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4.2. Tropical K3 surfaces [04YL]

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4.2. Tropical K3 surfaces

In our paper, what we mean by tropical polarized K3 surface is a topological space BB homeomorphic to the sphere S2S^{2}, with an affine structure away from certain finite points Sing⁡(B){\rm Sing}(B), with a metric which is Mongé-Ampere metric gg with respect to the affine structure on B∖Sing⁡(B)B\setminus{\rm Sing}(B). Studies of such object as tropical version of K3 surfaces are pioneered in well-known papers of Gross-Wilson [GW00] and Kontsevich-Soibelman [KS04].

Here we assign such tropical K3 surface to each point in the boundary component ℱ2​d​(l)\mathcal{F}_{2d}(l) as follows. Let ll be an oriented one-dimensional isotropic subspace of Λ2​d⊗ℚ\Lambda_{2d}\otimes\mathbb{Q}. Write ee for the primitive element of ll such that ℝ>0​e\mathbb{R}_{>0}e agrees with the orientation of ll. Take a vector v∈(l⟂/l)⊗ℝv\in(l^{\perp}/l)\otimes\mathbb{R} such that (v,v)>0(v,v)>0. Write [e,v][e,v] for the corresponding point in ℱ2​d​(l)\mathcal{F}_{2d}(l). Then there exists a (not necessarily projective) K3 surface XX and a marking αX:H2​(X,ℤ)→Λ\alpha_{X}\colon H^{2}(X,\mathbb{Z})\to\Lambda with

  • •

    αX​(H2,0)⊂ℝ​λ+−1​ℝ​v\alpha_{X}(H^{2,0})\subset\mathbb{R}\lambda+\sqrt{-1}\mathbb{R}v,

  • •

    αX−1​(e)\alpha_{X}^{-1}(e) is in the closure of Kähler cone.

The pair (X,αX)(X,\alpha_{X}) is unique up to isomorphisms.

Let LL be a line bundle on XX such that αX​([L])=e\alpha_{X}([L])=e. Then we get an elliptic fibration f:X→B(≃ℙ1)f:X\to B(\simeq\mathbb{P}^{1}). Take a holomorphic volume form Ω\Omega on XX such that αX​([ReΩ])=λ\alpha_{X}([\mathop{\mathrm{Re}}\nolimits\Omega])=\lambda. The map ff is a Lagrangian fibration with respect to the symplectic form ReΩ\mathop{\mathrm{Re}}\nolimits\Omega. Hence it gives an affine manifold structure on B∖ΔB\setminus\Delta, where Δ\Delta denotes the finite set of singular points. Similarly, the imaginary part ImΩ\mathop{\mathrm{Im}}\nolimits\Omega gives another affine manifold structure on B∖ΔB\setminus\Delta.

We endow the base space BB with the McLean metric on the base BB ([ML98]), where we regard ff as special Lagrangian fibration after hyperKähler rotation. A straightforward calculation shows that this coincides with the “special Kähler metric” g𝑠𝑝g_{\it sp} introduced and studied in [DW96, Hit96, Freed99] and appears as the metric on ℙ1\mathbb{P}^{1} in [GTZ16]. We rescale the metric to make its diameter 11 and denote this obtained tropical K3 surface by Φalg​([e,v])\Phi_{\rm alg}([e,v]).

Remark 4.1.

Recall the concepts of the class of metric (metric class) and the radiance obstruction of Mongé-Ampére manifolds BB with singularities. They are introduced in [KS04] and discussed in [GS06] in more details. We denote them by k⁡(B)∈H1​(B,i∗​Λ~∨⊗ℝ)k(B)\in H^{1}(B,i_{*}\tilde{\Lambda}^{\vee}\otimes\mathbb{R}) and c⁡(B)∈H1​(B,i∗​Λ)c(B)\in H^{1}(B,i_{*}\Lambda), respectively. Here, Λ\Lambda is the affine structure as a ℤ𝑑𝑖𝑚⁡(B)\mathbb{Z}^{\it dim(B)}-local system in tangent bundle T⁡(B∖Δ)T(B\setminus\Delta), −∨-^{\vee} denotes −-’s dual local system, Λ~∨\tilde{\Lambda}^{\vee} is local system of affine functions. In particular, we naturally have a morphism of local systems f:Λ~∨→Λ∨f\colon\tilde{\Lambda}^{\vee}\to\Lambda^{\vee} which induces f∗:H1​(B,i∗​Λ~∨)→H1​(B,i∗​Λ∨)f_{*}\colon H^{1}(B,i_{*}\tilde{\Lambda}^{\vee})\to H^{1}(B,i_{*}\Lambda^{\vee}). It is also easy to see that, if we slightly change the definition of the metric class, to extract its “linear” part as f∗​k​(B)f_{*}k(B). Then, it naturally recovers the data v¯∈(e⟂⊗ℝ/ℝ​e)\overline{v}\in(e^{\perp}\otimes\mathbb{R}/\mathbb{R}e) i.e., we have f∗​k​(Φalg​([e,v]))=[v],f_{*}k(\Phi_{\rm alg}([e,v]))=[v], under the natural identification H1​(Φalg​([e,v]),i∗​Λ∨⊗ℝ)↪(e⟂⊗ℝ/ℝ​e)H^{1}(\Phi_{\rm alg}([e,v]),i_{*}\Lambda^{\vee}\otimes\mathbb{R})\hookrightarrow(e^{\perp}\otimes\mathbb{R}/\mathbb{R}e) which comes from the Leray spectral sequence applied to the elliptic fibration X↠Φalg​([e,v])X\twoheadrightarrow\Phi_{\rm alg}([e,v]) in §4.2. Our results in [Od16] and Theorem 3.1 for AgA_{g} can be re-interpretted similarly (but with weight 11).

Remark 4.2.

Yuto Yamamoto [Yam] has some ongoing interesting work which seems to be related to our works, where he constructs a sphere with an integral affine structure from the tropicalization of an anticanonical hypersurface in a toric Fano 3-fold, and computes its radiance obstruction.

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