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2 Toric structure along toric strata [04NC]

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2 Toric structure along toric strata

In this section we prove Theorem B. We recall the statement and fix the notation.

Theorem B.

Let X/KX/K be a smooth projective variety of dimension nn, and 𝒳/R\mathscr{X}/R be a dlt model of XX with reduced special fiber 𝒳k=∑αDα\mathscr{X}_{k}=\sum_{\alpha}D_{\alpha}, such that every DαD_{\alpha} is a Cartier divisor.
Let Z=D0∩D1∩…∩Dn−rZ=D_{0}\cap D_{1}\cap\ldots\cap D_{n-r} be an rr-dimensional stratum of 𝒳k\mathscr{X}_{k}, such that:

  • •

    Z̊⊂Z\mathring{Z}\subset Z is a torus embedding, where Z̊=Z∖∪α≠0,1,…,n−rDα\mathring{Z}=Z\setminus\cup_{\alpha\neq 0,1,\ldots,n-r}D_{\alpha};

  • •

    the conormal bundle νZ/𝒳∗\nu_{Z/\mathscr{X}}^{*} is a nef vector bundle on ZZ;

  • •

    for each α∉{0,…,n−r}\alpha\notin\{0,...,n-r\}, the intersection Dα∩ZD_{\alpha}\cap Z is either empty or connected.

Then the formal completion 𝒳/Z^\widehat{\mathscr{X}_{/Z}} is isomorphic to the formal completion of the normal bundle 𝒩=νZ/𝒳\mathcal{N}=\nu_{Z/\mathscr{X}} along the zero section. In particular, 𝒳\mathscr{X} is toric along ZZ (in the sense of Definition 1.2.6).

Note that the assumptions in Theorem B imply that ZZ is the smooth complete intersection of the irreducible components DjD_{j} of 𝒳k\mathscr{X}_{k} containing ZZ, and thus has simple normal crossing boundary, see Remark 2.1.1. Since ZZ is a complete intersection, the conormal bundle νZ/𝒳∗\nu^{*}_{Z/\mathscr{X}} is the direct sum of the line bundles 𝒪Z​(−Dj)\mathcal{O}_{Z}(-D_{j}). Hence, the nefness assumption simply means that the DjD_{j}’s containing ZZ are anti-nef divisors on ZZ.

As an immediate consequence of the theorem, we prove that

Corollary C.

The retraction ρ𝒳:Xan→Sk⁡(𝒳)\rho_{\mathscr{X}}:X^{\an}\rightarrow\Sk(\mathscr{X}) is an nn-dimensional affinoid torus fibration over Star⁡(τZ)\Star(\tau_{Z}). In particular, the integral affine structure induced by ρ𝒳\rho_{\mathscr{X}} on the complement of the faces of Sk⁡(𝒳)\Sk(\mathscr{X}) of codimension ⩾2\geqslant 2 extends to Star⁡(τZ)\Star(\tau_{Z}) with no singularities.

Proof.

Although this follows from Theorem B by [NXY19, Theorem 6.1] (end of the proof) and by [NXY19, §3.4], we sketch the proof for reader’s convenience.
As mentioned in Section 1.5, the retraction ρ𝒳\rho_{\mathscr{X}} over Star⁡(τZ)\Star(\tau_{Z}) only depends on 𝒳/Z^\widehat{\mathscr{X}_{/Z}}, so that by Theorem B we may assume that 𝒳\mathscr{X} is a toric RR-scheme. The equality ρ𝒳=val\rho_{\mathscr{X}}=\val now holds over Star⁡(τZ)\Star(\tau_{Z}) by Proposition 1.5.2, so that it follows from Definition 1.6.1 that ρ𝒳\rho_{\mathscr{X}} is an affinoid fibration over Star⁡(τZ)\Star(\tau_{Z}). ∎

2.1 Notation and strategy

We set J={0,1,…,n−r}J=\{0,1,\ldots,n-r\} such that Z=∩j∈JDjZ=\cap_{j\in J}D_{j}. Since for every irreducible component DD of 𝒳k\mathscr{X}_{k}, the intersection D∩ZD\cap Z is connected by assumption, this allows us to denote by DlD_{l} with l∈Ll\in L the components of 𝒳k\mathscr{X}_{k} intersecting ZZ transversally along Zl≔Z∩DlZ_{l}\coloneqq Z\cap D_{l}, so that the toric boundary of ZZ is given by ΔZ=∑l∈LZl\Delta_{Z}=\sum_{l\in L}Z_{l}.

Remark 2.1.1.

The dlt assumption on 𝒳\mathscr{X} and the toricness of ZZ ensure that ZZ is smooth, and that (Z,ΔZ)(Z,\Delta_{Z}) is an snc pair. Indeed, the singular locus of ZZ is a union of torus invariant subvarieties (see [CLS11, Proposition 11.1.2]), hence the generic point of a component of the singular locus is the generic point of a stratum of ΔZ\Delta_{Z}. However, (Z,ΔZ)(Z,\Delta_{Z}) is a dlt pair, thus snc at the generic point of each stratum of ΔZ\Delta_{Z}.

Remark 2.1.2.

The smoothness of ZZ and the assumption that the components of 𝒳k\mathscr{X}_{k} are Cartier divisors imply that 𝒳\mathscr{X} is regular at any point of ZZ. Indeed, for any point p∈Zp\in Z and j∈Jj\in J, let zj∈𝒪𝒳,pz_{j}\in\mathcal{O}_{\mathscr{X},p} be a local equation of DjD_{j} at pp. As 𝒪Z,p≃𝒪𝒳,p/(z0,…,zn−r)\mathcal{O}_{Z,p}\simeq\mathcal{O}_{\mathscr{X},p}/(z_{0},\ldots,z_{n-r}) is a regular local ring of dimension rr, (z0,…,zn−r)(z_{0},\ldots,z_{n-r}) can be extended to form a regular system of parameters for 𝒪𝒳,p\mathcal{O}_{\mathscr{X},p}.

We denote by Σ⊂Nℝ\Sigma\subset N_{\mathbb{R}} the fan of ZZ. Its rays are given by ℝ⩾0​ul\mathbb{R}_{\geqslant 0}u_{l} for l∈Ll\in L, with primitive generators ulu_{l}; the maximal cones of Σ\Sigma are in bijection with the set of unordered rr-tuples {i1,…,ir}∈Lr\{i_{1},\ldots,i_{r}\}\in L^{r} such that ∩β=1rDiβ∩Z≠∅\cap_{\beta=1}^{r}D_{i_{\beta}}\cap Z\neq\varnothing. For a maximal cone σ\sigma of Σ\Sigma, we write Lσ≔{l∈L|ul∈σ}L_{\sigma}\coloneqq\{l\in L\,|\,u_{l}\in\sigma\}.

Lemma 2.1.3.

For any maximal cone σ\sigma of Σ\Sigma, we have det((ul)l∈Lσ)=±1.\det((u_{l})_{l\in L_{\sigma}})=\pm 1.

Proof.

