ScalingStacks

Proof. [01F0]

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Proof.

Step 1. Given a finite set LL and a field ΞΊ\kappa, we rely on basic toric geometry (cf.Β [KKMS, Ful93, Oda88]) to show that Z:=𝐀κL=Spec⁑κ⁑[ti,i∈L]Z:=\mathbf{A}^{L}_{\kappa}=\Spec\kappa[t_{i},\,i\in L] and its coordinate hyperplanes (Hi)i∈L(H_{i})_{i\in L} satisfy an analogue of (i)-(iv). Set T:=(𝐆m,ΞΊ)LT:=(\mathbf{G}_{m,\kappa})^{L} to be the multiplicative split torus of dimension LL over ΞΊ\kappa. The fan Ξ£\Sigma of the toric ΞΊ\kappa-variety ZZ consists of the cones Οƒ^J=βˆ‘j∈J𝐑+​ej\hat{\sigma}_{J}=\sum_{j\in J}\mathbf{R}_{+}e_{j}, JβŠ‚LJ\subset L. For each sβˆˆπ‘+Ls\in\mathbf{R}_{+}^{L} let

valZ,s:κ⁑[[ti,i∈L]]→𝐑+\val_{Z,s}:\kappa[[t_{i},\,i\in L]]\to\mathbf{R}_{+}

be the monomial valuation with valZ,s⁑(ti)=si\val_{Z,s}(t_{i})=s_{i} for i∈Li\in L, so that the center of valZ,s\val_{Z,s} on ZZ is the generic point of HJ:=β‹‚j∈JHjH_{J}:=\bigcap_{j\in J}H_{j} for all ss in the relative interior of Οƒ^J\hat{\sigma}_{J}.

Let Ξ£β€²\Sigma^{\prime} be a simplicial fan decomposition of Ξ£\Sigma. The toric ΞΊ\kappa-variety Zβ€²Z^{\prime} attached to Ξ£β€²\Sigma^{\prime} comes with a TT-equivariant proper birational morphism ρ:Zβ€²β†’Z\rho:Z^{\prime}\to Z satisfying the following properties:

  • (a)

    Zβ€²Z^{\prime} is normal (because it is toric), and all toric Weil divisors of Zβ€²Z^{\prime} are 𝐐\mathbf{Q}-Cartier (since Ξ£β€²\Sigma^{\prime} is simplicial).

  • (b)

    There is a bijection between the set of rays (Ri)i∈Lβ€²(R_{i})_{i\in L^{\prime}} of Ξ£β€²\Sigma^{\prime} and the toric prime divisors (Hiβ€²)i∈Lβ€²(H^{\prime}_{i})_{i\in L^{\prime}} of Zβ€²Z^{\prime}, in such a way that for each s∈Riβˆ–{0}s\in R_{i}\setminus\{0\} the center of valZ,s\val_{Z,s} on Zβ€²Z^{\prime} is the generic point of Hiβ€²H^{\prime}_{i}.

  • (c)

    For each Jβ€²βŠ‚Lβ€²J^{\prime}\subset L^{\prime} the intersection HJβ€²β€²:=β‹‚j∈Jβ€²Hjβ€²H^{\prime}_{J^{\prime}}:=\bigcap_{j\in J^{\prime}}H^{\prime}_{j} is normal, irreducible, and non-empty iff Οƒ^Jβ€²β€²=βˆ‘j∈Jβ€²Rj\hat{\sigma}^{\prime}_{J^{\prime}}=\sum_{j\in J^{\prime}}R_{j} is a cone of Ξ£β€²\Sigma^{\prime}. In this case HJβ€²β€²H^{\prime}_{J^{\prime}} has codimension |Jβ€²||J^{\prime}|, and its generic point is the center of valZ,s\val_{Z,s} on Zβ€²Z^{\prime} for all ss in the relative interior of Οƒ^Jβ€²β€²\hat{\sigma}^{\prime}_{J^{\prime}}.

  • (d)

    For each toric divisor GG of Zβ€²Z^{\prime}, the map s↦valZ,s⁑(G)s\mapsto\val_{Z,s}(G) is linear on each cone of Ξ£β€²\Sigma^{\prime}.

