up of
at the singularities of \(C+L_1+L_2\) and the double cover of the blow-up branched along the strict transforms of C, \(L_1\) and \(L_2\) (see [4, Section III.7]).
Let
be the pullback of the class of a line in
. The class h is a degree 2 polarization of \(S_{(C,L_1,L_2)}\). We assume that \(C \cap L_1 = \{p_1, p_2, p_3, p_4\}\),
and
. Denote the classes of the exceptional divisors corresponding to \(p_i\), \(q_i\), and r by \(\alpha _i\), \(\beta _i\) and \(\gamma \) respectively (\(1 \leqslant i \leqslant 4\)). Let us also denote by \(l_1'\) (respectively \(l_2'\)) the class of the strict transform of \(L_1\) (respectively \(L_2\)). Note that the morphism
is given by the class
It is straightforward to check that
,
,
for \(1 \leqslant i,j \leqslant 4\). Clearly, we have
,
, and
for \(1 \leqslant i,j \leqslant 4\).
Consider the sublattice of the Picard lattice of \(S_{(C,L_1,L_2)}\) generated by the curve classes \(\gamma ,l_1',\alpha _1, \ldots , \alpha _4,l_2',\beta _1, \ldots , \beta _4\). Let
It follows from (5) that
forms a \(\mathbb {Z}\)-basis of the sublattice. The Gram matrix with respect to this basis is computed as follows:
$$\begin{aligned} \left( {\begin{array}{c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c} -2 &{} 1 &{} 0 &{} 0 &{} 0 &{} 1 &{} 0 &{} 0 &{} 0 &{} 2 \\ 1 &{} -2 &{} 1 &{} 1 &{} 1 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 \\ 0 &{} 1 &{} -2 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 \\ 0 &{} 1 &{} 0 &{} -2 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 \\ 0 &{} 1 &{} 0 &{} 0 &{} -2 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 \\ 1 &{} 0 &{} 0 &{} 0 &{} 0 &{} -2 &{} 1 &{} 1 &{} 1 &{} 0 \\ 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 1 &{} -2 &{} 0 &{} 0 &{} 0 \\ 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 1 &{} 0 &{} -2 &{} 0 &{} 0 \\ 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 1 &{} 0 &{} 0 &{} -2 &{} 0 \\ 2 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 \\ \end{array} } \right) _{\textstyle .} \end{aligned}$$
Notation 3.3
Let M be the abstract lattice of rank 10 spanned by an ordered basis
with the intersection form given by the above Gram matrix, which we will call \(G_M\). Notice that M is an even lattice. If \(S_{(C,L_1,L_2)}\) is a K3 surface obtained as above from a smooth quartic C and two lines \(L_1,L_2\) such that \(C+L_1+L_2\) has simple normal crossings, then there is a natural lattice embedding
as described before.
We set \(h = \gamma + \xi \). Observe that \(\jmath (h)\) is linearly equivalent to the pullback of a line in
via \(\pi \) and therefore, it is a base point free polarization. In particular, we have \((h,h) = 2\), \((h,l_1') = (h, l_2') = 1\), and
for
. We also let
and
.
Let us compute the discriminant group \(A_M\) and the quadratic form
.
Lemma 3.4
The discriminant group
is isomorphic to \((\mathbb {Z}/2\mathbb {Z})^{\oplus 6}\).
Proof
Let us denote by
(respectively
) the dual element of \(\alpha _i\in M\) (respectively
, for \(1 \leqslant i,j \leqslant 3\)). Recall that \(\alpha _i^*\) is defined to be the unique element of \(M^*\) such that \((\alpha _i^*, \alpha _i) = 1\) and the pairing of \(\alpha _i^*\) with any other element of the basis
is 0. We define
and \(\xi ^*\) in a similar way. The coefficients of the dual elements \(\gamma ^*\!, l_1'^*, \alpha _1^*, \alpha _2^*, \alpha _3^*, l_2'^*, \beta _1^*, \beta _2^*, \beta _3^*, \xi ^*\) (with respect to the basis
) can be read from the rows or columns of the inverse matrix \(G_M^{-1}\) of the Gram matrix \(G_M\) of M:
$$\begin{aligned} G_M^{-1}= \left( {\begin{array}{c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} \frac{1}{2} \\ 0 &{} -2 &{} -1 &{} -1 &{} -1 &{} 0 &{} 0 &{} 0 &{} 0 &{} 1 \\ 0 &{} -1 &{} -1 &{} -\frac{1}{2} &{} -\frac{1}{2} &{} 0 &{} 0 &{} 0 &{} 0 &{} \frac{1}{2} \\ 0 &{} -1 &{} -\frac{1}{2} &{} -1 &{} -\frac{1}{2} &{} 0 &{} 0 &{} 0 &{} 0 &{} \frac{1}{2} \\ 0 &{} -1 &{} -\frac{1}{2} &{} -\frac{1}{2} &{} -1 &{} 0 &{} 0 &{} 0 &{} 0 &{} \frac{1}{2} \\ 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} -2 &{} -1 &{} -1 &{} -1 &{} 1 \\ 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} -1 &{} -1 &{} -\frac{1}{2} &{} -\frac{1}{2} &{} \frac{1}{2} \\ 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} -1 &{} -\frac{1}{2} &{} -1 &{} -\frac{1}{2} &{} \frac{1}{2} \\ 0 &{} 0 &{} 0 &{} 0 &{} 0 &{} -1 &{} -\frac{1}{2} &{} -\frac{1}{2} &{} -1 &{} \frac{1}{2} \\ \frac{1}{2} &{} 1 &{} \frac{1}{2} &{} \frac{1}{2} &{} \frac{1}{2} &{} 1 &{} \frac{1}{2} &{} \frac{1}{2} &{} \frac{1}{2} &{} -\frac{1}{2} \end{array} } \right) _{\textstyle .} \end{aligned}$$
For instance,
, where we identify each element of M with its image in \(M^*\). By abuse of notation, we also use
to denote the corresponding elements in
. Observe that \(l_1'^* = l_2'^* \equiv 0 \in A_M\). It is straightforward to verify that \(A_M\) can be generated by
and hence \(A_M\) is isomorphic to \((\mathbb {Z}/2\mathbb {Z})^{ \oplus 6}\). Indeed, this follows from observing from the columns of \(G_M^{-1}\) that \(\alpha ^*_3=\gamma ^* + \alpha _1^*+\alpha _2^*\in A_M\) and \(\beta ^*_3=\gamma ^* + \beta _1^*+\beta _2^*\in A_M\).\(\square \)
Remark 3.5
We derive a formula for the quadratic form \(q_M:A_M \rightarrow \mathbb {Q}/2\mathbb {Z}\):
$$\begin{aligned}&q_M\bigl (a\gamma ^* + b\alpha _1^* + c\alpha _2^* + d\beta _1^* + e\beta _2^* + f\xi ^*\bigr )\\ {}&\;\;\equiv b^2 + c^2 +bc + d^2 + e^2 + de + (a+b+c+d+e)f - \frac{1}{2}\, f^2 \in \mathbb {Q}/2\mathbb {Z}. \end{aligned}$$
Proposition 3.6
Let S be a K3 surface. If
is a lattice embedding such that \(\jmath (h)\) is a base point free polarization and
, and
(\(1 \leqslant i,j \leqslant 3\)) all represent irreducible curves, then \(\jmath \) is a primitive embedding.
