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4. Toric varieties [02PA]

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4. Toric varieties

In this section we recall some basic facts about the algebraic geometry of toric varieties and schemes. In the first place, we consider toric varieties over a field and then toric schemes over a DVR. We refer to [KKMS73, Oda88, Ful93, Ewa96] for more details.

We will use the notations of the previous section concerning concave functions and polyhedra, with the proviso that the vector space NℝN_{\mathbb{R}} will always be equipped with a lattice NN and most of the objects we consider will be compatible with this integral structure, even if not said explicitly. In particular, from now on by a fan (Definition 3.13) we will mean a rational fan and by a polytope we will mean a lattice polytope.

4.1. Fans and toric varieties

Let KK be a field and 𝕋≃𝔾mn\mathbb{T}\simeq\mathbb{G}_{m}^{n} a split torus over KK. We alternatively denote it by 𝕋K\mathbb{T}_{K} if we want to refer to its field of definition.

Definition 4.1.

A toric variety is a normal variety XX over KK equipped with a dense open embedding 𝕋↪X\mathbb{T}\hookrightarrow X and an action μ:𝕋×X→X\mu\colon\mathbb{T}\times X\to X that extends the action of 𝕋\mathbb{T} on itself by translations. When we want to stress the torus, we will call XX a toric variety with torus 𝕋\mathbb{T}.

Toric varieties can be described in combinatorial terms as we recall in the sequel. Let N=Hom⁡(𝔾m,𝕋)≃ℤnN=\operatorname{Hom}(\mathbb{G}_{m},\mathbb{T})\simeq\mathbb{Z}^{n} be the lattice of one-parameter subgroups of 𝕋\mathbb{T} and M=Hom⁡(𝕋,𝔾m)=N∨=Hom⁡(N,ℤ)M=\operatorname{Hom}(\mathbb{T},\mathbb{G}_{m})=N^{\vee}=\operatorname{Hom}(N,\mathbb{Z}) its dual lattice of characters of 𝕋\mathbb{T}. For a ring RR we set NR=N⊗RN_{R}=N\otimes R and MR=M⊗RM_{R}=M\otimes R.

To a fan Σ\Sigma we associate a toric variety XΣX_{\Sigma} over KK by gluing together the affine toric varieties corresponding to the cones of the fan. For σ∈Σ\sigma\in\Sigma, let σ∨\sigma^{\vee} be the dual cone (Definition 3.67) and set

Mσ=σ∨∩M={m∈M∣⟨m,u⟩≥0,∀u∈σ}M_{\sigma}=\sigma^{\vee}\cap M=\{m\in M\mid\langle m,u\rangle\geq 0,\ \forall u\in\sigma\}

for the saturated semigroup of its lattice points. We consider the semigroup algebra

K[Mσ]={∑m∈Mσαmχm|αm∈K,αm=0 for almost all m}K[M_{\sigma}]=\Big\{\sum_{m\in M_{\sigma}}\alpha_{m}\chi^{m}\Big|\alpha_{m}\in K,\alpha_{m}=0\text{ for almost all }m\Big\}

of formal finite sums of elements of MσM_{\sigma} with the natural ring structure. It is an integrally closed domain of Krull dimension nn. We set Xσ=Spec⁡(K⁡[Mσ])X_{\sigma}=\operatorname{Spec}(K[M_{\sigma}]) for the associated affine toric variety. If τ\tau is a face of σ\sigma we have that K⁡[Mτ]K[M_{\tau}] is a localization of K⁡[Mσ]K[M_{\sigma}]. Hence there is an inclusion of open sets

Xτ=Spec⁡(K⁡[Mτ])⸦⟶Xσ=Spec⁡(K⁡[Mσ]).X_{\tau}=\operatorname{Spec}(K[M_{\tau}])\lhook\joinrel\longrightarrow X_{\sigma}=\operatorname{Spec}(K[M_{\sigma}]).

For σ,σ′∈Σ\sigma,\sigma^{\prime}\in\Sigma, the affine toric varieties XσX_{\sigma}, Xσ′X_{\sigma^{\prime}} glue together through the open subset Xσ∩σ′X_{\sigma\cap\sigma^{\prime}} corresponding to their common face. Thus these affine varieties glue together to form the toric variety

XΣ=⋃σ∈ΣXσ.X_{\Sigma}=\bigcup_{\sigma\in\Sigma}X_{\sigma}.

This is a normal variety over KK of dimension nn. When we need to specify the field of definition we will denote it as XΣ,KX_{\Sigma,K}. We denote by 𝒪XΣ\mathcal{O}_{X_{\Sigma}} its structural sheaf and by 𝒦XΣ\mathcal{K}_{X_{\Sigma}} its sheaf of rational functions. The open subsets Xσ⊂XΣX_{\sigma}\subset X_{\Sigma} may be denoted by XΣ,σX_{\Sigma,\sigma} when we want to include the ambient toric variety in the notation.

The cone {0}\{0\}, that we denote simply by 00, is a face of every cone and its associated affine scheme

X0=Spec⁡(K⁡[M])X_{0}=\operatorname{Spec}(K[M])

is an open subset of all of the schemes XσX_{\sigma}. This variety is an algebraic group over KK canonically isomorphic to 𝕋\mathbb{T}. We identify this variety with 𝕋\mathbb{T} and call it the principal open subset of XΣX_{\Sigma}.

For each σ∈Σ\sigma\in\Sigma, the homomorphism

K⁡[Mσ]→K⁡[M]⊗K⁡[Mσ],χm↦χm⊗χmK[M_{\sigma}]\to K[M]\otimes K[M_{\sigma}],\quad\chi^{m}\mapsto\chi^{m}\otimes\chi^{m}

induces an action of 𝕋\mathbb{T} on XσX_{\sigma}. This action is compatible with the inclusion of open sets and so it extends to an action on the whole of XΣX_{\Sigma}

μ:𝕋×XΣ⟶XΣ.\mu\colon\mathbb{T}\times X_{\Sigma}\longrightarrow X_{\Sigma}.

Thus we have obtained a toric variety in the sense of Definition 4.1. In fact, all toric varieties are obtained in this way.

Theorem 4.2.

The correspondence Σ↦XΣ\Sigma\mapsto X_{\Sigma} is a bijection between the set of fans in NℝN_{\mathbb{R}} and the set of isomorphism classes of toric varieties with torus 𝕋\mathbb{T}.

Proof.

This result is [KKMS73, §I.2, Theorem 6(i)]. ∎

For each σ∈Σ\sigma\in\Sigma, the set of KK-rational points in XσX_{\sigma} can be identified with the set of semigroup homomorphisms from (Mσ,+)(M_{\sigma},+) to the semigroup (K,×):=K×∪{0}(K,\times):=K^{\times}\cup\{0\}. That is,

Xσ​(K)=Homsg⁡(Mσ,(K,×)).X_{\sigma}(K)=\operatorname{Hom}_{\operatorname{sg}}(M_{\sigma},(K,\times)).

In particular, the set of KK-rational points of the algebraic torus can be written intrinsically as

𝕋⁡(K)=Homsg⁡(M0,(K,×))=Homgp⁡(M,K×)≃(K×)n.\mathbb{T}(K)=\operatorname{Hom}_{\operatorname{sg}}(M_{0},(K,\times))=\operatorname{Hom}_{\text{\rm gp}}(M,K^{\times})\simeq(K^{\times})^{n}.