The smoothness of ZZ (see Remark 2.1.1) implies that the primitive generators of σ\sigma form a ℤ\mathbb{Z}-basis of NN, which is equivalent to the condition det((ul)l∈Lσ)=±1.\det((u_{l})_{l\in L_{\sigma}})=\pm 1. ∎

Let 𝒩≔νZ/𝒳→𝑝Z\mathcal{N}\coloneqq\nu_{Z/\mathscr{X}}\xrightarrow{p}Z be the normal bundle of ZZ in 𝒳\mathscr{X}, and denote by Z⊂𝒩Z\subset\mathcal{N} the zero section. We write 𝒪𝒳(Dj)|Z=𝒪Z(Fj)\mathcal{O}_{\mathscr{X}}(D_{j})_{|Z}=\mathcal{O}_{Z}(F_{j}) so that 𝒩=⊕j∈J𝒪Z(Fj)\mathcal{N}=\oplus_{j\in J}\mathcal{O}_{Z}(F_{j}). Since any Cartier divisor on ZZ is linearly equivalent to a toric one, for any j=1,…,n−rj=1,\ldots,n-r, there exist integers λj,l\lambda_{j,l} such that

(2.1.4) 𝒪Z(Fj)=𝒪Z(−∑l∈Lλj,lZl).\mathcal{O}_{Z}(F_{j})=\mathcal{O}_{Z}\big(-\sum_{l\in L}\lambda_{j,l}Z_{l}\big).

For j=0j=0 we set λ0,l≔1−∑j∈J∖{0}λj,l\lambda_{0,l}\coloneqq 1-\sum_{j\in J\setminus\{0\}}\lambda_{j,l} and verify that

𝒪Z(F0)=𝒪𝒳(D0−𝒳k)|Z=𝒪Z(−∑j∈J∖{0}Fj−∑l∈LZl)=𝒪Z(−∑l∈Lλ0,lZl).\displaystyle\mathcal{O}_{Z}(F_{0})=\mathcal{O}_{\mathscr{X}}(D_{0}-\mathscr{X}_{k})_{|Z}=\mathcal{O}_{Z}\Big(-\sum_{j\in J\setminus\{0\}}F_{j}-\sum_{l\in L}Z_{l}\Big)=\mathcal{O}_{Z}(-\sum_{l\in L}\lambda_{0,l}Z_{l}).

We obtain that 𝒩=⊕j∈J𝒪Z(−∑l∈Lλj,lZl)\mathcal{N}=\oplus_{j\in J}\mathcal{O}_{Z}\big(-\sum_{l\in L}\lambda_{j,l}Z_{l}\big) and for all ll in LL

(2.1.5) ∑j∈Jλj,l=1.\sum_{j\in J}\lambda_{j,l}=1.

The normal bundle 𝒩\mathcal{N} is a toric variety of dimension n+1n+1. The corresponding fan Σ^\hat{\Sigma} lies in Nℝ×ℝJN_{\mathbb{R}}\times\mathbb{R}^{J} and consists of the following cones and their faces (see [CLS11, §7.3] for a reference). Let e0,…,en−re_{0},\ldots,e_{n-r} be the standard basis of ℝJ\mathbb{R}^{J}; given a cone σ∈Σ\sigma\in\Sigma, we have

σ^=Cone​((0,e0),…,(0,en−r),(ul,(λj,l))|ul∈σ)∈Σ^.\hat{\sigma}=\textrm{Cone}((0,e_{0}),\ldots,(0,e_{n-r}),(u_{l},(\lambda_{j,l}))\,|\,u_{l}\in\sigma)\in\hat{\Sigma}.

In particular, we denote the rays of Σ^\hat{\Sigma} by

vj=(0,ej)​ for ​j∈J,vl=(ul,(λj,l))​ for ​l∈L.v_{j}=(0,e_{j})\textrm{ for }j\in J,\quad v_{l}=(u_{l},(\lambda_{j,l}))\textrm{ for }l\in L.
Proposition 2.1.6.

For any 1-dimensional toric stratum C⊆ZC\subseteq Z

(2.1.7) ∑j∈J(C⋅Dj)​vj+∑l∈L(C⋅Dl)​vl=0​in​Nℝ×ℝJ.\sum_{j\in J}(C\cdot D_{j})v_{j}+\sum_{l\in L}(C\cdot D_{l})v_{l}=0\;\text{in}\;N_{\mathbb{R}}\times\mathbb{R}^{J}.
Proof.

The relation in Eq. 2.1.7 boils down to the two following:

{∑l∈L(C⋅Dl)​ul=0(C⋅Dj)+∑l∈Lλj,l​(C⋅Dl)=0.\begin{cases}\sum_{l\in L}(C\cdot D_{l})u_{l}=0\\ (C\cdot D_{j})+\sum_{l\in L}\lambda_{j,l}(C\cdot D_{l})=0.\\ \end{cases}

The first one follows directly from Eq. 1.2.4 in the fan Σ\Sigma of ZZ; the second comes from the construction of λl\lambda_{l}, and in particular from C⋅Dj=C⋅Fj=−C⋅∑l∈Lλj,lZlC\cdot D_{j}=C\cdot F_{j}=-C\cdot\sum_{l\in L}\lambda_{j,l}Z_{l}. ∎

The map

ord⁡(t):Nℝ×ℝJ→ℝ⩾0(u,w)↦∑j=0n−rwj\ord(t):N_{\mathbb{R}}\times\mathbb{R}^{J}\rightarrow\mathbb{R}_{\geqslant 0}\quad(u,w)\mapsto\sum_{j=0}^{n-r}w_{j}

is ℤ\mathbb{Z}-linear, sends all the primitive generators of the rays of Σ^\hat{\Sigma} to 11 by Eq. 2.1.5, and is compatible with Σ^\hat{\Sigma} and the fan of 𝔸k1\mathbb{A}^{1}_{k}. Thus, it induces a toric morphism t:𝒩→𝔸k1t:\mathcal{N}\rightarrow\mathbb{A}^{1}_{k} whose fiber over 00 is the toric boundary of 𝒩\mathcal{N}. The base change 𝒩≔𝒩×𝔸1R\mathscr{N}\coloneqq\mathcal{N}\times_{\mathbb{A}^{1}}R to RR is a toric RR-scheme, whose generic fiber is isomorphic to 𝔾m,Kn\mathbb{G}_{m,K}^{n}. The special fiber 𝒩k\mathscr{N}_{k} can be written as 𝒩k=∑i∈J∪LEi\mathscr{N}_{k}=\sum_{i\in J\cup L}E_{i}, where the combinatoric of intersections between components is exactly the same as in 𝒳k\mathscr{X}_{k}.

We prove Theorem B by constructing a formal isomorphism

f:𝒳/Z^→≃𝒩/Z^.f:\widehat{\mathscr{X}_{/Z}}\xrightarrow{\simeq}\widehat{\mathscr{N}_{/Z}}.

More specifically, we proceed as follows. We set the notations 𝔛=𝒳/Z^\mathfrak{X}=\widehat{\mathscr{X}_{/Z}} and 𝔑=𝒩/Z^\mathfrak{N}=\widehat{\mathscr{N}_{/Z}}.

  • •

    (Sections 2.2 and 2.3) Let σ∈Σ\sigma\in\Sigma be a maximal cone. Denote by ZσZ_{\sigma} and 𝒩σ≔𝒩Zσ/𝒳\mathcal{N}_{\sigma}\coloneqq\mathcal{N}_{Z_{\sigma}/\mathscr{X}} the corresponding toric affine charts in ZZ and 𝒩\mathcal{N} respectively. This induces an open formal subscheme of 𝔑\mathfrak{N}, which we denote by 𝔑σ\mathfrak{N}_{\sigma}. We construct a morphism

    fσ:𝔛∖(∪l∈L∖LσDl)≕𝔛σ→𝔑σ,f_{\sigma}:\mathfrak{X}\setminus\big(\cup_{l\in L\setminus L_{\sigma}}D_{l}\big)\eqqcolon\mathfrak{X}_{\sigma}\,\rightarrow\mathfrak{N}_{\sigma},

    in a similar manner to [NXY19]: we construct n+1n+1 divisors WjσW^{\sigma}_{j} and WiσW^{\sigma}_{i} on 𝒳\mathscr{X}, whose defining equations on the chart 𝔛σ\mathfrak{X}_{\sigma} yields the morphism fσf_{\sigma}. The equations are induced by sections of 𝒪Z​(Wjσ)\mathcal{O}_{Z}(W^{\sigma}_{j}) and 𝒪Z​(Wiσ)\mathcal{O}_{Z}(W^{\sigma}_{i}): these are first constructed on ZZ, then extended to 𝔛\mathfrak{X} by the nef condition on the conormal bundle νZ/𝒳∗\nu_{Z/\mathscr{X}}^{*} assumed in Theorem B, which ensures the vanishing of higher cohomology groups for the tensor powers of νZ/𝒳∗\nu_{Z/\mathscr{X}}^{*}.