Proof
Assume that \(\jmath \) is not primitive. Then the embedding \(\jmath \) must factor through the saturation
of M which is a non-trivial even overlattice of M:
. By [26, Proposition 1.4.1], there is a bijection between even overlattices of M and isotropic subgroups of
(which are generated by isotropic elements, i.e. \(v\in A_M\) such that \(q_M(v)=0\)). Using Lemma 3.4 and Remark 3.5, it is easy to classify the isotropic elements of \(A_M\). As
and
in \(A_M\), there are only three cases to consider. We drop the embedding \(\jmath \) in the rest of the proof.
Case 1. The isotropic element is \(\gamma ^*\). From the columns of \(G_M^{-1}\) we see that \(\gamma ^* = \xi /2 \in A_M\). Hence, we have \(\xi = 2x\) for some
. But then
and
which would imply that h is not base point free by Theorem 3.2.
Case 2. The isotropic element is
where \(1 \leqslant i,j \leqslant 3\). Let us take \(\alpha _1^* + \beta _1^*\) for example. The other cases are similar. Note that
in \(A_M\). We have \(\alpha _2 + \alpha _3 + \beta _2 + \beta _3 = 2y\) for some
. Because S is a K3 surface and
, either y or \(-y\) is effective. Note that \(l_1'\), \(l_2'\), \(\alpha _i\) and
(\(1 \leqslant i,j \leqslant 3\)) are irreducible curves (by the assumption), h is nef and
. It follows that
is nef. Since
, y is effective. Because \((y,\alpha _2) = (y, \alpha _3) = (y, \beta _2) = (y, \beta _3) = -1\), we know \(\alpha _2,\alpha _3,\beta _2\) and \(\beta _3\) are in the support of y. Write \(y = m\alpha _2 + n\alpha _3 + k \beta _2 + l \beta _3 + D = (\alpha _2 + \alpha _3 + \beta _2 + \beta _3)/2\) where D is an effective divisor,
and \(m,n,k,l \geqslant 1\). But then we have a contradiction
Case 3. The isotropic element is
where \(1 \leqslant i,j \leqslant 3\). Take \(\alpha _1^* + \beta _1^* + \gamma ^*\) for example. Since \(\alpha _1^* + \beta _1^* + \gamma ^* = \alpha _2 /2+ \alpha _3/2 + \beta _2/2 + \beta _3/2 + \xi /2\) in \(A_M\), there exists an element z of
such that
. Because S is a K3 surface,
and \((z,h) = 1\), the class z represents an effective divisor. By the assumption \(l_1',l_2',\alpha _i\) and
(\(1 \leqslant i,j \leqslant 3\)) represent irreducible curves. Note that
. Let us write \(z = m\alpha _2 + n\alpha _3 + k\beta _2 + l\beta _3 + D\), where D is effective,
and \(m,n,k,l > 0\). Then we have
which implies that \((D, l_1') < 0\) and \((D, l_2') < 0\). Now we write
$$\begin{aligned} z = m\alpha _2 + n\alpha _3 + k\beta _2 + l\beta _3 + sl_1' + tl_2'+D' \end{aligned}$$
where \(D'\) is effective,
and \(m,n,k,l,s,t \geqslant 1\). But this is impossible: \(2\leqslant s+t \leqslant (z, h) = 1\). \(\square \)
Corollary 3.7
Let C be a smooth plane quartic curve and \(L_1\), \(L_2\) two distinct lines such that \(C+L_1+L_2\) has simple normal crossings and let
be the lattice embedding given in Notation 3.3. Then \(\jmath \) is a primitive embedding.
The proof of Proposition 3.6 can easily be adapted to proof the following lemma.
Lemma 3.8
Let S be a K3 surface and
be a lattice embedding. If none of \(\jmath (\xi )\),
or
(\(1 \leqslant i, i'\!, j, j' \leqslant 3\)) is divisible by 2 in
, then the embedding \(\jmath \) is primitive.
Proposition 3.9
Assume that S is a K3 surface such that
is isomorphic to the lattice M. Then S is the double cover of
branched over a reducible curve \(C + L_1 + L_2\) where C is a smooth plane quartic, \(L_1, L_2\) are lines and \(C+L_1+L_2\) has simple normal crossings.
Proof
By assumption there exist
satisfying the numerical conditions in Notation 3.3. Without loss of generality, we assume that h is nef (this can be achieved by acting by \(\pm W(S)\)). Then \(l_1'\) and \(l_2'\) are both effective (as
, \((h,l_i')=1\)). We further assume that
(\(1 \leqslant i,j \leqslant 4\)) and \(\gamma \) are effective (apply \(s_{\alpha _i}\) or
or \(s_{\gamma }\) if necessary).
As h is nef and \((h,h)=2>0\), h is a polarization of degree 2. We will show that h is base point free by reductio ad absurdum. By Theorem 3.2, there exists a divisor D such that \((D, D) = 0\) and \((h, D) = 1\). Note that this is a numerical condition. Write D as a linear combination of \(\gamma , l_1', \alpha _1, \ldots , \alpha _3, l_2', \beta _1, \ldots , \beta _3\) and \(\xi \), with coefficients \(c_1,\ldots , c_{10}\). Let \(S_{(Q,L,L')}\) be the K3 surface associated to a smooth quartic curve Q and two lines \(L,L'\) such that \(Q+L+L'\) has simple normal crossings. Find the curve classes corresponding to \(\gamma , l_1', \alpha _1, \ldots , \alpha _3, l_2', \beta _1, \ldots , \beta _3,\xi \) (as what we did at the beginning of this subsection) and consider their linear combination \(D'\) with coefficients \(c_1,\ldots , c_{10}\), the same values as in the expression for D. Then, both D and \(D'\) satisfy the same numerical conditions in S (respectively \(S_{(Q,L,L')}\)) with respect to the divisor class \(h= \gamma + \xi \). Again, by Theorem 3.2 the pull-back h of
in \(S_{(Q,L,L')}\) has base points, which gives a contradiction. So the linear system of h defines a degree two map
. Since S is a K3 surface of degree 2, the branching locus must be a sextic curve B.