Every affine toric variety has a distinguished rational point: we will denote by xσ∈Xσ​(K)=Homsg⁡(Mσ,(K,×))x_{\sigma}\in X_{\sigma}(K)=\operatorname{Hom}_{\operatorname{sg}}(M_{\sigma},(K,\times)) the point given by the semigroup homomorphism

Mσ∋m⟼{1, if −m∈Mσ,0, otherwise.M_{\sigma}\ni m\longmapsto\begin{cases}1,&\text{ if }-m\in M_{\sigma},\\ 0,&\text{ otherwise}.\end{cases}

For instance, the point x0∈X0=𝕋x_{0}\in X_{0}=\mathbb{T} is the unit of 𝕋\mathbb{T}.

Most algebro-geometric properties of the toric scheme translate into combinatorial properties of the fan. In particular, XΣX_{\Sigma} is proper if and only if the fan is complete in the sense that |Σ|=Nℝ|\Sigma|=N_{\mathbb{R}}. The variety XΣX_{\Sigma} is smooth if and only if every cone σ∈Σ\sigma\in\Sigma can be written as σ=ℝ≥0​v1+⋯+ℝ≥0​vk\sigma=\mathbb{R}_{\geq 0}v_{1}+\cdots+\mathbb{R}_{\geq 0}v_{k} with v1,…,vkv_{1},\dots,v_{k} which are part of an integral basis of NN.

Example 4.3.

Let ΣΔn\Sigma_{\Delta^{n}} be the fan in Example 3.70. The toric variety XΣΔnX_{\Sigma_{\Delta^{n}}} is the projective space ℙKn\mathbb{P}^{n}_{K}. More generally, to a polytope Δ⊂Mℝ\Delta\subset M_{\mathbb{R}} of maximal dimension we can associate a complete toric variety XΣΔX_{\Sigma_{\Delta}}, where ΣΔ\Sigma_{\Delta} is the fan of Example 3.71.

4.2. Orbits and equivariant morphisms

The action of the torus induces a decomposition of a toric variety into disjoint orbits. These orbits are in one to one correspondence with the cones of the fan. Let σ∈Σ\sigma\in\Sigma and set

(4.4) N⁡(σ)=N/(N∩ℝ​σ),M⁡(σ)=N​(σ)∨=M∩σ⊥,N(\sigma)=N/(N\cap\mathbb{R}\sigma),\quad M(\sigma)=N(\sigma)^{\vee}=M\cap\sigma^{\bot},

where σ⊥\sigma^{\bot} denotes the orthogonal space to σ\sigma. We will denote by πσ:N→N⁡(σ)\pi_{\sigma}\colon N\to N(\sigma) the projection of lattices. By abuse of notation, we will also denote by πσ:Nℝ→N​(σ)ℝ\pi_{\sigma}\colon N_{\mathbb{R}}\to N(\sigma)_{\mathbb{R}} the induced projection of vector spaces.

The orthogonal space σ⊥\sigma^{\bot} is the maximal linear space inside σ∨\sigma^{\vee} and M⁡(σ)M(\sigma) is the maximal subgroup sitting inside the semigroup MσM_{\sigma}. Set

O⁡(σ)=Spec⁡(K⁡[M⁡(σ)]),O(\sigma)=\operatorname{Spec}(K[M(\sigma)]),

which is a torus over KK of dimension n−dim(σ)n-\dim(\sigma). The surjection of rings

K[Mσ]⟶K[M(σ)],χa⟼{χa, if a∈σ⊥,0, if ​a∉σ⊥,K[M_{\sigma}]\longrightarrow K[M(\sigma)],\quad\chi^{a}\longmapsto\begin{cases}\chi^{a},&\text{ if }a\in\sigma^{\bot},\\ 0,&\text{ if }a\notin\sigma^{\bot},\end{cases}

induces a closed immersion O⁡(σ)↪XσO(\sigma)\hookrightarrow X_{\sigma}. In terms of rational points, the inclusion O⁡(σ)​(K)↪Xσ​(K)O(\sigma)(K)\hookrightarrow X_{\sigma}(K) sends a group homomorphism γ:M⁡(σ)→K×\gamma\colon M(\sigma)\to K^{\times} to the semigroup homomorphism γ~:Mσ→(K,×){\widetilde{\gamma}}\colon M_{\sigma}\to(K,\times) obtained by extending γ\gamma by zero. In particular, the distinguished point xσ∈Xσ​(K)x_{\sigma}\in X_{\sigma}(K) belongs to the image of O​(σ)​(K)O(\sigma)(K) by the above inclusion. Composing with the open immersion Xσ↪XΣX_{\sigma}\hookrightarrow X_{\Sigma}, we identify O⁡(σ)O(\sigma) with a locally closed subvariety of XΣX_{\Sigma}. For instance, the orbit associated to the cone 00 agrees with the principal open subset X0X_{0}. In fact, if we consider xσx_{\sigma} as a rational point of XΣX_{\Sigma}, then O⁡(σ)O(\sigma) agrees with the orbit of xσx_{\sigma} by 𝕋\mathbb{T}.

We denote by V⁡(σ)V(\sigma) the Zariski closure of O⁡(σ)O(\sigma) with its induced structure of reduced closed subvariety of XΣX_{\Sigma}. The subvariety V⁡(σ)V(\sigma) has a natural structure of toric variety. To see it, we consider the fan on N​(σ)ℝN(\sigma)_{\mathbb{R}}

(4.5) Σ⁡(σ):={πσ​(τ)|τ⊃σ}.\Sigma(\sigma):=\{\pi_{\sigma}(\tau)|\tau\supset\sigma\}.

This fan is called the star of σ\sigma in Σ\Sigma. For each τ∈Σ\tau\in\Sigma with σ⊂τ\sigma\subset\tau, set τ¯=πσ​(τ)∈Σ⁡(σ){\overline{\tau}}=\pi_{\sigma}(\tau)\in\Sigma(\sigma). Then, M​(σ)τ¯=M⁡(σ)∩Mτ.M(\sigma)_{{\overline{\tau}}}=M(\sigma)\cap M_{\tau}. There is a surjection of rings

K[Mτ]⟶K[M(σ)τ¯],χm⟼{χm, if m∈σ⊥,0, if ​m∉σ⊥,K[M_{\tau}]\longrightarrow K[M(\sigma)_{{\overline{\tau}}}],\quad\chi^{m}\longmapsto\begin{cases}\chi^{m},&\text{ if }m\in\sigma^{\bot},\\ 0,&\text{ if }m\notin\sigma^{\bot},\end{cases}

that defines a closed immersion Xτ¯↪XτX_{{\overline{\tau}}}\hookrightarrow X_{\tau}. These maps glue together to give a closed immersion ισ:XΣ⁡(σ)↪XΣ\iota_{\sigma}\colon X_{\Sigma(\sigma)}\hookrightarrow X_{\Sigma}.

Proposition 4.6.

The closed immersion ισ\iota_{\sigma} induces an isomorphism XΣ⁡(σ)≃V⁡(σ).X_{\Sigma(\sigma)}\simeq V(\sigma).