  • •

    (Sections 2.4 and 2.5) Let σ\sigma and σ′\sigma^{\prime} be two maximal cones of Σ\Sigma intersecting along a face of codimension one. We establish relations among the respective divisors and construct sections on 𝔛σ′\mathfrak{X}_{\sigma^{\prime}} from those on 𝔛σ\mathfrak{X}_{\sigma}. This allows us to prove that the morphisms fσf_{\sigma} on the charts 𝔛σ\mathfrak{X}_{\sigma}’s can be chosen so that they are compatible on the overlaps 𝔛σ∩𝔛σ′\mathfrak{X}_{\sigma}\cap\mathfrak{X}_{\sigma^{\prime}}. This yields a well defined morphism ff which extends the identity on ZZ and preserves the ideal ℐZ\mathscr{I}_{Z}, so that it turns out to be an isomorphism.

2.2 Construction of the divisors

We set

Δ:=∑l∈Lul⊗Dl∈N⊗Div0⁡(𝒳)≃(Div0⁡(𝒳))r;\Delta:=\sum_{l\in L}u_{l}\otimes D_{l}\,\in\,N\otimes\Div_{0}(\mathscr{X})\simeq(\Div_{0}(\mathscr{X}))^{r};

this is an rr-tuple of divisors on 𝒳\mathscr{X}. Moreover, the restriction of any of these to ZZ is a principal divisor by Corollary 1.2.2. Given a maximal cone σ\sigma of Σ\Sigma, for any i∈Lσi\in L_{\sigma}, we define

Wiσ≔−det(Δ,(ul)l∈Lσ∖{i})det(ui,(ul)l∈Lσ∖{i})∈Div0⁡(𝒳)W^{\sigma}_{i}\coloneqq-\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma}\setminus\{i\}})}{\det(u_{i},(u_{l})_{l\in L_{\sigma}\setminus\{i\}})}\in\Div_{0}(\mathscr{X})

where the column vectors ulu_{l} are in the same order in the numerator and in the denominator, and the denominator has value ±1\pm 1 by Lemma 2.1.3.

Lemma 2.2.1.

The divisor WiσW^{\sigma}_{i} has multiplicity −1-1 along DiD_{i}, multiplicity 00 along DlD_{l} for l∈Lσ∖{i}l\in L_{\sigma}\setminus\{i\}, and along DjD_{j} for j∈Jj\in J. In other words, we may write:

Wiσ=−Di+∑l∈L∖Lσci,l​DlW^{\sigma}_{i}=-D_{i}+\sum_{l\in L\setminus L_{\sigma}}c_{i,l}D_{l}

for some coefficients ci,l∈ℤc_{i,l}\in\mathbb{Z}. Moreover, the restriction of WiσW^{\sigma}_{i} to ZZ is principal.

Proof.

The statement on the multiplicities follows from the definition of WiσW^{\sigma}_{i}, as

Wσi=−∑l∈Ldet(ul,(ul′)l′∈Lσ∖{i})det(ui,(ul′)l′∈Lσ∖{i})Dl.W^{\sigma}_{i}=-\sum_{l\in L}\frac{\det(u_{l},(u_{l^{\prime}})_{l^{\prime}\in L_{\sigma}\setminus\{i\}})}{\det(u_{i},(u_{l^{\prime}})_{l^{\prime}\in L_{\sigma}\setminus\{i\}})}D_{l}.

Moreover, WiσW^{\sigma}_{i} is a linear combination of the divisors of the rr-tuple Δ\Delta, hence its restriction to ZZ is principal by Corollary 1.2.2. ∎

For j∈Jj\in J, we define the divisor on 𝒳\mathscr{X}

(2.2.2) Wjσ≔−Dj−∑l∈Lλj,l​Dl−∑i∈Lσλj,i​Wiσ=−Dj−∑l∈L∖Lσλj,l​Dl−∑l∈Lσλj,l​Dl−∑i∈Lσλj,i​(−Di+∑l∈L∖Lσci,l​Dl)=−Dj+∑l∈L∖Lσdj,lDl with dj,l=−λj,l−∑i∈Lσλj,ici,l.\displaystyle\begin{split}W^{\sigma}_{j}&\coloneqq-D_{j}-\sum_{l\in L}\lambda_{j,l}D_{l}-\sum_{i\in L_{\sigma}}\lambda_{j,i}W^{\sigma}_{i}\\ &=-D_{j}-\sum_{l\in L\setminus L_{\sigma}}\lambda_{j,l}D_{l}-\cancel{\sum_{l\in L_{\sigma}}\lambda_{j,l}D_{l}}-\sum_{i\in L_{\sigma}}\lambda_{j,i}\big(\cancel{-D_{i}}+\sum_{l\in L\setminus L_{\sigma}}c_{i,l}D_{l}\big)\\ &=-D_{j}+\sum_{l\in L\setminus L_{\sigma}}d_{j,l}D_{l}\quad\textrm{ with }\quad d_{j,l}=-\lambda_{j,l}-\sum_{i\in L_{\sigma}}\lambda_{j,i}c_{i,l}.\end{split}

The restriction of WjσW^{\sigma}_{j} to ZZ is a principal divisor, as the Wσi|Z{W^{\sigma}_{i}}_{|Z} are principal and −Dj|Z{-D_{j}}_{|Z} is linearly equivalent to ∑l∈Lλj,l​Zl\sum_{l\in L}\lambda_{j,l}Z_{l} by Eq. 2.1.4.

Lemma 2.2.3.

The relation ∑j∈JWσj+∑i∈LσWσi=−∑j∈JDj−∑l∈LDl\sum_{j\in J}W^{\sigma}_{j}+\sum_{i\in L_{\sigma}}W^{\sigma}_{i}=-\sum_{j\in J}D_{j}-\sum_{l\in L}D_{l} holds.

Proof.