With the notation of (c), assume that HJβ€²β€²H^{\prime}_{J^{\prime}} is non-empty and let Οƒ^J\hat{\sigma}_{J} be the smallest cone of Ξ£\Sigma containing Οƒ^Jβ€²β€²\hat{\sigma}^{\prime}_{J^{\prime}}. We then have ρ⁑(HJβ€²β€²)=HJ\rho(H^{\prime}_{J^{\prime}})=H_{J}, and we claim that

(3.7) Οβˆ—β€‹π’ͺHJβ€²β€²=π’ͺHJ.\rho_{*}\mathcal{O}_{H^{\prime}_{J^{\prime}}}=\mathcal{O}_{H_{J}}.

Indeed, denote by ΞΆJβ€²β€²\zeta^{\prime}_{J^{\prime}} and ΞΆJ\zeta_{J} the generic points of HJβ€²β€²H^{\prime}_{J^{\prime}} and HJH_{J} respectively. Since HJH_{J} is normal, (3.7) amounts to the fact κ⁑(ΞΆJ)\kappa(\zeta_{J}) is algebraically closed in κ⁑(ΞΆJβ€²β€²)\kappa(\zeta^{\prime}_{J^{\prime}}) (cf.Β [EGA, III.4.3.12]). But HJβ€²β€²H^{\prime}_{J^{\prime}} is the closure of a TT-orbit (HJβ€²β€²)0(H^{\prime}_{J^{\prime}})^{0} in Zβ€²Z^{\prime}, mapping to the TT-orbit HJ0:=(β‹‚j∈JHj)βˆ–(⋃jβˆ‰JHj)H_{J}^{0}:=(\bigcap_{j\in J}H_{j})\setminus(\bigcup_{j\notin J}H_{j}) in ZZ. The stabilizer of HJ0H_{J}^{0} in TT is (𝐆m,ΞΊ)J(\mathbf{G}_{m,\kappa})^{J}, so the TT-equivariant morphism (HJβ€²β€²)0β†’HJ0(H^{\prime}_{J^{\prime}})^{0}\to H_{J}^{0} has geometrically integral fibers. In particular ΞΆJβ€²β€²\zeta^{\prime}_{J^{\prime}} is the generic point of the fiber over ΞΆJ\zeta_{J}, and it follows as desired that κ⁑(ΞΆJ)\kappa(\zeta_{J}) is algebraically closed in κ⁑(ΞΆJβ€²β€²)\kappa(\zeta^{\prime}_{J^{\prime}}) (cf.Β [EGA, IV.4.5.9]).

Step 2. Let h∈PA⁑(Δ𝒳)𝐙h\in\PA(\Delta_{\mathcal{X}})_{\mathbf{Z}} be a strictly convex support function for Ξ”β€²\Delta^{\prime}. We define 𝒳′\mathcal{X}^{\prime} as the blow-up of 𝒳\mathcal{X} along the vertical fractional ideal sheaf π”žh\mathfrak{a}_{h} given in Definition 3.10.

Let ΞΎβˆˆπ’³0\xi\in\mathcal{X}_{0} be a given point and use the notation of Remark 3.8. Since 𝒳\mathcal{X} and Z:=𝐀κ⁑(ΞΎ)LZ:=\mathbf{A}^{L}_{\kappa(\xi)} are excellent we get a diagram

𝒳\textstyle{\mathcal{X}}𝒳^ΞΎ\textstyle{\widehat{\mathcal{X}}_{\xi}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}p\scriptstyle{p}q\scriptstyle{q}Z\textstyle{Z}

where pp and qq are regular, i.e. flat and with (geometrically) regular fibers (but a priori not of finite type, as opposed to a smooth morphism). By Remark 3.8 we have

(3.8) pβˆ—β€‹val𝒳^ΞΎ,s=val𝒳,s⁑ and ​qβˆ—β€‹val𝒳^ΞΎ,s=valZ,sp_{*}\val_{\widehat{\mathcal{X}}_{\xi},s}=\val_{\mathcal{X},s}\text{ and }q_{*}\val_{\widehat{\mathcal{X}}_{\xi},s}=\val_{Z,s}

for all sβˆˆΟƒIΞΎs\in\sigma_{I_{\xi}}. The subdivision of ΟƒIΞΎ\sigma_{I_{\xi}} defined by Ξ”β€²\Delta^{\prime} induces a simplicial fan decomposition Ξ£β€²\Sigma^{\prime} of 𝐑+L\mathbf{R}_{+}^{L}, to which the results of Step 1 apply. Since hh is a support function of Ξ”β€²\Delta^{\prime}, the toric κ⁑(ΞΎ)\kappa(\xi)-variety Zβ€²Z^{\prime} attached to Ξ£β€²\Sigma^{\prime} coincides in fact with the blow-up of ZZ along the toric fractional ideal sheaf