Proof.

Since the image of each Xτ¯X_{{\overline{\tau}}} contains O⁡(σ)O(\sigma) as a dense orbit, we deduce the result from the construction of ισ\iota_{\sigma}. ∎

In view of this proposition, we will identify V⁡(σ)V(\sigma) with XΣ⁡(σ)X_{\Sigma(\sigma)} and consider it a toric variety.

We now discuss more general equivariant morphisms of toric varieties.

Definition 4.7.

Let 𝕋i≃𝔾mni\mathbb{T}_{i}\simeq\mathbb{G}_{m}^{n_{i}}, i=1,2i=1,2, be split tori over KK, and ρ:𝕋1→𝕋2\rho\colon\mathbb{T}_{1}\to\mathbb{T}_{2} a group morphism. Let XiX_{i}, i=1,2i=1,2, be toric varieties with torus 𝕋i\mathbb{T}_{i}. A morphism φ:X1→X2\varphi\colon X_{1}\to X_{2} is ρ\rho-equivariant if the diagram

𝕋1×X1\textstyle{\mathbb{T}_{1}\times X_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}μ\scriptstyle{\mu}ρ×φ\scriptstyle{\rho\times\varphi}X1\textstyle{X_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}φ\scriptstyle{\varphi}𝕋2×X2\textstyle{\mathbb{T}_{2}\times X_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}μ\scriptstyle{\mu}X2\textstyle{X_{2}}

is commutative. A morphism φ:X1→X2\varphi\colon X_{1}\to X_{2} is ρ\rho-toric if its restriction to 𝕋1\mathbb{T}_{1} agrees with ρ\rho. We say that φ\varphi is equivariant or toric if it is ρ\rho-equivariant or ρ\rho-toric, respectively, for some ρ\rho.

Toric morphisms are equivariant. Indeed, a morphism is toric if and only if it is equivariant and sends the distinguished point x1,0∈X1​(K)x_{1,0}\in X_{1}(K) to the distinguished point x2,0∈X2​(K)x_{2,0}\in X_{2}(K).

The inclusion V⁡(σ)→XΣV(\sigma)\to X_{\Sigma} is an example of equivariant morphism that is not toric. Moreover, the underlying morphism of tori depends on the choice of a section of the projection πσ:N→N⁡(σ)\pi_{\sigma}\colon N\to N(\sigma).

Equivariant morphisms whose image intersects the principal open subset can be characterized in combinatorial terms. Let 𝕋i\mathbb{T}_{i}, i=1,2i=1,2, be split tori over KK. Put Ni=Hom⁡(𝔾m,𝕋i)N_{i}=\operatorname{Hom}(\mathbb{G}_{m},\mathbb{T}_{i}) and let Σi\Sigma_{i} be fans in Ni,ℝN_{i,\mathbb{R}}. Let H:N1→N2H\colon N_{1}\to N_{2} be a linear map such that, for every cone σ1∈Σ1\sigma_{1}\in\Sigma_{1}, there exists a cone σ2∈Σ2\sigma_{2}\in\Sigma_{2} with H⁡(σ1)⊂σ2H(\sigma_{1})\subset\sigma_{2}, and let p∈XΣ2,0​(K)p\in X_{\Sigma_{2},0}(K) be a rational point. The linear map induces a group homomorphism

ρH:𝕋1→𝕋2.\rho_{H}\colon\mathbb{T}_{1}\to\mathbb{T}_{2}.

Let σi∈Σi\sigma_{i}\in\Sigma_{i}, i=1,2,i=1,2, be cones such that H⁡(σ1)⊂σ2H(\sigma_{1})\subset\sigma_{2}. Let H∨:M2→M1H^{\vee}\colon M_{2}\to M_{1} be the map dual to HH. Then there is a homomorphism of semigroups M2,σ2→M1,σ1M_{2,\sigma_{2}}\to M_{1,\sigma_{1}} which we also denote by H∨H^{\vee}. For a monomial χm∈K⁡[M2,σ2]\chi^{m}\in K[M_{2,\sigma_{2}}] we denote by χH∨​m\chi^{H^{\vee}m} its image in K⁡[M1,σ1]K[{M_{1,\sigma_{1}}}]. The assignment χm↦χm​(p)​χH∨​m\chi^{m}\mapsto\chi^{m}(p)\chi^{H^{\vee}m} induces morphisms of algebras K⁡[M2,σ2]→K⁡[M1,σ1],K[M_{2,\sigma_{2}}]\to K[M_{1,\sigma_{1}}], that, in turn, induce morphisms

Xσ1=Spec⁡(K⁡[M1,σ1])⟶Xσ2=Spec⁡(K⁡[M2,σ2]).X_{\sigma_{1}}=\operatorname{Spec}(K[M_{1,\sigma_{1}}])\longrightarrow X_{\sigma_{2}}=\operatorname{Spec}(K[M_{2,\sigma_{2}}]).

These morphisms are compatible with the restriction to open subsets, and they glue together into a ρH\rho_{H}-equivariant morphism

(4.8) φp,H:XΣ1⟶XΣ2.\varphi_{p,H}\colon X_{\Sigma_{1}}\longrightarrow X_{\Sigma_{2}}.

In case p=x2,0p=x_{2,0}, the distinguished point on the principal open subset of XΣ2X_{\Sigma_{2}}, this morphism is a toric morphism and will be denoted as φH\varphi_{H} for short.

Theorem 4.9.

Let 𝕋i\mathbb{T}_{i}, NiN_{i}, and Σi\Sigma_{i}, i=1,2i=1,2, be as above. Then the correspondence (p,H)↦φp,H(p,H)\mapsto\varphi_{p,H} is a bijection between

  1. (1)

    the set of pairs (p,H)(p,H), where H:N1→N2H\colon N_{1}\to N_{2} is a linear map such that for every cone σ1∈Σ1\sigma_{1}\in\Sigma_{1} there exists a cone σ2∈Σ2\sigma_{2}\in\Sigma_{2} with H⁡(σ1)⊂σ2H(\sigma_{1})\subset\sigma_{2}, and pp is a rational point of XΣ2,0​(K)X_{\Sigma_{2},0}(K),

  2. (2)

    the set of equivariant morphisms φ:XΣ1→XΣ2\varphi\colon X_{\Sigma_{1}}\to X_{\Sigma_{2}} whose image intersects the principal open subset of XΣ2X_{\Sigma_{2}}.

Proof.

For a point p∈XΣ2,0​(K)=𝕋2​(K)p\in X_{\Sigma_{2},0}(K)=\mathbb{T}_{2}(K), let tp:X2→X2t_{p}\colon X_{2}\to X_{2} be the morphism induced by the toric action. Denote by x1,0∈XΣ1​(K)x_{1,0}\in X_{\Sigma_{1}}(K) the distinguished point of the principal open subset of XΣ1X_{\Sigma_{1}}. The correspondence φ↦(tφ⁡(x1,0)−1∘φ,φ⁡(x1,0))\varphi\mapsto(t_{\varphi(x_{1,0})}^{-1}\circ\varphi,\varphi(x_{1,0})) establishes a bijection between the set of equivariant morphisms φ:XΣ1→XΣ2\varphi\colon X_{\Sigma_{1}}\to X_{\Sigma_{2}} whose image intersects the principal open subset of XΣ2X_{\Sigma_{2}} and the set of pairs (ϕ,p)(\phi,p), where ϕ:XΣ1→XΣ2\phi\colon X_{\Sigma_{1}}\to X_{\Sigma_{2}} is a toric morphism and p∈XΣ2,0​(K)p\in X_{\Sigma_{2},0}(K) is a rational point in the principal open subset. Then the result follows from [Oda88, Theorem 1.13]. ∎

General equivariant morphisms are obtained composing an equivariant morphism of the form φp,H:XΣ1→XΣ2\varphi_{p,H}\colon X_{\Sigma_{1}}\rightarrow X_{\Sigma_{2}} with the inclusion of XΣ2X_{\Sigma_{2}} as a toric orbit of a third toric variety.