Write W≔∑j∈JWjσ+∑i∈LσWiσ∈Div0⁡(𝒳).W\coloneqq\sum_{j\in J}W^{\sigma}_{j}+\sum_{i\in L_{\sigma}}W^{\sigma}_{i}\in\Div_{0}(\mathscr{X}). We have

for ​j∈JordDj⁡(W)\displaystyle\textrm{for }j\in J\quad\ord_{D_{j}}(W) =ordDj⁡(Wjσ)=−1\displaystyle=\ord_{D_{j}}(W^{\sigma}_{j})=-1
for ​i∈LσordDi⁡(W)\displaystyle\textrm{for }i\in L_{\sigma}\quad\ord_{D_{i}}(W) =ordDi⁡(Wiσ)=−1\displaystyle=\ord_{D_{i}}(W^{\sigma}_{i})=-1
for ​l∈L∖LσordDl⁡(W)\displaystyle\textrm{for }l\in L\setminus L_{\sigma}\quad\ord_{D_{l}}(W) =∑j∈Jdj,l+∑i∈Lσci,l=−∑j∈Jλj,l+∑i∈Lσci,l(1−∑j∈Jλj,i)=−1\displaystyle=\sum_{j\in J}d_{j,l}+\sum_{i\in L_{\sigma}}c_{i,l}=-\sum_{j\in J}\lambda_{j,l}+\sum_{i\in L_{\sigma}}c_{i,l}(1-\sum_{j\in J}\lambda_{j,i})=-1

by Lemma 2.2.1, Eq. 2.2.2 and Eq. 2.1.5. ∎

2.3 Construction of the sections for a maximal cone

Let σ\sigma be a maximal cone of Σ\Sigma. We denote by ℒjσ\mathscr{L}^{\sigma}_{j} and ℒiσ\mathscr{L}^{\sigma}_{i} the line bundles on 𝔛\mathfrak{X} induced respectively by 𝒪𝒳​(Wjσ)\mathcal{O}_{\mathscr{X}}(W^{\sigma}_{j}) for j∈Jj\in J, and by 𝒪𝒳​(Wiσ)\mathcal{O}_{\mathscr{X}}(W^{\sigma}_{i}) for i∈Lσi\in L_{\sigma}. Since WjσW^{\sigma}_{j} and WiσW^{\sigma}_{i} are principal on ZZ, the restrictions ℒσj|Z{\mathscr{L}^{\sigma}_{j}}_{|Z} and ℒσi|Z{\mathscr{L}^{\sigma}_{i}}_{|Z} are trivial line bundles on ZZ, thus we may choose non-zero global sections sjσs^{\sigma}_{j} and siσs^{\sigma}_{i} on ZZ.

We now lift the sections sjσs^{\sigma}_{j} and siσs^{\sigma}_{i} to global sections of ℒjσ\mathscr{L}^{\sigma}_{j} and ℒiσ\mathscr{L}^{\sigma}_{i}, which we still denote by sjσs^{\sigma}_{j} and siσs^{\sigma}_{i}. Indeed, for any n⩾1n\geqslant 1, write (𝒳/Z)n(\mathscr{X}/Z)_{n} for the (non-reduced) subscheme of 𝒳\mathscr{X} defined by the ideal ℐZn\mathscr{I}^{n}_{Z}. In the exact sequence

H0​((𝒳/Z)n,ℒjσ)⟶H0​((𝒳/Z)n−1,ℒjσ)⟶H1​(Z,(νZ/𝒳∗)⊗n),H^{0}((\mathscr{X}/Z)_{n},\mathscr{L}^{\sigma}_{j})\longrightarrow H^{0}((\mathscr{X}/Z)_{n-1},\mathscr{L}^{\sigma}_{j})\longrightarrow H^{1}(Z,(\nu^{*}_{Z/\mathscr{X}})^{\otimes n}),

and in the analogous one for ℒiσ\mathscr{L}^{\sigma}_{i}, the right-hand vanishes: the conormal bundle is a direct sum of line bundles on ZZ which are nef by the hypothesis in Theorem B and so are its positive tensor powers, thus their first cohomology group vanishes by Proposition 1.2.5. We thus extend the sections constructed above to all of the (𝒳/Z)n(\mathscr{X}/Z)_{n} by induction, which yields an extension to 𝔛=lim←n⁡(𝒳/Z)n\mathfrak{X}=\varprojlim_{n}(\mathscr{X}/Z)_{n}.

Lemma 2.3.1.

The restrictions of sjσs^{\sigma}_{j} and siσs^{\sigma}_{i} to 𝔛σ\mathfrak{X}_{\sigma} are equations for DjD_{j} and DiD_{i}, and thus

wσ≔t⋅∏j∈J(sjσ)−1⋅∏i∈Lσ(siσ)−1w_{\sigma}\coloneqq t\cdot\prod_{j\in J}(s_{j}^{\sigma})^{-1}\cdot\prod_{i\in L_{\sigma}}(s_{i}^{\sigma})^{-1}

is an invertible function on 𝔛σ\mathfrak{X}_{\sigma}.

Proof.

We show that siσs^{\sigma}_{i} is an equation for DiD_{i} on 𝔛σ\mathfrak{X}_{\sigma}; the proof is analogous for sjσs^{\sigma}_{j}.

On ZZ, Wiσ|Z=div(h){W_{i}^{\sigma}}_{|Z}=\textrm{div}(h) and siσs^{\sigma}_{i} is a non-zero global section, which means that

ℒiσ|Z(Z)=𝒪Z(Wiσ)(Z)={f∈𝒦(Z)|div(f)+div(h)⩾0}\displaystyle{\mathscr{L}^{\sigma}_{i}}_{|Z}(Z)=\mathcal{O}_{Z}({W^{\sigma}_{i}})(Z)=\{f\in\mathcal{K}(Z)\,|\,\textrm{div}(f)+\textrm{div}(h)\geqslant 0\} →≃𝒪Z​(Z)=k\displaystyle\xrightarrow{\simeq}\mathcal{O}_{Z}(Z)=k
f\displaystyle f ↦f​h\displaystyle\mapsto fh
siσ\displaystyle s^{\sigma}_{i} ↦siσ​h=λ∈k×.\displaystyle\mapsto s^{\sigma}_{i}h=\lambda\in k^{\times}.

Let 𝒰\mathcal{U} be an open cover of 𝒳∖(∪i′∉J∪LσDi′)\mathscr{X}\setminus\big(\cup_{i^{\prime}\notin J\cup L_{\sigma}}D_{i^{\prime}}\big) such that Di|U=div(gU){D_{i}}_{|U}=\textrm{div}(g_{U}) for any U∈𝒰U\in\mathcal{U}; this is possible as DiD_{i} is a Cartier divisor. On UU, Wiσ|U=−Di|U=div(gU−1){W^{\sigma}_{i}}_{|U}=-{D_{i}}_{|U}=\textrm{div}(g_{U}^{-1}) and

ℒiσ​(𝔛σ∩U)\displaystyle\mathscr{L}^{\sigma}_{i}(\mathfrak{X}_{\sigma}\cap U) →≃𝒪𝔛σ​(𝔛σ∩U)\displaystyle\xrightarrow{\simeq}\mathcal{O}_{\mathfrak{X}_{\sigma}}(\mathfrak{X}_{\sigma}\cap U)
f\displaystyle f ↦f​gU−1\displaystyle\mapsto fg_{U}^{-1}
siσ\displaystyle s^{\sigma}_{i} ↦siσ​gU−1∈𝒪𝔛σ×​(𝔛σ∩U),\displaystyle\mapsto s^{\sigma}_{i}g_{U}^{-1}\in\mathcal{O}_{\mathfrak{X}_{\sigma}}^{\times}(\mathfrak{X}_{\sigma}\cap U),

where siσ​gU−1s^{\sigma}_{i}g_{U}^{-1} is a regular invertible function on 𝔛σ∩U\mathfrak{X}_{\sigma}\cap U, as its reduction to ZZ is invertible. Finally, the section siσs^{\sigma}_{i} is defined globally on 𝒳/Z^\widehat{\mathscr{X}_{/Z}} and on each open 𝔛σ∩U\mathfrak{X}_{\sigma}\cap U gives a local equation of the divisor DiD_{i}, hence it is a equation for DiD_{i} on 𝔛σ\mathfrak{X}_{\sigma}. ∎