Consider
. Note that \((h'\!, h')>0\) and \((h'\!, h) > 0\). We can write any effective divisor as
where \(a_i, b_i, c\in \mathbb Z\), where \(0\leqslant i\leqslant 4\). Let \(k_i= a_0/2-a_i\), \(l_i= b_0/2-b_i\) where \(1\leqslant i\leqslant 4\). It follows that
Let \(D\in \Delta (S)\) as in (6). Then
implies that
First note that when \(a_0+b_0=(D,h)=0\), then (8) gives that either
and
or \(c=0\), and all coefficients in
but one equal 0 and
. In particular,
. If \(D\in \Delta ^+(S)\cap \langle h \rangle ^{\perp }_M\), then \((D,h)=a_0+b_0=0\) which in turn implies that
.
Now suppose that \(D\in \Delta ^+(S)\) and \((h,D)>0\). Then (7) implies that \(a_0+b_0>0\) and (8) gives \(c\geqslant 0\). Then, by the arithmetic-geometric mean inequality and (8), we get
where the latter inequality follows from observing that the first summand is positive and
Hence \((h'\!,D)>0\) for all \(D\in \Delta ^+(S)\). Moreover, if \(D \subset S\) is rational and \( D \not \in \Delta ^+(S)\), then \(\pi _*(D)\ne 0\) and
. Hence, by [15, Corollary 8.1.7], \(h'\) is ample.
Because \((h'\!, l_1')=1\), the class \(l_1'\) is represented by an irreducible curve. Similarly, \(l_2',\alpha _i\) and
(\(1 \leqslant i,j \leqslant 3\)) all correspond to irreducible curves. It follows that the irreducible rational curves \(\alpha _1, \ldots , \alpha _4, \beta _1, \ldots , \beta _4\) are contracted by \(\pi \) to ordinary double points of the sextic B. Let \(L_1'\) (respectively \(L_2'\)) be the unique irreducible curve in S corresponding to the class \(l_1'\) (respectively \(l_2'\)) and set \(L_1 = \pi (L_1')\) (respectively \(L_2 = \pi (L_2')\)). Since
, the projection formula implies that \(L_1\) is a line. Moreover, the line \(L_1\) has to pass through four ordinary double points of the branched curve B since
. Similarly, \(L_2\) is also a line passing through four different ordinary double points of B. (Note that both \(L_1\) and \(L_2\) pass through the singularity of B corresponding to \(\gamma \).) By Bezout’s theorem, the two lines \(L_1\) and \(L_2\) are both components of B (otherwise we have contradictions:
and analogously for \(L_2\)).\(\square \)
Corollary 3.10
For a sufficiently general triple \((C, L_1, L_2)\) (i.e. outside the union of a countable number of proper subvarieties of the moduli space), the Picard lattice
coincides with M via the embedding \(\jmath \).
Proof
The argument in [16, Corollary 6.19] works here. Alternatively, let \(L_1\) and \(L_2\) be given by linear forms \(l_1\) and \(l_2\), respectively, and consider the elliptic fibration
defined by the function
. If \((C, L_1, L_2)\) is sufficiently general, then the pencil of lines generated by \(L_1\) and \(L_2\) only consists of lines intersecting C normally or lines tangent to C at a point. As a result, the elliptic fibration contains two reducible singular fibers of type \(I_0^*\) (i.e. with 5 components) and 12 singular fibers of type \(I_1\) (i.e. with one nodal component), where we follow Kodaira’s notation as in [4, Section V.7], [15, Section 11.1.3]. Note that the fibration admits a 2-section \(\gamma \). Consider the associated Jacobian fibration
(see for example [15, Section 11.4]). By the Shioda–Tate formula [15, Corollaries 11.3.4 and 11.4.7], the K3 surface \(S_{(C,L_1,L_2)}\) has Picard number 10 which equals the rank of M. Moreover, we have [15, Section 11, (4.5)]:
It is easy to compute that the Gram matrix \(G_M\) has determinant \((-64)\). The proposition then follows from the following standard fact on lattices (which implies
):
As
and they have the same rank and discriminant, then
.\(\square \)
Now let us consider the case when C has at worst simple singularities not contained in \(L_1+L_2\) and \(C+L_1+L_2\) has simple normal crossings away from the singularities of C. We still use \(S_{(C,L_1,L_2)}\) to denote the K3 surface obtained as a minimal resolution of the double cover of
along \(C+L_1+L_2\). The rank 10 lattice M is the same as in Notation 3.3.
Lemma 3.11
If C has at worst simple singularities not contained in \(L_1+L_2\) and \(C+L_1+L_2\) has simple normal crossings away from the singularities of C, then there exists a primitive embedding
such that \(\jmath (h)\) is a base point free degree two polarization.
Proof
Thanks to the transversal intersection, we define the embedding \(\jmath \) as in the generic case. In particular, the morphism
is defined by \(\jmath (h)\). The embedding \(\jmath \) is primitive by Proposition 3.6.\(\square \)
M-polarized K3 surfaces and the period map
In this subsection let us compute the (generic) Picard lattice M and the transcendental lattice T. Then we shall determine the period domain
and define a period map for generic triples \((C, L_1, L_2)\) via the periods of M-polarized K3 surfaces \(S_{(C, L_1, L_2)}\).
Definition 3.12
Let M be the lattice defined in Notation 3.3. An M
-polarized
K3 surface is a pair \((S, \jmath )\) such that
is a primitive lattice embedding. The embedding \(\jmath \) is called the M
-polarization of S. We will simply say that S is an M
-polarized
K3 surface when no confusion about \(\jmath \) is likely.
We now determine the lattice M and show that it admits a unique primitive embedding into the K3 lattice \(\Lambda _{K3}\).
Proposition 3.13
Let M be the lattice defined in Notation 3.3. Then M is isomorphic to the lattice \(U(2) \perp A_1^{2} \perp D_6\) and admits a unique primitive embedding (up to isometry) \(M \hookrightarrow \Lambda _{K3}\) into the K3 lattice \(\Lambda _{K3}\). The orthogonal complement
with respect to the embedding is isometric to \(U \perp U(2) \perp A_1^{2} \perp D_6\).
Proof
By [26, Corollary 1.13.3] the lattice M is uniquely determined by its invariants which can be easily computed from the Gram matrix \(G_M\) (see also Lemma 3.4 and Remark 3.5).
-
M has rank 10 and signature (1, 9).
-
The Gram matrix \(G_M\) has determinant \((-64)\).
-
The discriminant group is
with quadratic form
, where \(u,w_{2,1}^{1}\) and \(w_{2,1}^{-1}\) are the discriminant forms associated to \(U(2),E_7\) and \(A_1\) respectively (cf. [5, Section 1.5 and Appendix A] and references therein). Note that
is isomorphic to the discriminant form of \(D_6\).
By [26, Theorem 1.14.4] the lattice M admits a unique primitive embedding into \(\Lambda _{K3}\). The claim on the orthogonal complement T follows from [26, Proposition 1.6.1].\(\square \)
Remark 3.14
Note that both M and T are even indefinite 2-elementary lattices (a lattice L is 2-elementary if
for some k). One could also invoke Nikulin’s classification [26, Theorem 3.6.2] of such lattices to prove the previous proposition. Moreover, M and T are orthogonal to each other in a unimodular lattice and hence
.