Example 4.10.

The restriction of φp,H\varphi_{p,H} to the principal open subset can be written in coordinates by choosing basis of N1N_{1} and of N2N_{2}. Let nin_{i} be the rank of NiN_{i}. The chosen basis determine isomorphisms XΣi,0≃𝔾mniX_{\Sigma_{i},0}\simeq\mathbb{G}_{m}^{n_{i}}, which give coordinates 𝒙=(x1,…,xn1){\boldsymbol{x}}=(x_{1},\dots,x_{n_{1}}) and 𝒕=(t1,…,tn2){\boldsymbol{t}}=(t_{1},\dots,t_{n_{2}}) for XΣ1,0X_{\Sigma_{1},0} and XΣ2,0X_{\Sigma_{2},0}, respectively. We write the the linear map HH with respect to these basis as a matrix, and we denote its rows by aia_{i}, i=1,…,n2i=1,\dots,n_{2}. Write p=(p1,…,pn2)p=(p_{1},\dots,p_{n_{2}}). In these coordinates, the morphism φp,H\varphi_{p,H} is given by

φp,H​(𝒙)=(p1​𝒙a1,…,pn2​𝒙an2).\varphi_{p,H}({\boldsymbol{x}})=(p_{1}{\boldsymbol{x}}^{a_{1}},\dots,p_{n_{2}}{\boldsymbol{x}}^{a_{n_{2}}}).

We now show how to refine the Stein factorization for an equivariant morphism in terms of the combinatorial data. Let NiN_{i}, Σi\Sigma_{i} HH and pp be as in Theorem 4.9. The linear map HH factorizes as

N1​-↠Hsurj​N3:=H⁡(N1)​⸦⟶Hsat​N4:=sat⁡(N3)​⸦⟶Hinj​N2,N_{1}\overset{H_{\operatorname{surj}}}{\relbar\joinrel\twoheadrightarrow}N_{3}:=H(N_{1})\overset{H_{\operatorname{sat}}}{\lhook\joinrel\longrightarrow}N_{4}:=\operatorname{sat}(N_{3})\overset{H_{\operatorname{inj}}}{\lhook\joinrel\longrightarrow}N_{2},

where N3N_{3} is the image of HH and N4N_{4} is the saturation of N3N_{3} with respect to N2N_{2}. Clearly N3,ℝ=N4,ℝN_{3,\mathbb{R}}=N_{4,\mathbb{R}}. By restriction, the fan Σ2\Sigma_{2} induces a fan in this linear space. We will call this fan either Σ3\Sigma_{3} or Σ4\Sigma_{4}, depending on the lattice we are considering. Applying the combinatorial construction of equivariant morphisms, we obtain a diagram

XΣ1​⟶φHsurj​XΣ3​⟶φHsat​XΣ4​⟶φp,Hinj​XΣ2,X_{\Sigma_{1}}\overset{\varphi_{H_{\operatorname{surj}}}}{\longrightarrow}X_{\Sigma_{3}}\overset{\varphi_{H_{\operatorname{sat}}}}{\longrightarrow}X_{\Sigma_{4}}\overset{\varphi_{p,H_{\operatorname{inj}}}}{\longrightarrow}X_{\Sigma_{2}},

where the first morphism has connected fibres (see [Oda88, Proposition 1.14]), the second morphism is finite and surjective.

The third morphism is also finite and can be further factorized as a normalization followed by a closed immersion. In general, consider a saturated sublattice QQ of NN, Σ\Sigma a fan in NℝN_{\mathbb{R}} and p∈XΣ,0​(K)p\in X_{\Sigma,0}(K). Let ΣQ\Sigma_{Q} be the induced fan in QℝQ_{\mathbb{R}} and ι:Q↪N\iota\colon Q\hookrightarrow N the inclusion of QQ into NN. Then, we have a finite equivariant morphism

φp,ι:XΣQ⟶XΣ.\varphi_{p,\iota}\colon X_{\Sigma_{Q}}\longrightarrow X_{\Sigma}.

Set P=Q∨=M/Q⊥P=Q^{\vee}=M/Q^{\bot} and let ι∨:M→P\iota^{\vee}\colon M\to P be the dual of ι\iota. Let σ∈Σ\sigma\in\Sigma and σ′=σ∩Qℝ∈ΣQ\sigma^{\prime}=\sigma\cap Q_{\mathbb{R}}\in\Sigma_{Q}. The natural semigroup homomorphisms Mσ→Pσ′M_{\sigma}\to P_{\sigma^{\prime}} factors as

Mσ-↠MQ,σ:=(Mσ+Q⊥)/Q⊥⸦⟶Pσ′:=P∩(σ′)∨.M_{\sigma}\relbar\joinrel\twoheadrightarrow{M_{Q,\sigma}}:=(M_{\sigma}+Q^{\bot})/Q^{\bot}\lhook\joinrel\longrightarrow P_{\sigma^{\prime}}:=P\cap(\sigma^{\prime})^{\vee}.

The first arrow is the projection and will be denoted as m↦[m]m\mapsto[m], while the second one is the inclusion of MQ,σ{M_{Q,\sigma}} into its saturation with respect to PP. We have a diagram of KK-algebra morphisms

K⁡[Mσ]-↠K⁡[MQ,σ]⸦⟶K⁡[Pσ′],K[M_{\sigma}]\relbar\joinrel\twoheadrightarrow K[{M_{Q,\sigma}}]\lhook\joinrel\longrightarrow K[P_{\sigma^{\prime}}],

where the left map is given by χm↦χm​(p)​χ[m]\chi^{m}\mapsto\chi^{m}(p)\chi^{[m]}, and the right map is given by χ[m]↦χι∨​m\chi^{[m]}\mapsto\chi^{\iota^{\vee}m}. Let Yσ,Q,p≃Spec⁡(K⁡[MQ,σ])Y_{\sigma,Q,p}\simeq\operatorname{Spec}(K[{M_{Q,\sigma}}]) be the closed subvariety of XσX_{\sigma} given by the left surjection. Then we have induced maps

Xσ′-↠Yσ,Q,p⸦⟶Xσ.X_{\sigma^{\prime}}\relbar\joinrel\twoheadrightarrow Y_{\sigma,Q,p}\lhook\joinrel\longrightarrow X_{\sigma}.