2.4 Construction for two adjacent maximal cones

Let σ\sigma and σ′\sigma^{\prime} be two maximal cones of Σ\Sigma intersecting along a face of codimension one. Setting Lσ​σ′=Lσ∩Lσ′L_{\sigma\sigma^{\prime}}=L_{\sigma}\cap L_{\sigma^{\prime}}, we may write Lσ=Lσ​σ′∪{i0}L_{\sigma}=L_{\sigma\sigma^{\prime}}\cup\{i_{0}\} and Lσ′=Lσ​σ′∪{i∞}L_{\sigma^{\prime}}=L_{\sigma\sigma^{\prime}}\cup\{i_{\infty}\}. The sets ℬ=((vi)i∈Lσ​σ′,vi0,(vj)j∈J)\mathcal{B}=((v_{i})_{i\in L_{\sigma\sigma^{\prime}}},v_{i_{0}},(v_{j})_{j\in J}) and ℬ′=((vi)i∈Lσ​σ′,vi∞,(vj)j∈J)\mathcal{B}^{\prime}=((v_{i})_{i\in L_{\sigma\sigma^{\prime}}},v_{i_{\infty}},(v_{j})_{j\in J}) are bases of N^=N⊕ℤJ\hat{N}=N\oplus\mathbb{Z}^{J}. They induce isomorphisms β,β′:ℤr⊕ℤJ→N^\beta,\beta^{\prime}:\mathbb{Z}^{r}\oplus\mathbb{Z}^{J}\rightarrow\hat{N} such that the change of basis from ℬ\mathcal{B} to ℬ′\mathcal{B}^{\prime} is

Mℬ′​ℬ=β′∘β−1=Lσ​σ′i0JId(−C⋅Di)i∈Lσ​σ′0Lσ​σ′0−10i∞0(−C⋅Dj)j∈JIdJ and ​(vivi∞vj)=Mℬ′​ℬT​(vivi0vj).M_{\mathcal{B}^{\prime}\mathcal{B}}=\beta^{\prime}\circ\beta^{-1}=\begin{array}[]{cccc}L_{\sigma\sigma^{\prime}}&i_{0}&J\\ \Id&(-C\cdot D_{i})_{i\in L_{\sigma\sigma^{\prime}}}&0&L_{\sigma\sigma^{\prime}}\\ 0&-1&0&i_{\infty}\\ 0&(-C\cdot D_{j})_{j\in J}&\Id&J\\ \end{array}\quad\textrm{ and }\left(\begin{matrix}v_{i}\\ v_{i_{\infty}}\\ v_{j}\end{matrix}\right)=M_{\mathcal{B}^{\prime}\mathcal{B}}^{T}\left(\begin{matrix}v_{i}\\ v_{i_{0}}\\ v_{j}\end{matrix}\right).

Denote by ((εi)i∈Lσ​σ′,εi0,(εj)j∈J)((\varepsilon_{i})_{i\in L_{\sigma\sigma^{\prime}}},\varepsilon_{i_{0}},(\varepsilon_{j})_{j\in J}) the basis of M^≔Hom⁡(N^,ℤ)\hat{M}\coloneqq\Hom(\hat{N},\mathbb{Z}) dual to ℬ\mathcal{B}, and ((εi′)i∈Lσ​σ′,εi∞′,(εj′)j∈J)((\varepsilon^{\prime}_{i})_{i\in L_{\sigma\sigma^{\prime}}},\varepsilon^{\prime}_{i_{\infty}},(\varepsilon^{\prime}_{j})_{j\in J}) the basis dual to ℬ′\mathcal{B}^{\prime}. It follows that

(2.4.1) (εi′εi∞′εj′)=Mℬ′​ℬ​(εiεi0εj).\left(\begin{matrix}\varepsilon^{\prime}_{i}\\ \varepsilon^{\prime}_{i_{\infty}}\\ \varepsilon^{\prime}_{j}\end{matrix}\right)=M_{\mathcal{B}^{\prime}\mathcal{B}}\left(\begin{matrix}\varepsilon_{i}\\ \varepsilon_{i_{0}}\\ \varepsilon_{j}\end{matrix}\right).

The isomorphisms β\beta and β′\beta^{\prime} allow us to view

Wσ≔((Wiσ)i∈Lσ​σ′,Wi0σ,(Wjσ)j∈J)∈(ℤr⊕ℤJ)⊗Div0⁡(𝒳)≃(Div0⁡(𝒳))n+1W^{\sigma}\coloneqq((W^{\sigma}_{i})_{i\in L_{\sigma\sigma^{\prime}}},W^{\sigma}_{i_{0}},(W^{\sigma}_{j})_{j\in J})\,\in\,(\mathbb{Z}^{r}\oplus\mathbb{Z}^{J})\otimes\Div_{0}(\mathscr{X})\simeq(\Div_{0}(\mathscr{X}))^{n+1}

and Wσ′W^{\sigma^{\prime}} as elements of N^⊗Div0⁡(𝒳)\widehat{N}\otimes\Div_{0}(\mathscr{X}), that we will still denote by WσW^{\sigma} and Wσ′W^{\sigma^{\prime}} .

Lemma 2.4.2.

Let C⊆ZC\subseteq Z be the curve associated with the cone σ∩σ′\sigma\cap\sigma^{\prime}. We have

{Wiσ′=Wiσ−(C⋅Di)​Wi0σ for ​i∈Lσ​σ′Wi∞σ′=−Wi0σWjσ′=Wjσ−(C⋅Dj)​Wi0σ for ​j∈J\begin{cases}W^{\sigma^{\prime}}_{i}=W^{\sigma}_{i}-(C\cdot D_{i})W^{\sigma}_{i_{0}}&\textrm{ \hskip 10.22217ptfor }i\in L_{\sigma\sigma^{\prime}}\\ W^{\sigma^{\prime}}_{i_{\infty}}=-W^{\sigma}_{i_{0}}&\\ W^{\sigma^{\prime}}_{j}=W^{\sigma}_{j}-(C\cdot D_{j})W^{\sigma}_{i_{0}}&\textrm{ \hskip 10.22217ptfor }j\in J\end{cases}

In other words, the relation Wσ′=(Mℬ′​ℬ⊗Id)WσW^{\sigma^{\prime}}=(M_{\mathcal{B}^{\prime}\mathcal{B}}\otimes\Id)W^{\sigma} holds.

Proof.

By Eq. 1.2.4 we have ui∞=−ui0−∑m∈Lσ​σ′(C⋅Dm)​umu_{i_{\infty}}=-u_{i_{0}}-\sum_{m\in L_{\sigma\sigma^{\prime}}}(C\cdot D_{m})u_{m}, so