π”Ÿh:=βˆ‘{π’ͺZ​(Hm),mβˆˆπ™IΞΎ,⟨m,β‹…βŸ©β‰€h​ on ​σξ},\mathfrak{b}_{h}:=\sum\{\mathcal{O}_{Z}(H_{m}),\,m\in\mathbf{Z}^{I_{\xi}},\,\langle m,\cdot\rangle\leq h\text{ on }\sigma_{\xi}\},

where we have set Hm:=βˆ‘i∈IΞΎmi​HiH_{m}:=\sum_{i\in I_{\xi}}m_{i}H_{i}. Comparing with (3.6), we see that

pβˆ’1β€‹π”žhβ‹…π’ͺ^𝒳,ΞΎ=qβˆ’1β€‹π”Ÿhβ‹…π’ͺ^𝒳,ΞΎ.p^{-1}\mathfrak{a}_{h}\cdot\widehat{\mathcal{O}}_{\mathcal{X},\xi}=q^{-1}\mathfrak{b}_{h}\cdot\widehat{\mathcal{O}}_{\mathcal{X},\xi}.

Since blow-ups commute with flat base change (cf.Β [Liu, 8.1.12]), 𝒳^ΞΎβ€²:=𝒳′×𝒳Spec⁑𝒳^ΞΎ\widehat{\mathcal{X}}^{\prime}_{\xi}:=\mathcal{X}^{\prime}\times_{\mathcal{X}}\spec\widehat{\mathcal{X}}_{\xi} sits in a commutative diagram

(3.9) 𝒳′\textstyle{\mathcal{X}^{\prime}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Ο€\scriptstyle{\pi}𝒳^ΞΎβ€²\textstyle{\widehat{\mathcal{X}}^{\prime}_{\xi}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}pβ€²\scriptstyle{p^{\prime}}qβ€²\scriptstyle{q^{\prime}}Zβ€²\textstyle{Z^{\prime}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ρ\scriptstyle{\rho}𝒳\textstyle{\mathcal{X}}𝒳^ΞΎ\textstyle{\widehat{\mathcal{X}}_{\xi}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}p\scriptstyle{p}q\scriptstyle{q}Z\textstyle{Z}

where the two squares are Cartesian. The morphisms pβ€²p^{\prime} and qβ€²q^{\prime} are also regular, since the latter property is preserved under finite type base change (cf.Β [EGA, IV.6.8.3]).

Let (eiβ€²)i∈IΞΎβ€²(e^{\prime}_{i})_{i\in I^{\prime}_{\xi}} be the set of vertices of Ξ”β€²\Delta^{\prime} contained in ΟƒIΞΎ\sigma_{I_{\xi}}, so that each ray 𝐑+​eiβ€²\mathbf{R}_{+}e^{\prime}_{i} belongs to the fan Ξ£β€²\Sigma^{\prime}. If we let Hiβ€²H^{\prime}_{i} be the corresponding toric prime divisor of Zβ€²Z^{\prime} and pick Jβ€²βŠ‚IΞΎβ€²J^{\prime}\subset I^{\prime}_{\xi} then HJβ€²β€²=β‹‚j∈Jβ€²HjH^{\prime}_{J^{\prime}}=\bigcap_{j\in J^{\prime}}H_{j} is normal, irreducible, and non-empty iff the ejβ€²e^{\prime}_{j}, j∈Jβ€²j\in J^{\prime} span a face ΟƒJβ€²β€²\sigma^{\prime}_{J^{\prime}} of Ξ”β€²\Delta^{\prime}, by property (c). Since qβ€²q^{\prime} is regular, if follows that qβ€²βˆ’1​(HJβ€²β€²)q^{\prime-1}(H^{\prime}_{J^{\prime}}) is normal and is either empty or of codimension |Jβ€²||J^{\prime}|. It is furthermore irreducible, by (3.7) and Lemma 3.12 below. In particular, (qβ€²βˆ’1​(Hiβ€²))i∈IΞΎβ€²(q^{\prime-1}(H^{\prime}_{i}))_{i\in I^{\prime}_{\xi}} is exactly the set of irreducible components of the special fiber of 𝒳^ΞΎβ€²\widehat{\mathcal{X}}^{\prime}_{\xi}. We then easily obtain the analogue of (i)-(iv) of Theorem 3.11 with 𝒳^ΞΎβ€²\widehat{\mathcal{X}}^{\prime}_{\xi}, ΟƒIΞΎ\sigma_{I_{\xi}} and val𝒳^ΞΎ\val_{\widehat{\mathcal{X}}_{\xi}} in place of 𝒳′\mathcal{X}^{\prime}, Δ𝒳\Delta_{\mathcal{X}} and val𝒳\val_{\mathcal{X}}.