These maps are compatible with the restriction to open subsets and so they glue together into maps

(4.11) XΣQ-↠YΣ,Q,p⸦⟶XΣ.X_{\Sigma_{Q}}\relbar\joinrel\twoheadrightarrow Y_{\Sigma,Q,p}\lhook\joinrel\longrightarrow X_{\Sigma}.

Then YΣ,Q,pY_{\Sigma,Q,p} is the closure of the orbit of pp under the action of the subtorus of 𝕋\mathbb{T} determined by QQ, while the toric variety XΣQX_{\Sigma_{Q}} is the normalization of YΣ,Q,pY_{\Sigma,Q,p}.

When p=x0p=x_{0}, the subvariety YΣ,Q,pY_{\Sigma,Q,p} will be denoted by YΣ,QY_{\Sigma,Q} for short.

Definition 4.12.

A subvariety YY of XΣX_{\Sigma} will be called a toric subvariety (respectively, a translated toric subvariety) if it is of the form YΣ,QY_{\Sigma,Q} (respectively, YΣ,Q,pY_{\Sigma,Q,p}) for a saturated sublattice Q⊂NQ\subset N and p∈XΣ,0​(K)p\in X_{\Sigma,0}(K).

A translated toric subvariety is not necessarily a toric variety in the sense of Definition 4.1, since it may be non-normal.

Example 4.13.

Let N=ℤ2N=\mathbb{Z}^{2}, (a,b)∈N(a,b)\in N with gcd⁡(a,b)=1\gcd(a,b)=1 and ι:Q↪N\iota\colon Q\hookrightarrow N the saturated sublattice generated by (a,b)(a,b). Let Σ\Sigma be the fan in NℝN_{\mathbb{R}} of Example 3.70. Then XΣ=ℙ2X_{\Sigma}=\mathbb{P}^{2} with projective coordinates (x0:x1:x2)(x_{0}:x_{1}:x_{2}). The fan induced in QℝQ_{\mathbb{R}} has three cones: ΣQ={ℝ≤0,{0},ℝ≥0}\Sigma_{Q}=\{\mathbb{R}_{\leq 0},\{0\},\mathbb{R}_{\geq 0}\}. Thus XΣQ=ℙ1X_{\Sigma_{Q}}=\mathbb{P}^{1}. Let p=(1:p1:p2)p=(1:p_{1}:p_{2}) be a point of XΣ,0​(K)X_{\Sigma,0}(K). Then φp,ι((1:t))=(1:p1ta:p2tb)\varphi_{p,\iota}((1:t))=(1:p_{1}t^{a}:p_{2}t^{b}). Therefore, YΣ,Q,pY_{\Sigma,Q,p} is the curve of equation

p2a​x0a​x1b−p1b​x0b​x2a=0.p_{2}^{a}x_{0}^{a}x_{1}^{b}-p_{1}^{b}x_{0}^{b}x_{2}^{a}=0.

In general, this curve is not normal. Hence it is not a toric variety.

4.3. 𝕋\mathbb{T}-Cartier divisors and toric line bundles

When studying toric varieties, the objects that admit a combinatorial description are those that are compatible with the torus action. These objects are enough for many purposes. For instance, the divisor class group of a toric variety is generated by invariant divisors.

Let π2:𝕋×X→X\pi_{2}\colon\mathbb{T}\times X\to X denote the projection to the second factor and μ:𝕋×X→X\mu\colon\mathbb{T}\times X\to X the torus action. A Cartier divisor DD is invariant if and only if

π2∗​D=μ∗​D.\pi_{2}^{\ast}D=\mu^{\ast}D.
Definition 4.14.

Let XX the a toric variety with torus 𝕋\mathbb{T}. A Cartier divisor on XX is called a 𝕋\mathbb{T}-Cartier divisor if it is invariant under the action of 𝕋\mathbb{T} on XX.

The combinatorial description of 𝕋\mathbb{T}-Cartier divisors is done in terms of virtual support functions.

Definition 4.15.

Let Σ\Sigma be a fan in NℝN_{\mathbb{R}}. A function Ψ:|Σ|→ℝ\Psi\colon|\Sigma|\to\mathbb{R} is called a virtual support function on Σ\Sigma if it is a conic HH-lattice function (Definition 3.88). Alternatively, a virtual support function is a function Ψ:|Σ|→ℝ\Psi\colon|\Sigma|\to\mathbb{R} such that, for every cone σ∈Σ\sigma\in\Sigma, there exists mσ∈Mm_{\sigma}\in M with Ψ⁡(u)=⟨mσ,u⟩\Psi(u)=\langle m_{\sigma},u\rangle for all u∈σu\in\sigma. A set of functionals {mσ}σ∈Σ\{m_{\sigma}\}_{\sigma\in\Sigma} as above is called a set of defining vectors of Ψ\Psi. A concave virtual support function on a complete fan will be called a support function.

A support function on a complete fan in the sense of the previous definition, is the support function of a polytope as in Example 3.16: it is the support function of the polytope

conv⁡({mσ}σ∈Σn)⊂Mℝ,\operatorname{conv}(\{m_{\sigma}\}_{\sigma\in\Sigma^{n}})\subset M_{\mathbb{R}},

where Σn\Sigma^{n} is the subset of nn-dimensional cones of Σ\Sigma.

Two vectors m,m′∈Mm,m^{\prime}\in M define the same functional on a cone σ\sigma if and only if m−m′∈σ⊥m-m^{\prime}\in\sigma^{\bot}. Hence, for a given virtual support function Ψ\Psi on a fan Σ\Sigma, each defining vector mσm_{\sigma} is unique up to the orthogonal space σ⊥\sigma^{\bot}. In particular, mσ∈Mm_{\sigma}\in M is uniquely defined for σ∈Σn\sigma\in\Sigma^{n} and, in the other extreme, m0m_{0} can be any point of MM.

Let {mσ}σ∈Σ\{m_{\sigma}\}_{\sigma\in\Sigma} be a set of defining vectors of Ψ\Psi. These vectors have to satisfy the compatibility condition

(4.16) mσ|σ∩σ′=mσ′|σ∩σ′​ for all ​σ,σ′∈Σ.m_{\sigma}|_{\sigma\cap\sigma^{\prime}}=m_{\sigma^{\prime}}|_{\sigma\cap\sigma^{\prime}}\mbox{ for all }\sigma,\sigma^{\prime}\in\Sigma.

On each open set XσX_{\sigma}, the vector mσm_{\sigma} determines a rational function χ−mσ\chi^{-m_{\sigma}}. For σ,σ′∈Σ\sigma,\sigma^{\prime}\in\Sigma, the above compatibility condition implies that χ−mσ/χ−mσ′\chi^{-m_{\sigma}}/\chi^{-m_{\sigma^{\prime}}} is a regular function on the overlap Xσ∩Xσ′=Xσ∩σ′X_{\sigma}\cap X_{\sigma^{\prime}}=X_{\sigma\cap\sigma^{\prime}} and so Ψ\Psi determines a Cartier divisor on XΣX_{\Sigma}:

(4.17) DΨ:={(Xσ,χ−mσ)}σ∈Σ.D_{\Psi}:=\left\{(X_{\sigma},\chi^{-m_{\sigma}})\right\}_{\sigma\in\Sigma}.

This Cartier divisor does not depend on the choice of defining vectors and it is a 𝕋\mathbb{T}-Cartier divisor. All 𝕋\mathbb{T}-Cartier divisors are obtained in this way.