for i∈Lσ​σ′, Wiσ′\displaystyle\textrm{for $i\in L_{\sigma\sigma^{\prime}}$, }\quad W^{\sigma^{\prime}}_{i} =−det(Δ,(ul)l∈Lσ​σ′∖{i},ui∞)det(ui,(ul)l∈Lσ​σ′∖{i},ui∞)\displaystyle=-\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{\infty}})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{\infty}})}
=−det(Δ,(ul)l∈Lσ​σ′∖{i},ui0)det(ui,(ul)l∈Lσ​σ′∖{i},ui0)−∑m∈Lσ​σ′(C⋅Dm)​det(Δ,(ul)l∈Lσ​σ′∖{i},um)det(ui,(ul)l∈Lσ​σ′∖{i},ui0)\displaystyle=-\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}-\sum_{m\in L_{\sigma\sigma^{\prime}}}(C\cdot D_{m})\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{m})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}
=Wiσ−(C⋅Di)​det(Δ,(ul)l∈Lσ​σ′∖{i},ui)det(ui,(ul)l∈Lσ​σ′∖{i},ui0)=Wiσ−(C⋅Di)​Wi0σ;\displaystyle=W^{\sigma}_{i}-(C\cdot D_{i})\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i})}{\det(u_{i},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}\setminus\{i\}},u_{i_{0}})}=W^{\sigma}_{i}-(C\cdot D_{i})W^{\sigma}_{i_{0}};
for i=i∞, Wi∞σ′\displaystyle\textrm{for $i=i_{\infty}$, }\quad W^{\sigma^{\prime}}_{i_{\infty}} =det(Δ,(ul)l∈Lσ​σ′)det(ui∞,(ul)l∈Lσ​σ′)=−det(Δ,(ul)l∈Lσ​σ′)det(ui0,(ul)l∈Lσ​σ′)=−Wi0σ.\displaystyle=\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}{\det(u_{i_{\infty}},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}=-\frac{\det(\Delta,(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}{\det(u_{i_{0}},(u_{l})_{l\in L_{\sigma\sigma^{\prime}}})}=-W^{\sigma}_{i_{0}}.

For j∈Jj\in J

∑i∈Lσ′λj,i​Wiσ′\displaystyle\sum_{i\in L_{\sigma^{\prime}}}\lambda_{j,i}W^{\sigma^{\prime}}_{i} =−λj,i∞​Wi0σ+∑i∈Lσ​σ′λj,i​(Wiσ−(C⋅Di)​Wi0σ)\displaystyle=-\lambda_{j,i_{\infty}}W^{\sigma}_{i_{0}}+\sum_{i\in L_{\sigma\sigma^{\prime}}}\lambda_{j,i}\left(W^{\sigma}_{i}-(C\cdot D_{i})W^{\sigma}_{i_{0}}\right)
=(−λj,i∞−∑i∈Lσ​σ′λj,i​(C⋅Di)−λj,i0)​Wi0σ+∑i∈Lσλj,i​Wiσ\displaystyle=\Big(-\lambda_{j,i_{\infty}}-\sum_{i\in L_{\sigma\sigma^{\prime}}}\lambda_{j,i}(C\cdot D_{i})-\lambda_{j,i_{0}}\Big)W^{\sigma}_{i_{0}}+\sum_{i\in L_{\sigma}}\lambda_{j,i}W^{\sigma}_{i}
=(C⋅Dj)Wi0σ+∑i∈Lσλi,jWiσby Eq. 2.1.7\displaystyle=(C\cdot D_{j})W^{\sigma}_{i_{0}}+\sum_{i\in L_{\sigma}}\lambda_{i,j}W^{\sigma}_{i}\hskip 30.0pt\textrm{by \lx@cref{creftype~refnum}{equ fan}}
Wjσ′\displaystyle W^{\sigma^{\prime}}_{j} =−Dj−∑l∈Lλj,l​Dl−∑i∈Lσ′λj,i​Wiσ′\displaystyle=-D_{j}-\sum_{l\in L}\lambda_{j,l}D_{l}-\sum_{i\in L_{\sigma^{\prime}}}\lambda_{j,i}W^{\sigma^{\prime}}_{i}
=−Dj−∑l∈Lλj,l​Dl−∑i∈Lσλj,i​Wiσ−(C⋅Dj)​Wi0σ=Wjσ−(C⋅Dj)​Wi0σ.\displaystyle=-D_{j}-\sum_{l\in L}\lambda_{j,l}D_{l}-\sum_{i\in L_{\sigma}}\lambda_{j,i}W^{\sigma}_{i}-(C\cdot D_{j})W^{\sigma}_{i_{0}}=W^{\sigma}_{j}-(C\cdot D_{j})W^{\sigma}_{i_{0}}.

These relations can be summed up as (Wiσ′Wi∞σ′Wjσ′)=Mℬ′​ℬ​(WiσWi0σWjσ)\left(\begin{matrix}W^{\sigma^{\prime}}_{i}\\ W^{\sigma^{\prime}}_{i_{\infty}}\\ W^{\sigma^{\prime}}_{j}\end{matrix}\right)=M_{\mathcal{B}^{\prime}\mathcal{B}}\left(\begin{matrix}W^{\sigma}_{i}\\ W^{\sigma}_{i_{0}}\\ W^{\sigma}_{j}\end{matrix}\right), i.e. Wσ′=(Mℬ′​ℬ⊗Id)WσW^{\sigma^{\prime}}=(M_{\mathcal{B}^{\prime}\mathcal{B}}\otimes\Id)W^{\sigma}. ∎

The inverse (si0σ)−1(s^{\sigma}_{i_{0}})^{-1} is a section on 𝔛\mathfrak{X} of ℒi∞σ′\mathscr{L}^{\sigma^{\prime}}_{i_{\infty}}, so by Lemma 2.4.2 the sections

{siσ′≔siσ⋅(si0σ)−(C⋅Di) for ​i∈Lσ​σ′si∞σ′≔(si0σ)−1sjσ′≔sjσ⋅(si0σ)−(C⋅Dj) for ​j∈J\begin{cases}s^{\sigma^{\prime}}_{i}\coloneqq s^{\sigma}_{i}\cdot(s^{\sigma}_{i_{0}})^{-(C\cdot D_{i})}&\textrm{ \quad for }i\in L_{\sigma\sigma^{\prime}}\\ s^{\sigma^{\prime}}_{i_{\infty}}\coloneqq(s^{\sigma}_{i_{0}})^{-1}&\\ s^{\sigma^{\prime}}_{j}\coloneqq s^{\sigma}_{j}\cdot(s^{\sigma}_{i_{0}})^{-(C\cdot D_{j})}&\textrm{ \quad for }j\in J\end{cases}

are sections on 𝔛\mathfrak{X} of the line bundles ℒiσ′\mathscr{L}^{\sigma^{\prime}}_{i} and ℒjσ′\mathscr{L}^{\sigma^{\prime}}_{j}. By Lemma 2.3.1 these give equations for DiD_{i} and DjD_{j} on the open subscheme 𝔛σ′,\mathfrak{X}_{\sigma^{\prime}}, and on 𝔛σ∩𝔛σ′\mathfrak{X}_{\sigma}\cap\mathfrak{X}_{\sigma^{\prime}} we have

(2.4.3) (siσ′si∞σ′sjσ′)=Mℬ′​ℬ​(siσsi0σ′sjσ)\left(\begin{matrix}s^{\sigma^{\prime}}_{i}\\ s^{\sigma^{\prime}}_{i_{\infty}}\\ s^{\sigma^{\prime}}_{j}\end{matrix}\right)=M_{\mathcal{B}^{\prime}\mathcal{B}}\left(\begin{matrix}s^{\sigma}_{i}\\ s^{\sigma^{\prime}}_{i_{0}}\\ s^{\sigma}_{j}\end{matrix}\right)

where the additive notation on the matrix corresponds to the multiplicative notation on the sections. Moreover, on 𝔛σ∩𝔛σ′\mathfrak{X}_{\sigma}\cap\mathfrak{X}_{\sigma^{\prime}} we have