The moduli space of M-polarized K3 surfaces is a quotient
for a certain Hermitian symmetric domain
of type IV and some arithmetic group \(\Gamma \) (see [8]). Fix the (unique) embedding \(M \hookrightarrow \Lambda _{K3}\) and define
to be one of the two connected components. Note that
can also be identified with
To specify the moduli of M-polarized K3 surfaces, one also needs to determine the arithmetic group \(\Gamma \). In the standard situation considered in [8] it is required that the M-polarization is pointwise fixed by the arithmetic group and one takes \(\Gamma \) to be \(O^*(T)\). In our geometric context the choice is different. Specifically, the permutations among \(\alpha _1, \ldots , \alpha _4\) and among \(\beta _1, \ldots , \beta _4\) are allowed. Observe that at the moment we view the lines \(L_1\) and \(L_2\) as labeled lines, distinguishing the tuples \((C, L_1, L_2)\) and \((C, L_2, L_1)\) and we do not consider the isometry of M induced by flipping the two lines.
Let L be an even lattice. Recall that any \(g \in O(L)\) naturally induces
by \(g^*\varphi :v \mapsto \varphi (g^{-1}v)\) (which further defines an automorphism of \(A_L\) preserving \(q_L\), therefore giving a natural homomorphism \(r_L:O(L)\rightarrow O(q_L)\)).
Lemma 3.15
The homomorphisms \(r_M:O(M) \rightarrow O(q_M)\) and \(r_T:O(T) \rightarrow O(q_T)\) are both surjective.
Proof
The lemma follows from Lemma 3.4 and [26, Theorem 1.14.2].\(\square \)
In particular, we have \(O(M) \twoheadrightarrow O(q_M) \cong O(q_T) \twoheadleftarrow O(T)\). By [26, Theorem 1.6.1, Corollary 1.5.2], an automorphism \(g_M \in O(M)\) can be extended to an automorphism of \(\Lambda _{K3}\) if and only if
. In our case, any automorphism \(g_M \in O(M)\) can be extended to an element in \(O(\Lambda _{K3})\).
Lemma 3.16
Let \(g_M\) (respectively \(g_T\)) be an automorphism of M (respectively T). If \(r_M(g_M) = r_T(g_T)\), then \(g_M\) can be lifted to \(g \in O(\Lambda _{K3})\) with \(g|_T = g_T\). The same statement holds for \(g_T\).
Proof
The proof is similar to that for [15, Proposition 14.2.6]. Take any \(x = x_M + x_T \in \Lambda _{K3}\) with \(x_M \in M^*\) and
. View \(\Lambda _{K3}\) as an overlattice of
. The corresponding isotropic subgroup (cf. [26, Section 1.4]) of
is
. Since \(x \in \Lambda _{K3}\), \(\overline{x}_M + \overline{x}_T\) is contained in
(where \(\overline{x}_M\) denotes the corresponding element of \(x_M\) in \(A_M\) and similarly for \(\overline{x}_T\)). Consider
. Note that the image of \(g_M(x_M) + g_T(x_T)\) under the map
is \(r_M(g_M)(\overline{x}_M) + r_T(g_T)(\overline{x}_T)\). Recall that \(A_M\) and \(A_T\) are identified via the natural projections
. Because \(r_M(g_M) = r_T(g_T)\), \(r_M(g_M)(\overline{x}_M) + r_T(g_T)(\overline{x}_T)\) is contained in
. In other words, we have \(g_M(x_M) + g_T(x_T) \in \Lambda _{K3}\).\(\square \)
Let \(\Sigma _{\alpha } \subset O(M)\) (respectively
) be the subgroup which permutes
(respectively the subgroup which permutes \(\{\beta _1, \ldots , \beta _4\}\)). We seek automorphisms of T which can be extended to automorphisms of \(\Lambda _{K3}\) whose restrictions to M belong to \(\Sigma _\alpha \) or \(\Sigma _\beta \). We observe that there is a natural inclusion
.
Lemma 3.17
The composition
is injective.
Proof
First let us describe the automorphisms of \(A_M\) induced by the transpositions in \(\Sigma _\alpha \) and \(\Sigma _{\beta }\). We consider \(\Sigma _\alpha \) and the case of \(\Sigma _\beta \) is analogous. The image of the transposition \((\alpha _i\alpha _i')\) (with \(1 \leqslant i \ne i' \leqslant 3\)) defines the element \(r_M((\alpha _i\alpha _i'))\) in \(O(q_M)\) given by \(\alpha _i^* \mapsto \alpha _{i'}^*\), \(\alpha _{i'}^* \mapsto \alpha _i^*\), leaving \(\gamma ^*\!,\alpha _{i''}^*\) (
),
(\(1 \leqslant j \leqslant 3\)) and \(\xi ^*\) invariant.
The automorphism of \(A_M\) induced by the transposition \((\alpha _1\alpha _4)\) between \(\alpha _1\) and \(\alpha _4\) is given by
$$\begin{aligned}&\alpha _2^* \mapsto \alpha _3^* + \gamma ^* \equiv \alpha _1^* + \alpha _2^*,&\alpha _3^* \mapsto \alpha _2^* + \gamma ^* \equiv \alpha _1^* + \alpha _3^*,&\xi ^* \mapsto \xi ^* + \alpha _1^*, \end{aligned}$$
and
(\(1 \leqslant j \leqslant 3\)) are invariant by this action. The case of transpositions \((\alpha _2\alpha _4)\) and \((\alpha _3\alpha _4)\) is analogous. As it is well-known, the transpositions generate \(\Sigma _\alpha \) and \(\Sigma _\beta \). It is easy to compute the image of
in \(O(q_M)\) using the previous descriptions.
Let \(g_\alpha \in \Sigma _\alpha \) and \(g_\beta \in \Sigma _\beta \). Now we describe how to univocally recover
from the induced action \(\overline{g}\) on \(A_M\). In particular, this will show that the composed map
is injective. Consider \(\overline{g}(\xi ^*)\). Because
, the induced action \(\overline{g}\) sends \(\xi ^*\) to an element \(v^*\) satisfying
. By Remark 3.5 such elements are \(\xi ^*\), \(\xi ^* + \alpha _i^*\),
and
(\(1 \leqslant i,j \leqslant 3\)).
-
If \(\overline{g}(\xi ^*) = \xi ^*\), then \(g_\alpha \) (respectively \(g_\beta \)) fixes \(\alpha _4\) (respectively \(\beta _4\)) by the description of the permutations above and \(g_\alpha \) (respectively \(g_\beta \)) can be recovered from the action of \(\overline{g}\) on the set
(respectively \(\{\beta _1^*, \beta _2^*, \beta _3^*\}\)).