Theorem 4.18.

Let Σ\Sigma be a fan in NℝN_{\mathbb{R}} and XΣX_{\Sigma} the corresponding toric variety. The correspondence Ψ↦DΨ\Psi\mapsto D_{\Psi} is a bijection between the set of virtual support functions on Σ\Sigma and the set of 𝕋\mathbb{T}-Cartier divisors on XΣX_{\Sigma}. Two Cartier divisors DΨ1D_{\Psi_{1}} and DΨ2D_{\Psi_{2}} are rationally equivalent if and only if the function Ψ1−Ψ2\Psi_{1}-\Psi_{2} is linear.

Proof.

This is proved in [KKMS73, §I.2, Theorem 9]. ∎

We next recall the relationship between Cartier divisors and line bundles in the toric case.

Definition 4.19.

Let XX be a toric variety and LL a line bundle on XX. A toric structure on LL is the choice of a non-zero vector zz on the fibre Lx0=x0∗​LL_{x_{0}}=x_{0}^{\ast}L over the distinguished point. A toric line bundle is a pair (L,z)(L,z), where LL is a line bundle on XX and zz is a toric structure on LL. A rational section ss of a toric line bundle is a toric section if it is regular and nowhere vanishing on the principal open subset X0X_{0}, and s⁡(x0)=zs(x_{0})=z. In order not to burden the notation, a toric line bundle will generally be denoted by LL, the vector zz being implicit.

Remark 4.20.

The terminology “toric structure”, “toric line bundle” and “toric section” comes from the fact that the total space of a toric line bundle V⁡(L)=𝐒𝐩𝐞𝐜X⁡(Sym⁡(L∨))V(L)=\operatorname{\bf Spec}_{X}(\operatorname{Sym}(L^{\vee})) admits a unique structure of toric variety satisfying the conditions:

  1. (1)

    zz is the distinguished point of the principal open subset;

  2. (2)

    the structural morphism V⁡(L)→XV(L)\to X is a toric morphism;

  3. (3)

    for each point x∈Xx\in X and vector w∈Lxw\in L_{x}, the morphism 𝔾m→V⁡(L)\mathbb{G}_{m}\to V(L), given by scalar multiplication λ↦λ​w\lambda\mapsto\lambda w, is equivariant;

  4. (4)

    every toric section ss determines a toric morphism U→V⁡(L)U\to V(L), where UU is the invariant open subset of regular points of ss.

This can be shown using the construction of V⁡(L)V(L) as a toric variety in [Oda88, Proposition 2.1].

Remark 4.21.

Every toric line bundle equipped with a toric section admits a unique structure of 𝕋\mathbb{T}-equivariant line bundle such that the toric section becomes an invariant section. Conversely, every 𝕋\mathbb{T}-equivariant toric line bundle admits a unique invariant toric section. Thus, there is a natural bijection between the space of 𝕋\mathbb{T}-equivariant toric line bundles and the space of toric line bundles with a toric section. In particular, every line bundle admits a structure of 𝕋\mathbb{T}-equivariant line bundle. This is not the case for higher rank vector bundles on toric varieties, nor for line bundles on other spaces with group actions like, for instance, elliptic curves.

To a Cartier divisor DD, one associates an invertible sheaf of fractional ideals of 𝒦X\mathcal{K}_{X}, denoted 𝒪⁡(D)\mathcal{O}(D). When DD is a 𝕋\mathbb{T}-Cartier divisor given by a set of defining vectors, {mσ}σ∈Σ\{m_{\sigma}\}_{\sigma\in\Sigma}, the sheaf 𝒪⁡(D)\mathcal{O}(D) can be realized as the subsheaf of 𝒪X\mathcal{O}_{X}-modules generated, in each open subset XσX_{\sigma}, by the rational function χmσ\chi^{m_{\sigma}}. The section 1∈𝒦X1\in\mathcal{K}_{X} provides us with a distinguished rational section sDs_{D} such that div⁡(sD)=D\operatorname{div}(s_{D})=D. Since DD is supported on the complement of the principal open subset, sDs_{D} is regular and no-where vanishing on X0X_{0}. We set z=sD​(x0)z=s_{D}(x_{0}). This is a toric structure on 𝒪⁡(D)\mathcal{O}(D). From now on, we will assume that 𝒪⁡(D)\mathcal{O}(D) is equipped with this toric structure. Then ((𝒪⁡(D),z),sD)((\mathcal{O}(D),z),s_{D}) is a toric line bundle with a toric section.

Theorem 4.22.

Let XX be a toric variety with torus 𝕋\mathbb{T}. Then the correspondence D↦((𝒪⁡(D),sD​(x0)),sD)D\mapsto((\mathcal{O}(D),s_{D}(x_{0})),s_{D}) determines a bijection between the sets of

  1. (1)

    𝕋\mathbb{T}-Cartier divisors on XX,

  2. (2)

    isomorphism classes of pairs (L,s)(L,s) where LL is a toric line bundle and ss is a toric section.

Proof.

We have already shown that a 𝕋\mathbb{T}-Cartier divisor produces a toric line bundle with a toric section. Let now ((L,z),s)((L,z),s) be a toric line bundle equipped with a toric section and Σ\Sigma the fan that defines XX. Since every line bundle on an affine toric variety is trivial, for each σ∈Σ\sigma\in\Sigma we can find a section sσs_{\sigma} that generates LL on XσX_{\sigma} and such that sσ​(x0)=zs_{\sigma}(x_{0})=z. Since ss is regular and nowhere vanishing on X0X_{0} and s⁡(x0)=zs(x_{0})=z, we can find elements mσ∈Mm_{\sigma}\in M such that s=χ−mσ​sσs=\chi^{-m_{\sigma}}s_{\sigma}, because any regular nowhere vanishing function on a torus is a constant times a monomial. The elements mσm_{\sigma} glue together to define a virtual support function Ψ\Psi on Σ\Sigma that does not depend on the chosen trivialization. It is easy to see that the correspondence (L,s)↦DΨ(L,s)\mapsto D_{\Psi} is the inverse of the previous one, which proves the theorem. ∎

Thanks to this result and Theorem 4.18, we can freely move between the languages of virtual support functions, 𝕋\mathbb{T}-Cartier divisors, and toric line bundles with a toric section.

Notation 4.23.

Let Ψ\Psi be a virtual support function. We will write ((LΨ,zΨ),sΨ)((L_{\Psi},z_{\Psi}),s_{\Psi}) for the toric line bundle with toric section associated to the 𝕋\mathbb{T}-Cartier divisor DΨD_{\Psi} by Theorem 4.22. When we do not need to make explicit the vector zΨz_{\Psi}, we will simply write (LΨ,sΨ)(L_{\Psi},s_{\Psi}).

We next recall the relationship between Cartier divisors and Weil divisors in the toric case.

Definition 4.24.

A 𝕋\mathbb{T}-Weil divisor on a toric variety XX is a finite formal linear combination of hypersurfaces of XX which are invariant under the torus action.