On the other hand, for each irreducible component Eβ€²E^{\prime} of 𝒳0β€²\mathcal{X}^{\prime}_{0} dominating ΞΎ\xi, we claim that the divisor pβ€²βˆ’1​(Eβ€²)p^{\prime-1}(E^{\prime}) is irreducible. Indeed, each irreducible component of the divisor pβ€²βˆ’1​(Eβ€²)p^{\prime-1}(E^{\prime}) is of the form qβ€²βˆ’1​(Hiβ€²)q^{\prime-1}(H^{\prime}_{i}) for some i∈IΞΎβ€²i\in I^{\prime}_{\xi}. If we denote by ΞΎβ€²\xi^{\prime} and Ξ·iβ€²\eta^{\prime}_{i} the generic points of Eβ€²E^{\prime} and pβ€²βˆ’1​(Hiβ€²)p^{\prime-1}(H_{i}^{\prime}) respectively then we have on the one hand p′​(Ξ·iβ€²)=ΞΎβ€²p^{\prime}(\eta^{\prime}_{i})=\xi^{\prime} since pβ€²p^{\prime} is flat. On the other hand, Ξ·iβ€²\eta_{i}^{\prime} is the center of val𝒳^ΞΎ,eiβ€²\val_{\widehat{\mathcal{X}}_{\xi},e^{\prime}_{i}} on 𝒳^ΞΎβ€²\widehat{\mathcal{X}}^{\prime}_{\xi}, hence p′​(Ξ·iβ€²)=c𝒳′​(val𝒳,eiβ€²)p^{\prime}(\eta_{i}^{\prime})=c_{\mathcal{X}^{\prime}}(\val_{\mathcal{X},e^{\prime}_{i}}) thanks to (3.8). For dimension reason it follows that emb𝒳⁑(eiβ€²)=xEβ€²βˆˆX\emb_{\mathcal{X}}(e^{\prime}_{i})=x_{E^{\prime}}\in X, and the injectivity of emb𝒳\emb_{\mathcal{X}} shows that ii is uniquely determined by Eβ€²E^{\prime}, which implies as desired that pβ€²βˆ’1​(Eβ€²)p^{\prime-1}(E^{\prime}) is irreducible.

We may thus write the irreducible components of 𝒳0β€²\mathcal{X}^{\prime}_{0} dominating ΞΎ\xi as (Eiβ€²)i∈IΞΎβ€²(E^{\prime}_{i})_{i\in I^{\prime}_{\xi}}, with the property that

pβ€²βˆ’1​(Eiβ€²)=qβ€²βˆ’1​(Hiβ€²).p^{\prime-1}(E^{\prime}_{i})=q^{\prime-1}(H^{\prime}_{i}).

By flat descent it follows that Eiβ€²E^{\prime}_{i} is normal over ΞΎ\xi. It is also 𝐐\mathbf{Q}-Cartier, since a Weil divisor is Cartier at a point iff its restriction to the formal neighborhood of that point is Cartier. It is now easy to conclude the proof of (i)-(iv), using the analogous properties for 𝒳^ΞΎβ€²\widehat{\mathcal{X}}^{\prime}_{\xi} together with (3.8). ∎

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