-
If \(\overline{g}(\xi ^*) = \xi ^* + \alpha _i^*\) (\(1 \leqslant i \leqslant 3\)), then \(g_\alpha \) maps \(\alpha _4\) to \(\alpha _i\) and \(g_\beta \) fixes \(\beta _4\). Then \(g_\alpha \) (respectively \(g_\beta \)) is determined by the action of \(\overline{g}\) on the set
(respectively \(\{\beta _1^*, \beta _2^*, \beta _3^*\}\)).
-
If
(\(1 \leqslant j \leqslant 3\)), then \(g_\beta \) maps \(\beta _4\) to
and \(g_\alpha \) fixes \(\alpha _4\). Then \(g_\alpha \) (respectively \(g_\beta \)) is determined by the action of \(\overline{g}\) on the set
(respectively \(\{\xi ^*+ \beta _1^*, \xi ^*+\beta _2^*, \xi ^*+\beta _3^*, \xi ^*\}\)).
-
If
(\(1 \leqslant i,j \leqslant 3\)), then \(g_\alpha \) maps \(\alpha _4\) to \(\alpha _i\) and \(g_\beta \) maps \(\beta _4\) to
. Then \(g_\alpha \) (respectively \(g_\beta \)) can be recovered by the action of \(\overline{g}\) on the set
(respectively
). \(\square \)
By abuse of notation, we also use
to denote its image in \(O(q_T) \cong O(q_M)\). There exists a natural exact sequence \(1 \rightarrow \widetilde{O}(T) \rightarrow O(T) \xrightarrow {r_T} O(q_T) \rightarrow 1\) which also induces \(1 \rightarrow O^*(T) \rightarrow O_-(T) \rightarrow O(q_T) \rightarrow 1\). We define \(\Gamma \subset O_{-} (T)\subset O(T)\) as the following extension:
By Lemmas 3.16 and 3.17, the group \(\Gamma \) fixes M but may permute the elements \(\alpha _1, \ldots , \alpha _4\) (respectively \(\beta _1, \ldots , \beta _4\)). Note that \(O^*(T)\) is a normal subgroup of \(\Gamma \) and
. Also, \(\Gamma \) and O(T) are commensurable and hence \(\Gamma \) is an arithmetic group. There is a natural action of \(\Gamma \) on
(see the description of
in (10)).
Recall that
is the moduli space of triples \((C, L_1, L_2)\) consisting of a quartic curve C and (labeled) lines \(L_1\), \(L_2\) such that \(C + L_1 + L_2\) has at worst simple singularities.
Proposition 3.18
The period map
that associates to a (generic) triple \((C, L_1, L_2)\) the periods of the K3 surface \(S_{(C,L_1,L_2)}\) defines a birational map
.
Proof
Let U be an open subset of
parameterizing triples \((C, L_1, L_2)\) with C smooth quartic curves and \(L_1,L_2\) two (labeled) lines such that \(C+L_1+L_2\) has simple normal crossings. Set \(\Sigma _4\) to be the permutation group of four elements and note that \(\Sigma _\alpha \cong \Sigma _\beta \cong \Sigma _4\). Let \(\widetilde{U}\) be the
-cover of U that parametrizes quintuples \((C, L_1, L_2, \sigma _1,\sigma _2)\) where
, \(k=1,2\), is a labeling of the intersection points of \(C \cap L_k\). Note that the monodromy group acts as the permutation group \(\Sigma _4\) on the four points of intersection \(C \cap L_k\). By Corollary 3.7, \(\sigma _1\) and \(\sigma _2\) determine an M-polarization \(\jmath \) of the K3 surface \(S_{(C, L_1, L_2)}\). Therefore there is a well-defined map
By the global Torelli theorem and the surjectivity of the period map for K3 surfaces (see also Proposition 3.9), the map
is a birational morphism. The group
acts naturally on both \(\widetilde{U}\) and
as \(\Gamma \) is an extension of
and \(O^*(T)\). Essentially, the actions are induced by the permutation of the labeling of the intersection points \(C \cap L_k\) (\(k=0,1\)). It follows that
is
-equivariant and descends to the birational map
(see also Lemmas 3.16 and 3.17).\(\square \)
M-polarization for non-generic intersections
We will show in this section that the birational map
in Proposition 3.18 extends to a birational morphism
. To do this, we need to extend the construction of M-polarization
to the non-generic triples \((C, L_1, L_2)\) and show that the construction fits in families. The idea is to use the normalized lattice polarization (cf. [17, Definition 4.24]) for degree 5 pairs constructed in [17, Section 4.2.3]. A degree
d
pair (D, L) consists of a degree d plane curve D and a line
(see [17, Definition 2.1]). Given a triple \((C, L_1, L_2)\) of a quartic curve C and two different lines \(L_1\) and \(L_2\), one can construct a degree 5 pair in two ways: \((C+L_2, L_1)\) or \((C+L_1, L_2)\). We follow the notation of the previous subsections, especially Notation 3.3. We will determine the images of \(\gamma , l_1', \alpha _1, \ldots , \alpha _4\) (respectively \(\gamma , l_2', \beta _1, \ldots , \beta _4\)) using the degree 5 pair \((C+L_2, L_1)\) (respectively \((C+L_1, L_2)\)).
Let us briefly review the construction of normalized lattice polarization for degree 5 pairs. See [17, Section 4.2.3] for more details. Let (D, L) be a degree 5 pair such that
has at worst simple singularities. Let \(\overline{S}_{(D,L)}\) be the normal surface obtained as the double cover of
branched along B. Let \(S_{(D,L)}\) be the minimal resolution of \(\overline{S}_{(D,L)}\), called the K3 surface associated to (D, L). The surface \(S_{(D,L)}\) can also be obtained as the canonical resolution of \(\overline{S}_{(D,L)}\), see [4, Section III.7]. Namely, there exists a commutative diagram:
where \(S'\) is obtained by an inductive process. Start with
and \(B_{-1} = B = D+ L\). Simultaneously blow up all the singular points of B. Let
be the resulting surface and set \(B_0\) to be the strict transform of B together with the exceptional divisors of \(\epsilon _0\) reduced mod 2. Repeat the process for \(S_0\) and \(B_0\) until the resulting divisor \(B_N\) is smooth. Let \(S' = S_N\), \(B' = B_N\) and
. Now take the double cover \(\pi ':S_{(D, L)} \rightarrow S'\) branched along the smooth locus \(B'\).
