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3.3.1 Integral affine structure induced by the model 𝒳 i ​ j ​ k [04PS]

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3.3.1 Integral affine structure induced by the model 𝒳i​j​k\mathscr{X}_{ijk}

By [NXY19] the non-archimedean SYZ fibration ρ𝒳i​j​k:San→Sk⁡(𝒳i​j​k)=Sk⁡(X)≃𝕊2\rho_{\mathscr{X}_{ijk}}:S^{\an}\rightarrow\Sk(\mathscr{X}_{ijk})=\Sk(X)\simeq\mathbb{S}^{2} is an affinoid torus fibration (at least) away from the vertices of the triangulation of Sk⁡(X)\Sk(X) induced by the special fiber of 𝒳i​j​k\mathscr{X}_{ijk}, i.e. away from the vDmv_{D_{m}}’s.
By Theorem B, ρ𝒳i​j​k\rho_{\mathscr{X}_{ijk}} is an affinoid torus fibration over Star⁡(τDh)\Star(\tau_{D_{h}}) for h≠i,j,kh\neq i,j,k, as Dh≃ℙ2D_{h}\simeq\mathbb{P}^{2} and gi​j​kg_{ijk} is an isomorphism on the strict transform of DhD_{h}. Moreover, by Remark 3.1.7 and Eq. 3.3.1 the integral affine structure induced by ρ𝒳i​j​k\rho_{\mathscr{X}_{ijk}} does not extend to vDiv_{D_{i}}, vDjv_{D_{j}} and vDkv_{D_{k}}.

We conclude that the singular points of the affine structure on Sk⁡(X)\Sk(X) induced by ρ𝒳i​j​k\rho_{\mathscr{X}_{ijk}} are precisely vDiv_{D_{i}}, vDjv_{D_{j}} and vDkv_{D_{k}}. Corollary 3.1.6 establishes that the monodromies around these vertices are

Tρ𝒳i​j​k\displaystyle T_{\rho_{\mathscr{X}_{ijk}}} (γi)=(218−8−3)\displaystyle(\gamma_{i})=\left(\begin{matrix}21&8\\ -8&-3\end{matrix}\right)
in the basis (vDj,vDk) and origin vDi,\displaystyle\text{in the basis $(v_{D_{j}},v_{D_{k}})$ and origin $v_{D_{i}}$},
Tρ𝒳i​j​k\displaystyle T_{\rho_{\mathscr{X}_{ijk}}} (γj)=(−15−441)\displaystyle(\gamma_{j})=\left(\begin{matrix}-15&-4\\ 4&1\end{matrix}\right)
in the basis (vDk,vDh) and origin vDj,\displaystyle\text{in the basis $(v_{D_{k}},v_{D_{h}})$ and origin $v_{D_{j}}$},
Tρ𝒳i​j​k\displaystyle T_{\rho_{\mathscr{X}_{ijk}}} (γk)=(1041)\displaystyle(\gamma_{k})=\left(\begin{matrix}1&0\\ 4&1\end{matrix}\right)
in the basis (vDh,vDi) and origin vDk.\displaystyle\text{in the basis $(v_{D_{h}},v_{D_{i}})$ and origin $v_{D_{k}}$}.
v2=vjv_{2}=v_{j}vh=v4v_{h}=v_{4}v3=vkv_{3}=v_{k}v1=viv_{1}=v_{i}γj\gamma_{j}γk\gamma_{k}γi\gamma_{i}

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