(2.4.4) wσ′≔t⋅∏j∈J(sjσ′)−1⋅∏i∈Lσ′(siσ′)−1=t⋅∏j∈J(sjσ)−1​(si0σ)C⋅Dj⋅∏i∈Lσ​σ′(siσ)−1​(si0σ)C⋅Di⋅(si0σ)=t⋅∏j∈J(sjσ)−1⋅∏i∈Lσ​σ′(siσ)−1⋅(si0σ)∑j∈JC⋅Dj+∑i∈Lσ​σ′C⋅Di+1=wσ,\displaystyle\begin{split}w_{\sigma^{\prime}}&\coloneqq t\cdot\prod_{j\in J}(s_{j}^{\sigma^{\prime}})^{-1}\cdot\prod_{i\in L_{\sigma^{\prime}}}(s_{i}^{\sigma^{\prime}})^{-1}=t\cdot\prod_{j\in J}(s^{\sigma}_{j})^{-1}(s^{\sigma}_{i_{0}})^{C\cdot D_{j}}\cdot\prod_{i\in L_{\sigma\sigma^{\prime}}}(s^{\sigma}_{i})^{-1}(s^{\sigma}_{i_{0}})^{C\cdot D_{i}}\cdot(s^{\sigma}_{i_{0}})\\ &=t\cdot\prod_{j\in J}(s^{\sigma}_{j})^{-1}\cdot\prod_{i\in L_{\sigma\sigma^{\prime}}}(s^{\sigma}_{i})^{-1}\cdot(s^{\sigma}_{i_{0}})^{\sum_{j\in J}C\cdot D_{j}+\sum_{i\in L_{\sigma\sigma^{\prime}}}C\cdot D_{i}+1}=w_{\sigma},\end{split}

hence the invertible function wσw_{\sigma} on 𝔛σ\mathfrak{X}_{\sigma} extends to 𝔛σ∪𝔛σ′\mathfrak{X}_{\sigma}\cup\mathfrak{X}_{\sigma^{\prime}} by wσ′w_{\sigma^{\prime}}.

2.5 Construction of the morphism

Let Γ\Gamma be the graph with vertices the maximal cones of Σ\Sigma (hence the maximal cones of Σ^\widehat{\Sigma}) and with an edge between σ\sigma and σ′\sigma^{\prime} if and only if σ∩σ′\sigma\cap\sigma^{\prime} is a common face of codimension one. Note that since ZZ is proper, if 𝕊⊂Nℝ\mathbb{S}\subset N_{\mathbb{R}} is a sphere with center the origin, then Σ∩𝕊\Sigma\cap\mathbb{S} is a triangulation of 𝕊\mathbb{S}. In particular, Γ\Gamma is the 1-skeleton of the dual complex of a triangulation of the sphere, and is thus connected.

Let σ0∈Σ\sigma_{0}\in\Sigma be a maximal cone, and p0∈Γp_{0}\in\Gamma the corresponding vertex, that we will use as a reference point. We fix a tuple of sections sσ0s^{\sigma_{0}} of Wσ0W^{\sigma_{0}} as in Section 2.3.
Let σ∈Σ\sigma\in\Sigma be a maximal cone, and p∈Γp\in\Gamma the corresponding vertex. By connectedness of Γ\Gamma, there exists a path γ\gamma from p0p_{0} to pp, hence a sequence of maximal cones σ0,…,σq=σ\sigma_{0},\ldots,\sigma_{q}=\sigma such that σh∩σh+1\sigma_{h}\cap\sigma_{h+1} is a codimension one face of both σh\sigma_{h} and σh+1\sigma_{h+1}, for h=0,…,q−1h=0,\ldots,q-1. The construction of Section 2.4 allows us to construct inductively along γ\gamma a tuple of sections sσhs^{\sigma_{h}} of WσhW^{\sigma_{h}}.

Lemma 2.5.1.

The tuple of sections sσs^{\sigma} is independent on the choice of path.

Proof.

By Eq. 2.4.3, for any h=0,…,q−1h=0,\ldots,q-1, the sections sσh+1s^{\sigma_{h+1}} are constructed from sσhs^{\sigma_{h}} by multiplication by the matrix for the change of basis from ((vi)i∈Lσh,(vj)j∈J)((v_{i})_{i\in L_{\sigma_{h}}},(v_{j})_{j\in J}) to ((vi)i∈Lσh+1,(vj)j∈J)((v_{i})_{i\in L_{\sigma_{h+1}}},(v_{j})_{j\in J}). Thus, by composition, the sections sσs^{\sigma} only depends on sσ0s^{\sigma_{0}} and the change of basis from ((vi)i∈Lσ0,(vj)j∈J)((v_{i})_{i\in L_{\sigma_{0}}},(v_{j})_{j\in J}) to ((vi)i∈Lσ,(vj)j∈J)((v_{i})_{i\in L_{\sigma}},(v_{j})_{j\in J}). ∎

This provides us with a tuple of sections sσs^{\sigma} of WσW^{\sigma} for each maximal cone σ∈Σ\sigma\in\Sigma, and the function

wσ=t⋅∏j∈J(sjσ)−1⋅∏i∈Lσ(siσ)−1∈𝒪​(𝔛σ)×.w_{\sigma}=t\cdot\prod_{j\in J}(s_{j}^{\sigma})^{-1}\cdot\prod_{i\in L_{\sigma}}(s_{i}^{\sigma})^{-1}\,\in\mathcal{O}(\mathfrak{X}_{\sigma})^{\times}.

By Eq. 2.4.4 the wσw_{\sigma} glue to an invertible function ww on 𝔛\mathfrak{X}; ww admits a (n+1)(n+1)-th root on ZZ, since it is constant, and by Hensel’s lemma we obtain an invertible function w′w^{\prime} on 𝔛\mathfrak{X} such that (w′)n+1=w(w^{\prime})^{n+1}=w. We use the sections sσs^{\sigma} and the function w′w^{\prime} to define a morphism

fσ:𝔛σ⟶𝔑σf_{\sigma}:\mathfrak{X}_{\sigma}\longrightarrow\mathfrak{N}_{\sigma}

as follows. Denoting by ((εi)i∈Lσ,(εj)j∈J)((\varepsilon_{i})_{i\in L_{\sigma}},(\varepsilon_{j})_{j\in J}) the dual basis to ((vi)i∈Lσ,(vj)j∈J)((v_{i})_{i\in L_{\sigma}},(v_{j})_{j\in J}), the toric chart 𝔑σ\mathfrak{N}_{\sigma} has the following explicit description:

𝔑σ=Spf⁡R⁡[χεi,i∈Lσ]​[[χεj,j∈J]]/{t−χ∑i∈Lσεi+∑j∈Jεj}.\mathfrak{N}_{\sigma}=\Spf R[\chi^{\varepsilon_{i}},i\in L_{\sigma}][[\chi^{\varepsilon_{j}},j\in J]]/\{t-\chi^{\sum_{i\in L_{\sigma}}\varepsilon_{i}+\sum_{j\in J}\varepsilon_{j}}\}.