The construction of a normalized lattice polarization for degree 5 pairs is a modification of the process of canonical resolution. We may choose a labeling of the intersection points of D and L, which means a surjective map
satisfying
for every \(p \in D \cap L\). As argued in [17, Proposition 4.25], L is blown up exactly 5 times in the desingularization process described above. The blown-up points can be chosen as the first five steps of the sequence of blow-ups:
, and the labeling determines the order of these first five blow-ups. Let \(\{p_k\}_{k=0}^4\) be the centers of these blow-ups and \(E_k\) be the exceptional divisors. Note that \(p_k \in S_{k-1}\) (the image of \(p_k\) under the contraction to
is a point of intersection \(D \cap L\)) and \(E_k\) is a divisor on \(S_k\) for \(k = 0, \ldots , 4\). We define the following divisors:
for \(0 \leqslant k \leqslant 4\). The divisor \(D_k\) on \(S_{(D,L)}\) is Artin’s fundamental cycle (see for example [4, p. 76]) associated to the simple singularity of the curve \(B_{k-1}\) at the point \(p_k\).
The procedure described above produces five divisors: \(D_0, \ldots , D_4\). One can also consider the strict transform of L in \(S'\) and take its preimage in \(S_{(D,L)}\). This is a smooth rational curve on the K3 surface and we will denote its corresponding class by \(L'\). We summarize the properties of these 6 divisors \(L'\!, D_0, \ldots , D_4\) in the following result. Given families of curves (C, L), we can carry out a simultaneous resolution in families. As a result the construction above fits well in families, see [17, p. 2141].
Lemma 3.19
For a pair (D, L) and the surface \(S_{(D,L)}\) as described above the following statements hold:
-
(a)
the polarization class of \(S_{(D,L)}\) is
, and
-
(b)
their intersections are
,
, \((L'\!, D_k) = 1\) for \(0 \leqslant k,k' \leqslant 4\).
Proof
See the proof of [17, Proposition 4.25].\(\square \)
Let us consider triples \((C, L_1, L_2)\) consisting of a quartic curve C and lines \(L_1\), \(L_2\) such that \(C+L_1+L_2\) has worst simple singularities. Let \(\overline{S}_{(C,L_1,L_2)}\) be the double plane branched along \(C+L_1+L_2\) and \(S_{(C,L_1,L_2)}\) be the K3 surface obtained by taking the minimal resolution of \(\overline{S}_{(C,L_1,L_2)}\). Let
be the natural morphism. To define a lattice embedding
, one needs to specify the images of \(\gamma , l_1', \alpha _1, \ldots , \alpha _4, l_2', \beta _1, \ldots , \beta _4\) so that the intersection form is preserved. There is a compatibility condition induced by \(2l_1' + \alpha _1 + \ldots + \alpha _4 = 2l_2' + \beta _1 + \cdots + \beta _4\). Recall that \(h=\xi + \gamma = 2l_1' + \alpha _1 + \ldots + \alpha _4 +\gamma = 2l_2' + \beta _1 + \cdots + \beta _4 + \gamma \). We also require that \(\jmath (h)\) is the class of the base point free polarization
.
Given a triple \((C, L_1, L_2)\), one has two associated degree 5 pairs:
and
, which induce the same K3 surface \(S_{(D,L)}\), constructed as above. Let us fix two labelings
and
such that
. Every degree 5 pair produces six divisors as described above. For the pair \((C+L_2, L_1)\) (respectively \((C+L_1, L_2)\)), we denote the 6 divisors by \(L_1', R_0, \ldots , R_4\) (respectively \(L_2', T_0, \ldots , T_4\)). Note that
. We define
as follows:
-
\(\jmath (\gamma ) = R_0 = T_0\) (by our choice of the labelings, both \(R_0\) and \(T_0\) are the fundamental cycle associated to the singularity of \(C+L_1+L_2\) at the point \(L_1 \cap L_2\));
-
and
;
-
\(\jmath (\alpha _i) = R_i\) and
for \(1 \leqslant i,j \leqslant 4\).
After the first blow-up \(\epsilon _0\), the strict transforms of the two lines \(L_1\) and \(L_2\) are disjoint and hence, we have
for \(1 \leqslant i,j \leqslant 4\). Using Lemma 3.19, it is straightforward to verify that \(\jmath \) is a well-defined lattice embedding. The embedding \(\jmath \) also satisfies the following geometric properties and fits well in families (cf. [17, Section 4.2.3], especially the last paragraph on p. 2141).
-
\(\jmath (h)\) is the class of the base point free polarization
.
-
and
are the classes of irreducible rational curves.
-
\(\jmath (\gamma ), \jmath (\alpha _1), \ldots , \jmath (\alpha _4)\) (respectively \(\jmath (\gamma ), \jmath (\beta _1), \ldots , \jmath (\beta _4)\)) are classes of effective divisors which are contracted by \(\pi \) to the points of the intersection \(C \cap L_1\) (respectively \(C \cap L_2\)). In particular, \(\jmath (\gamma )\) is contracted to the point \(L_1 \cap L_2\).
To conclude that \(\jmath \) is an M-polarization we also need the following lemma.
Lemma 3.20
The lattice embedding
is primitive.
Proof
This follows from a case by case analysis. Specifically, we check the conditions of Lemma 3.8 as in the proof of Proposition 3.6.\(\square \)
Proposition 3.21
The birational map in Proposition 3.18 extends to a morphism
. Moreover, the map
is injective.
Proof
Given a triple \((C, L_1, L_2)\) consisting of a quartic curve C and lines \(L_1\), \(L_2\) such that \(C + L_1 + L_2\) has at worst simple singularities, we consider the M-polarized K3 surface \((S_{(C, L_1, L_2)}, \jmath )\) where \(S_{(C,L_1,L_2)}\) is the K3 surface obtained by taking the minimal resolution of the double plane branched along \(C + L_1 +L_2\) and \(\jmath \) is the lattice polarization constructed above. By [8], the M-polarized K3 surface \((S_{(C, L_1, L_2)}, \jmath )\) corresponds to a point in
. The polarization \(\jmath \) depends only on \((C, L_1, L_2)\), the ordering of \(C \cap L_1\) and the ordering of \(C \cap L_2\), and it is compatible with the action of
. Consequently, we can associate to every triple \((C, L_1, L_2)\) a point in
. In other words, we have a well-defined morphism
extending the birational map in Proposition 3.18.
Choose a point
(more precisely, \(\omega \) is a \(\Gamma \)-orbit) which corresponds to an M-polarization K3 surface \(S_{(C, L_1, L_2)}\). Lemma 3.16 allows us to extend an element of \(\Gamma \) to an isometry of the K3 lattice \(\Lambda _{K3}\). The global Torelli theorem for K3 surfaces implies that the period \(\omega \) determines the isomorphism class of the K3 surface \(S_{(C + L_1 + L_2)}\). By our construction the classes h, \(l_1'\) and \(l_2'\) are fixed by \(\Gamma \). It follows that the period point \(\omega \) uniquely expresses the K3 surface as a double cover of
and determines two line components of the branched locus. Now we conclude that \(\omega \) determines uniquely the triple \((C, L_1, L_2)\). \(\square \)
Surjectivity of the period map
We will show in this section that the period map
is surjective. Given the general result of surjectivity of period maps for (lattice) polarized K3, one has to establish that any K3 surface carrying an M-polarization is of type \(S_{(C, L_1, L_2)}\).