The invariant hypersurfaces of a toric variety are particular cases of the toric subvarieties considered in the previous section: they are the varieties of the form V⁡(τ)V(\tau) for τ∈Σ1\tau\in\Sigma^{1}. Hence, a 𝕋\mathbb{T}-Weil divisor is a finite formal linear combination of subvarieties of the form V⁡(τ)V(\tau) for τ∈Σ1\tau\in\Sigma^{1}.

Since the toric variety XX is normal, each Cartier divisor determines a Weil divisor. This correspondence associates to the 𝕋\mathbb{T}-Cartier divisor DΨD_{\Psi}, the 𝕋\mathbb{T}-Weil divisor

(4.25) [DΨ]=∑τ∈Σ1−Ψ(vτ)V(τ),[D_{\Psi}]=\sum_{\tau\in\Sigma^{1}}-\Psi(v_{\tau})V(\tau),

where vτ∈Nv_{\tau}\in N is the smallest nonzero lattice point in τ\tau.

Example 4.26.

We continue with the notation of examples 3.76 and 4.3. The fan ΣΔn\Sigma_{\Delta^{n}} has n+1n+1 rays. For each i=0,…,ni=0,\dots,n, the closure of the orbit corresponding to the ray generated by the vector eie_{i} is the standard hyperplane of ℙn\mathbb{P}^{n}

Hi:=V(⟨ei⟩)={(p0:…:pn)∈ℙn∣pi=0}.H_{i}:=V(\langle e_{i}\rangle)=\{(p_{0}:\dots:p_{n})\in\mathbb{P}^{n}\mid p_{i}=0\}.

The function ΨΔn\Psi_{\Delta^{n}} is a support function on ΣΔn\Sigma_{\Delta^{n}} and the 𝕋\mathbb{T}-Weil divisor associated to DΨΔnD_{\Psi_{\Delta^{n}}} is [DΨΔn]=H0[D_{\Psi_{\Delta^{n}}}]=H_{0}.

For a toric variety XΣX_{\Sigma} of dimension nn, we denote by Div𝕋⁡(XΣ)\operatorname{Div}_{\mathbb{T}}(X_{\Sigma}) its group of 𝕋\mathbb{T}-Cartier divisors, and by Zn−1𝕋​(XΣ)Z_{n-1}^{\mathbb{T}}(X_{\Sigma}) its group of 𝕋\mathbb{T}-Weil divisors. Recall that Pic⁡(XΣ)\operatorname{Pic}(X_{\Sigma}), the Picard group of XΣX_{\Sigma}, is the group of isomorphism classes of line bundles. Let An−1​(XΣ)A_{n-1}(X_{\Sigma}) denote the Chow group of cycles of dimension n−1n-1. The following result shows that these groups can computed in terms of invariant divisors.

Theorem 4.27.

Let Σ\Sigma be a fan in NℝN_{\mathbb{R}} that is not contained in any hyperplane. Then there is a commutative diagram with exact rows

    0          M                            Div𝕋⁡(XΣ)                    Pic⁡(XΣ)                    0   0          M          Zn−1𝕋​(XΣ)          An−1​(XΣ)          0    .\lx@xy@svg{\hbox{\raise 2.55554pt\hbox{\kern 5.5pt\hbox{\ignorespaces\ignorespaces\ignorespaces\hbox{\vtop{\halign{\entry@#!@&&\entry@@#!@\cr&&&&\cr&&&&\crcr}}}\ignorespaces{\hbox{\kern-5.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 29.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 29.5pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{M\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 70.29166pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\hbox{\kern 1.0pt\raise 0.0pt\hbox{\lx@xy@droprule}}\hbox{\kern-1.0pt\raise 0.0pt\hbox{\lx@xy@droprule}}}}\ignorespaces{}{\hbox{\hbox{\kern 1.0pt\raise 0.0pt\hbox{\lx@xy@droprule}}\hbox{\kern-1.0pt\raise 0.0pt\hbox{\lx@xy@droprule}}}}{\hbox{\hbox{\kern 1.0pt\raise 0.0pt\hbox{\lx@xy@droprule}}\hbox{\kern-1.0pt\raise 0.0pt\hbox{\lx@xy@droprule}}}}{\hbox{\kern 70.29166pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{\operatorname{Div}_{\mathbb{T}}(X_{\Sigma})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 148.04816pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 95.77087pt\raise-8.05554pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@hook{1}}}}}}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 95.77087pt\raise-23.54387pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 148.04816pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{\operatorname{Pic}(X_{\Sigma})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 217.9296pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{\hbox{\kern 169.58984pt\raise-8.05554pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@hook{1}}}}}}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 169.58984pt\raise-24.45613pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 217.9296pt\raise 0.0pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{0}$}}}}}}}{\hbox{\kern-5.5pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 29.5pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 29.5pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{M\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 71.4103pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 71.4103pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{Z_{n-1}^{\mathbb{T}}(X_{\Sigma})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 145.25009pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 145.25009pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{A_{n-1}(X_{\Sigma})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}$}}}}}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces{}{\hbox{\lx@xy@droprule}}\ignorespaces{\hbox{\kern 217.9296pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\lx@xy@tip{1}\lx@xy@tip{-1}}}}}}{\hbox{\lx@xy@droprule}}{\hbox{\lx@xy@droprule}}{\hbox{\kern 217.9296pt\raise-32.40059pt\hbox{\hbox{\kern 0.0pt\raise 0.0pt\hbox{\hbox{\kern 3.0pt\raise-2.55554pt\hbox{$\textstyle{0}$}}}}}}}\ignorespaces}}}}\ignorespaces.
Proof.

This is the first proposition in [Ful93, §3.4]. ∎

Remark 4.28.

In the previous theorem, the hypothesis that Σ\Sigma is not contained in any hyperplane is only needed for the injectivity of the second arrow in each row of the diagram.

In view of Theorem 4.22, the upper exact sequence of the diagram in Theorem 4.27 can be interpreted as follows.

Corollary 4.29.

Let XX be a toric variety with torus 𝕋\mathbb{T}.

  1. (1)

    Every toric line bundle LL on XX admits a toric section. Moreover, if ss and s′s^{\prime} are two toric sections, then there exists m∈Mm\in M such that s′=χm​ss^{\prime}=\chi^{m}s.

  2. (2)

    If the fan Σ\Sigma that defines XX is not contained in any hyperplane, and LL and L′L^{\prime} are toric line bundles on XX, then there is at most one isomorphism between them.

Proof.

This follows from theorems 4.27 and 4.22. ∎

We next study the intersection of a 𝕋\mathbb{T}-Cartier divisor with the closure of an orbit. Let Σ\Sigma be a fan in NℝN_{\mathbb{R}} and Ψ\Psi the virtual support function on Σ\Sigma given by the set of defining vectors {mτ}τ∈Σ\{m_{\tau}\}_{\tau\in\Sigma}. Let σ\sigma be a cone of Σ\Sigma and ισ:V⁡(σ)↪XΣ\iota_{\sigma}\colon V(\sigma)\hookrightarrow X_{\Sigma} the associated closed immersion. We consider first the case when Ψ|σ=0\Psi|_{\sigma}=0. Let τ⊃σ\tau\supset\sigma be another cone of Σ\Sigma. For vectors u∈τu\in\tau and v∈ℝ​σv\in\mathbb{R}\sigma such that u+v∈τu+v\in\tau, the condition Ψ|σ=0\Psi|_{\sigma}=0 implies

Ψ⁡(u+v)=⟨mτ,u+v⟩=⟨mτ,u⟩=Ψ⁡(u)\Psi(u+v)=\langle m_{\tau},u+v\rangle=\langle m_{\tau},u\rangle=\Psi(u)

because mτ|ℝ​σ=0m_{\tau}\big|_{\mathbb{R}\sigma}=0. Hence, we can define a function

(4.30) Ψ⁡(σ):N​(σ)ℝ⟶ℝ,u+ℝ​σ⟼Ψ⁡(u+v)\Psi(\sigma)\colon N(\sigma)_{\mathbb{R}}\longrightarrow\mathbb{R},\quad u+\mathbb{R}\sigma\longmapsto\Psi(u+v)

for any v∈ℝ​σv\in\mathbb{R}\sigma such that u+v∈⋃τ⊃στu+v\in\bigcup_{\tau\supset\sigma}\tau.