Indeed, 𝔑σ\mathfrak{N}_{\sigma} is the formal completion along ZZ of 𝒩σ^×𝔸1R\mathcal{N}_{\hat{\sigma}}\times_{\mathbb{A}^{1}}R, where 𝒩σ^=Spec⁡k⁡[(σ^)∨∩N^]\mathcal{N}_{\hat{\sigma}}=\Spec k[(\hat{\sigma})^{\vee}\cap\hat{N}]; since ord⁡(t)=∑i∈Lσεi+∑j∈Jεj\ord(t)=\sum_{i\in L_{\sigma}}\varepsilon_{i}+\sum_{j\in J}\varepsilon_{j} on σ^\widehat{\sigma}, the relation t=χ∑i∈Lσεi+∑j∈Jεjt=\chi^{\sum_{i\in L_{\sigma}}\varepsilon_{i}+\sum_{j\in J}\varepsilon_{j}} holds.
The map fσf_{\sigma} is now defined at the level of function rings by

fσ#:𝒪⁡(𝔑σ)\displaystyle f^{\#}_{\sigma}:\mathcal{O}(\mathfrak{N}_{\sigma}) ⟶𝒪⁡(𝔛σ)\displaystyle\longrightarrow\mathcal{O}(\mathfrak{X}_{\sigma})
χεi\displaystyle\chi^{\varepsilon_{i}} ↦w′​siσ​ for ​i∈Lσ\displaystyle\mapsto w^{\prime}s^{\sigma}_{i}\;\textrm{ \quad for }i\in L_{\sigma}
χεj\displaystyle\chi^{\varepsilon_{j}} ↦w′​sjσ​ for ​j∈J\displaystyle\mapsto w^{\prime}s_{j}^{\sigma}\;\textrm{ \quad for }j\in J

where the sections sσs^{\sigma} are viewed as functions on 𝔛σ\mathfrak{X}_{\sigma} thanks to the proof of Lemma 2.3.1.

Lemma 2.5.2.

For any pair of maximal cones σ,σ′\sigma,\sigma^{\prime} intersecting along a codimension one face, the morphisms fσf_{\sigma} and fσ′f_{\sigma^{\prime}} coincide on the overlap 𝔛σ∩𝔛σ′\mathfrak{X}_{\sigma}\cap\mathfrak{X}_{\sigma^{\prime}}.

Proof.

The cones σ\sigma and σ′\sigma^{\prime} correspond to adjacent vertices in Γ\Gamma. Thus, by Lemma 2.5.1 we construct sσs^{\sigma} from any path joining σ0\sigma_{0} to σ\sigma, and sσ′s^{\sigma^{\prime}} from sσs^{\sigma} by the relation sσ′=Mℬ′​ℬ​sσs^{\sigma^{\prime}}=M_{\mathcal{B^{\prime}}\mathcal{B}}\,s^{\sigma} in Eq. 2.4.3.

The functions χε\chi^{\varepsilon} transform into χε′\chi^{\varepsilon^{\prime}} via the change of dual bases, which is given by ε′=Mℬ′​ℬ​ε\varepsilon^{\prime}=M_{\mathcal{B^{\prime}}\mathcal{B}}\,\varepsilon in Eq. 2.4.1. Comparing the two formulas, it follows that fσ=fσ′f_{\sigma}=f_{\sigma^{\prime}} on 𝔛σ∩𝔛σ′\mathfrak{X}_{\sigma}\cap\mathfrak{X}_{\sigma^{\prime}}. ∎

Proposition 2.5.3.

The morphism of formal RR-schemes f:𝒳/Z^⟶𝒩/Z^f:\widehat{\mathscr{X}_{/Z}}\longrightarrow\widehat{\mathscr{N}_{/Z}} obtained by gluing the morphisms fσf_{\sigma} is an isomorphism.

Proof.

We follow the argument in [NXY19, Proposition 5.4].
Since the source and the target have same dimension and are integral, it is enough to check that ff is a closed immersion.
If 𝒥\mathscr{J} is the largest ideal of definition of 𝒩/Z^\widehat{\mathscr{N}_{/Z}}, i.e. the defining ideal of Z⊂𝒩Z\subset\mathscr{N}, then f∗​𝒥=ℐZf^{*}\mathscr{J}=\mathscr{I}_{Z} is the largest ideal of definition of 𝒳/Z^\widehat{\mathscr{X}_{/Z}}. Indeed, since ZZ is cut out inside 𝒳\mathscr{X} by the DjD_{j} for j∈Jj\in J, the ideal ℐZ\mathscr{I}_{Z} is locally generated by the sjs_{j} for j∈Jj\in J; the same reasoning shows that 𝒥\mathscr{J} is locally generated by the χεj\chi^{\varepsilon_{j}}. The equality f∗​𝒥=ℐZf^{*}\mathscr{J}=\mathscr{I}_{Z} now follows directly from the local definition of ff.
We use [Gro61, 4.8.10] and the fact that ff induces an isomorphism on the reductions to infer that ff is a closed immersion, and thus an isomorphism by equality of dimensions. ∎

This concludes the proof of Theorem B: 𝒳\mathscr{X} is toric along ZZ.

2.6 Integral affine structure and toric irreducible components

The case where ZZ is an irreducible component DD of 𝒳k\mathscr{X}_{k} is particularly relevant for proving Theorem A. Under the assumptions of Theorem B, we proved that 𝒳\mathscr{X} is toric along DD, and ρ𝒳\rho_{\mathscr{X}} is an affinoid torus fibration over Star⁡(vD)\Star(v_{D}) by Corollary C. Moreover, we have the following explicit description of the ℤ\mathbb{Z}-affine structure on Star⁡(vD)\Star(v_{D}) induced by ρ𝒳\rho_{\mathscr{X}} - note that it only depends on DD and not on how DD sits inside 𝒳\mathscr{X}.

Corollary 2.6.1.

In the setting of Theorem B, let Z=DZ=D be an irreducible component of 𝒳k\mathscr{X}_{k}. Then there is a natural ℤ\mathbb{Z}-linear embedding of Star⁡(vD)\Star(v_{D}) inside the fan ΣD\Sigma_{D} of DD which sends the polyhedral decomposition of Star⁡(vD)\Star(v_{D}) to the cone decomposition of ΣD\Sigma_{D}.

Proof.

By the proof of Theorem B and Proposition 1.5.2 we have the following diagram:

𝔛D{\lx@inpgf@ignorespaces\mathfrak{X}_{D}}𝔑D{\lx@inpgf@ignorespaces\mathfrak{N}_{D}}Star⁡(vD){\lx@inpgf@ignorespaces\Star(v_{D})}Int⁡(Σ1){\lx@inpgf@ignorespaces\mathrm{Int}(\Sigma_{1})}≃\simeqρ𝒳{\rho_{\mathscr{X}}}val\val≃\simeqφ\varphi

where the upper arrow is an isomorphism of analytic spaces, and the lower one a homeomorphism. Here 𝔛D\mathfrak{X}_{D} and 𝔑D\mathfrak{N}_{D} are the generic fibers (in the sense of Berkovich) of the formal completions 𝒳/D^\widehat{\mathscr{X}_{/D}} and 𝒩/D^\widehat{\mathscr{N}_{/D}} respectively, and Int⁡(Σ1)\mathrm{Int}(\Sigma_{1}) denotes the interior of the polyhedral complex Σ1\Sigma_{1} obtained by intersecting the fan Σ^⊂Nℝ×ℝ\hat{\Sigma}\subset N_{\mathbb{R}}\times\mathbb{R} of the normal bundle of DD in 𝒳\mathscr{X} with Nℝ×{1}N_{\mathbb{R}}\times\{1\}. In particular, Int⁡(Σ1)\mathrm{Int}(\Sigma_{1}) is embedded in ΣD≃Nℝ≃ℝn\Sigma_{D}\simeq N_{\mathbb{R}}\simeq\mathbb{R}^{n}, the polyhedral decomposition of Star⁡(vD)\Star(v_{D}) is the same of ΣD\Sigma_{D}, and the vertex vDv_{D} corresponds to the origin. By Section 1.6, the integral affine structure on Star⁡(vD)\Star(v_{D}) is the pullback via φ\varphi of the integral affine structure on ΣD\Sigma_{D}, and this concludes the proof. ∎

Original mathematics by the credited authors. Source-backed reader collection; mathematical self-containment is not assessed.