Proposition 3.22
Let S be a K3 surface such that there exists a primitive embedding
. Then there exists a plane quartic curve C and two different lines
such that \(S \cong S_{(C, L_1, L_2)}\) and \(C+L_1+L_2\) has at worst simple singularities.
Proof
We apply [17, Proposition 4.31] (see also [17, Lemmas 4.27, 4.28, 4.30]). The idea is to consider the primitive sublattices \(M_1\) and \(M_2\) of M generated by \(l_1', \gamma , \alpha _1, \ldots , \alpha _4\) and \(l_2', \gamma , \beta _1, \ldots , \beta _4\) respectively. Both of the sublattices have the following Gram matrix
$$\begin{aligned} \left( {\begin{array}{c@{\quad }c@{\quad }c@{\quad }c@{\quad }c@{\quad }c} -2 &{} 1 &{} 1 &{} 1 &{} 1 &{} 1 \\ 1 &{} -2 &{} 0 &{} 0 &{} 0 &{} 0 \\ 1 &{} 0 &{} -2 &{} 0 &{} 0 &{} 0 \\ 1 &{} 0 &{} 0 &{} -2 &{} 0 &{} 0 \\ 1 &{} 0 &{} 0 &{} 0 &{} -2 &{} 0 \\ 1 &{} 0 &{} 0 &{} 0 &{} 0 &{} -2 \\ \end{array} } \right) _. \end{aligned}$$
Hence they are isomorphic to the lattice considered in [17, Notation 4.11] for degree 5 pairs. In particular, S is both \(M_1\)-polarized and \(M_2\)-polarized. Indeed, recall that
which coincides with Laza’s lattice (for both \(M_1\) and \(M_2\)). Using [17, Proposition 4.31], we find two degree 5 pairs \((D_1, L_1)\) and \((D_2, L_2)\) (where, a priori, \(D_1\) and \(D_2\) may be irreducible) such that \(D_1 + L_1 = D_2 + L_2\) has at worst simple singularities. The two morphisms
associated to each degree 5 pair are both defined by \(\jmath (h)\), and hence they are the same. Because \(L_1\) and \(L_2\) are both contained in the branch locus of the map
, \(D_1=L_2+C\) and \(D_2=L_1+C\), where C is a quartic plane curve such that \(C+L_1+L_2\) has at worst simple singularities. \(\square \)
Theorem 3.23
Consider the triples \((C, L_1, L_2)\) consisting of a quartic curve C and lines \(L_1,L_2\) such that \(C + L_1 + L_2\) has at worst simple singularities. Let \(S_{(C,L_1,L_2)}\) be the K3 surface obtained by taking the minimal resolution of the double plane branched along \(C + L_1 +L_2\). The birational map sending \((C, L_1, L_2)\) to the periods of \(S_{(C,L_1,L_2)}\) in Proposition 3.18 extends to an isomorphism
.
Proof
It suffices to prove that
is surjective. Let
be a period point. By the surjectivity of the period map of lattice-polarized K3 surfaces (see [8, Theorem 3.1]) there exists an M-polarized K3 surface
corresponding to \(\omega \). By Proposition 3.22, the K3 surface S is the double cover of
branched at a plane quartic curve C and two different lines \(L_1,L_2\). Moreover, let \(M_1\) and \(M_2\) be the primitive sublattices of M defined in the proof of Proposition 3.22. After choosing the Kähler cone \(V^+(S)\) and the set of effective \((-2)\) curves \(\Delta ^+(S)\) as in the proof of [17, Theorem 4.1], we may assume that the restrictions \(\jmath |_{M_1}\) and \(\jmath |_{M_2}\) of the polarization \(\jmath \) to the sublattices \(M_1\) and \(M_2\) are both normalized embeddings, as defined in [17, Definition 4.24]. The embeddings \(\jmath |_{M_1}\) and \(\jmath |_{M_2}\) are unique up to permutation of the classes \(\alpha _1,\ldots , \alpha _4\) (\(\beta _1,\ldots , \beta _4\), respectively) thanks to [17, Lemma 4.29]. It follows that the polarization \(\jmath \) is unique up to action of
and coincides with our construction in Sect. 3.4. By Propositions 3.18 and 3.21, the period map
is a bijective birational morphism between normal varieties. As a result,
is an isomorphism, by Zariski’s Main Theorem.\(\square \)
The period map for unlabeled triples
Consider the compact space
and
, consisting on the subset of triples \((C, L, L')\) formed by a quartic curve C and unlabeled lines \(L,L'\) such that the sextic curve \(C + L + L'\) is reduced and has at worst simple singularities, as constructed in Corollary 2.16. In this subsection we define the period map
—for an appropriately chosen arithmetic group \(\Gamma '\)—and show that
is an isomorphism. We use the same approach taken to define
(Propositions 3.18 and 3.21) and to prove Theorem 3.23. The modification one needs to do is to choose a different arithmetic group \(\Gamma '\). We follow the same notation as in the previous subsections, especially regarding the description of the subgroup
in Lemma 3.17. Consider the subgroup
where the factor \(\mathbb {Z}/2\mathbb {Z}\) corresponds to the swap of \(\alpha _i\)’s and \(\beta _i\)’s for \(0 \leqslant i \leqslant 4\) (the induced action on \(A_M\) exchanges \(\alpha _i^*\) with \(\beta _i^*\) for \(1 \leqslant i \leqslant 3\) and fixes \(\gamma ^*\) and \(\xi ^*\)). As in the proof of Lemma 3.17, we can verify that the composition
is injective. Now we define \(\Gamma '\) to be the following extension:
For
(such that \(C+L+L'\) is reduced and has at worst simple singularities) we consider the period of the K3 surface \(S_{(C,L,L')}\) which is the minimal resolution of the double cover of
branched along \(C+L+L'\). Because \(S_{(C,L,L')}\) is polarized by the lattice M, the period corresponds to a point in
. The lattice polarization depends on the labeling of L and \(L'\), the ordering of \(C \cap L\) and the ordering of \(C \cap L'\), and thus is compatible with the action of
. Therefore we have a well-defined period map
(see also Propositions 3.18 and 3.21). Moreover, the same argument in Proposition 3.21 and Theorem 3.23 allows us to prove that the period map
is an isomorphism.
Comparison of the GIT and the Baily–Borel compactifications
Consider the moduli space
of triples \((C, L, L')\) formed by a quartic curve C and unlabeled lines L, \(L'\) such that the sextic curve \(C + L + L'\) has at worst simple singularities. We have constructed a period map
in Sect. 3.6 and have shown that it is an isomorphism. There are two natural ways to compactify
as the GIT quotient
defined in (3) and described in Corollary 2.16, or as the Baily–Borel compactification [3]. We compare these two compactifications by applying some general results of Looijenga [21]. See also [17, Theorem 4.2].
Theorem 3.24
The period map
extends to an isomorphism of projective varieties
where
denotes the Baily–Borel compactification of
.
Proof
We apply a general framework of comparing GIT compactifications to certain compactifications of the period domain developed by Looijenga. Specifically, by [21, Theorem 7.6] an isomorphism
(typically coming from a period map) between a geometric quotient
and a complement of an arithmetic hyperplane arrangement
in a type IV domain \(\Omega \) extends to an isomorphism
between the GIT compactification
and the Looijenga compactification \(\widetilde{\Omega /\Lambda }\) associated to
if their polarizations agree and
. We have
. The hyperplane arrangement is empty and the associated Looijenga compactification is the Baily–Borel compactification
. Moreover, by Corollary 2.16 and Lemma 2.7, we have
and their polarizations agree by restriction of the isomorphic polarizations for the GIT of sextic curves and for the compact moduli of K3 surfaces of degree 2 (see [21, Section 8]). Hence, by [21, Theorem 7.6]
is an isomorphism for polarized varieties. \(\square \)
Question 3.25
Does the period map for labeled triples
(cf. Theorem 3.23) preserve the natural polarizations?
A positive answer to this question would imply that the period map
can be extended to an isomorphism
. We strongly believe that the answer is yes (by pulling back the polarizations for sextic curves and degree 2 K3 surfaces via the double covers
and
).
The Baily–Borel compactification
The locally symmetric space
admits a canonical minimal compactification, the Baily–Borel compactification
(cf. [3]). The boundary components of
are either 0-dimensional (Type III components) or 1-dimensional (Type II components), and they correspond to the primitive rank 1, respectively, rank 2 isotropic sublattices of T up to \(\Gamma '\)-equivalence. Following the approach of [17, 29, 31], we determine the number of the Type III boundary components of
and compute certain invariants for the Type II boundary components. Notice that by Theorem 3.24, the number of these boundary components and some of their invariants (such as the dimension) can be worked out from the boundary components of the GIT quotient
described in Corollary 2.16.
We determine the 0-dimensional components of
using [29, Proposition 4.1.3]. The 0-dimensional boundary components are in one-to-one correspondence with the \(\Gamma '\)-orbits of primitive isotropic rank 1 sublattices of T. By Proposition 3.13 and [26, Theorem 3.6.2] we have
. (In particular, T contains two hyperbolic planes.) Write
(see Sect. 3.6). Note that for \(v \in T\) one can associate a vector
defined by
\(\mathrm{mod}\,T\) (where
is the divisor of v which is a positive integer such that
). If v is a primitive isotropic vector then \(\overline{v}\) is an isotropic element in \(A_T\). By [29, Proposition 4.1.3] the map \(\mathbb {Z}v \mapsto \overline{v}\) induces a bijection between the equivalence classes of primitive isotropic rank 1 sublattices of T and \(\Gamma ^*\)-orbits of isotropic elements of \(A_T\). Because T is the orthogonal complement of M in \(\Lambda _{K3}\), one has
. We have computed the discriminant quadratic form \(q_M\) in Lemma 3.4. In particular, there are 20 isotropic elements in \(A_M \cong A_T\): \(0, \gamma ^*\),
and
(\(1 \leqslant i,j \leqslant 3\)). The action of \(\Gamma ^*\) has been described in the proof of Lemma 3.17 and Sect. 3.6. It is easy to see that
and
(\(1 \leqslant i,j \leqslant 3\)) form one \(\Gamma ^*\)-orbit. As a result, the Baily–Borel compactification
consists of three 0-dimensional boundary components.
Remark 3.26
Similarly, one can show that
has three 0-dimensional boundary components (compare Lemma 2.15).
Remark 3.27
As discussed in [17, Section 4.4.1], one important invariant for the \(O_-(T)\)-equivalence class of isotropic sublattices E of T is the isomorphism classes of
(and we shall use it to label E). Let us compute the isomorphism classes of
(where \(\mathbb {Z}v\) is a primitive isotropic rank 1 sublattice of T). Observe that
. One could compute the Gram matrix of
explicitly. Alternatively, we consider
(cf. [17, Section 4.4.1]) which is an isotropic subgroup of \(A_T \cong (\mathbb {Z}/2\mathbb {Z})^6\) and the discriminant group \(A_{v^{\perp }/\mathbb {Z}v} \cong H_v^{\perp }/H_v\). In our case, \(H_v\) equals either 0 or \(\mathbb {Z}/2\mathbb {Z}\). The lattice
is an even hyperbolic (N.B. the signature is (1, 9)) 2-elementary lattice. By a direct computation we get the following (see also [26, Theorem 3.6.2]).
To determine the 1-dimensional components of
, one needs to compute the equivalence classes of primitive isotropic rank 2 sublattices of T. We use the algorithm for classifying isotropic vectors in hyperbolic lattices due to Vinberg [33]. Specifically, for each of the equivalence classes of primitive isotropic rank 1 sublattices \(\mathbb {Z}v\) of T we apply Vinberg’s algorithm to the hyperbolic lattice
(with respect to the action by the stabilizer \(\Gamma '_v\) of v).
Now we briefly recall Vinberg’s algorithm [33] (see also [31, Section 4.3]). Let N be a hyperbolic lattice of signature (1, n). (In our case we take
.) The algorithm starts by fixing an element \(h \in N\) of positive square. Then one needs to inductively choose roots \(\delta _1, \delta _2, \ldots \) such that the distance function \({(h,\delta )^2}/{|(\delta ,\delta )|}\) is minimized. The algorithm stops with the choice of \(\delta _N\) if every connected parabolic subdiagram (i.e. the extended Dynkin diagram of a root system) of the Dynkin diagram \(\Sigma \) associated to the roots \(\delta _1, \delta _2, \ldots , \delta _N\) is a connected component of some parabolic subdiagram of rank \(n-1\). If the algorithm stops then the W(N)-orbits of the isotropic lines in N correspond to the parabolic subdiagrams of rank \(n-1\) of \(\Sigma \) (N.B. the isomorphism classes of
, where E is an isotropic rank 2 sublattice of T containing v, are determined by the Dynkin diagrams of the parabolic subdiagrams). To determine the equivalence classes of the isotropic vectors by a larger group which contains the Weyl group W(N) as a subgroup of finite index, one should take certain symmetries of \(\Sigma \) into consideration.
In our case, a straightforward application of Vinberg’s algorithm allows us to compute the isomorphism classes of
.
By Theorem 3.24 and Corollary 2.16 we conclude that the Baily–Borel compactification
consists of five 1-dimensional boundary components labeled by
,
,
,
and \(D_8\) respectively.
Remark 3.28
Using the Clemens–Schmid exact sequence and the incidence relation of the GIT boundary components (see also [17, Theorem 4.32]), we match the GIT boundary of
in Corollary 2.16 with the Baily–Borel boundary of
.
GIT boundary
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\(D_8\)
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