It is easy to produce a set of defining vectors of Ψ⁡(σ)\Psi(\sigma). For each cone τ⊃σ\tau\supset\sigma we denote by τ¯=πσ​(τ){\overline{\tau}}=\pi_{\sigma}(\tau) the corresponding cone in Σ⁡(σ)\Sigma(\sigma). Since mτ|ℝ​σ=0m_{\tau}\big|_{\mathbb{R}\sigma}=0, then mτ∈M⁡(σ)=M∩σ⟂m_{\tau}\in M(\sigma)=M\cap\sigma^{\perp}. We set mτ¯=mτ∈M⁡(σ)m_{{\overline{\tau}}}=m_{\tau}\in M(\sigma).

Proposition 4.31.

Let notation be as above. If Ψ|σ=0\Psi|_{\sigma}=0, then DΨD_{\Psi} intersects V⁡(σ)V(\sigma) properly and ισ∗​DΨ=DΨ⁡(σ)\iota_{\sigma}^{\ast}D_{\Psi}=D_{\Psi(\sigma)}. Moreover, {mτ¯}τ¯∈Σ⁡(σ)\{m_{{\overline{\tau}}}\}_{{\overline{\tau}}\in\Sigma(\sigma)} is a set of defining vectors of Ψ⁡(σ)\Psi(\sigma).

Proof.

The 𝕋\mathbb{T}-Cartier divisor DΨD_{\Psi} is given by {(Xτ,χ−mτ)}τ∈Σ\{(X_{\tau},\chi^{-m_{\tau}})\}_{\tau\in\Sigma}. If mσ=0m_{\sigma}=0, the local equation of DΨD_{\Psi} in XσX_{\sigma} is χ0=1\chi^{0}=1. Therefore, the orbit O⁡(σ)O(\sigma) does not meet the support of DΨD_{\Psi}. Hence V⁡(σ)V(\sigma) and DΨD_{\Psi} intersect properly.

To see that {mτ¯}τ¯∈Σ⁡(σ)\{m_{{\overline{\tau}}}\}_{{\overline{\tau}}\in\Sigma(\sigma)} is a set of defining vectors, we pick a point u¯∈τ¯{\overline{u}}\in{\overline{\tau}} and we choose u∈τu\in\tau such that πσ​(u)=u¯\pi_{\sigma}(u)={\overline{u}}. Then

Ψ⁡(σ)​(u¯)=Ψ⁡(u)=mτ​(u)=mτ¯​(u¯),\Psi(\sigma)({\overline{u}})=\Psi(u)=m_{\tau}(u)=m_{{\overline{\tau}}}({\overline{u}}),

which proves the claim. Now, using the characterization of Ψ⁡(σ)\Psi(\sigma) in terms of defining vectors, we have

ισ∗​DΨ={(Xτ∩V⁡(σ),χ−mτ∣Xτ∩V⁡(σ))}τ¯={(Xτ¯,χ−mτ¯)}τ¯=DΨ⁡(σ).\iota_{\sigma}^{\ast}D_{\Psi}=\{(X_{\tau}\cap V(\sigma),\chi^{-m_{\tau}}\mid_{X_{\tau}\cap V(\sigma)})\}_{{\overline{\tau}}}=\{(X_{{\overline{\tau}}},\chi^{-m_{{\overline{\tau}}}})\}_{{\overline{\tau}}}=D_{\Psi(\sigma)}.

∎

When Ψ|σ≠0\Psi|_{\sigma}\not=0, the cycles DΨD_{\Psi} and V⁡(σ)V(\sigma) do not intersect properly, and we can only intersect DΨD_{\Psi} with V⁡(σ)V(\sigma) up to rational equivalence. To this end, we choose any mσ′m_{\sigma}^{\prime} such that Ψ⁡(u)=⟨mσ′,u⟩\Psi(u)=\langle m^{\prime}_{\sigma},u\rangle for every u∈σu\in\sigma. Then the divisor DΨ−mσ′D_{\Psi-m_{\sigma}^{\prime}} is rationally equivalent to DΨD_{\Psi} and Ψ−mσ′|σ=0\Psi-m_{\sigma}^{\prime}|_{\sigma}=0. By the above result, this divisor intersects V⁡(σ)V(\sigma) properly, and its restriction to V⁡(τ)V(\tau) is given by the virtual support function (Ψ−mσ′)​(σ)(\Psi-m_{\sigma}^{\prime})(\sigma).

Example 4.32.

We can use the above description of the restriction of a line bundle to an orbit to compute the degree of an orbit of dimension one. Let Σ\Sigma be a complete fan and τ∈Σn−1\tau\in\Sigma^{n-1}. Hence V⁡(τ)V(\tau) is a toric curve. Let σ1\sigma_{1} and σ2\sigma_{2} be the two nn-dimensional cones that have τ\tau as a common face. Let Ψ\Psi be a virtual support function. Choose v∈σ1v\in\sigma_{1} such that πτ​(v)\pi_{\tau}(v) is a generator of the lattice N⁡(τ)N(\tau). Then, by (4.25) and (4.30),

(4.33) degDΨ⁡(V⁡(τ))=deg⁡(ιτ∗​DΨ)=mσ2​(v)−mσ1​(v).\deg_{D_{\Psi}}(V(\tau))=\deg(\iota_{\tau}^{*}D_{\Psi})=m_{\sigma_{2}}(v)-m_{\sigma_{1}}(v).

Let now (L,z)(L,z) be a toric line bundle on XΣX_{\Sigma} and σ∈Σ\sigma\in\Sigma. The line bundle ισ∗​L\iota^{\ast}_{\sigma}L on V⁡(σ)V(\sigma) has an induced toric structure. Let ss be a toric section of LL that is regular and nowhere vanishing on XσX_{\sigma}, and set zσ=s⁡(xσ)∈Lxσ∖{0}z_{\sigma}=s(x_{\sigma})\in L_{x_{\sigma}}\setminus\{0\}. If s′s^{\prime} is another such section, then s′=χm​ss^{\prime}=\chi^{m}s for an m∈Mm\in M such that m|σ=0m|_{\sigma}=0, by Corollary 4.29. Therefore s′​(xσ)=s⁡(xσ)s^{\prime}(x_{\sigma})=s(x_{\sigma}). Hence, zσz_{\sigma} does not depend on the choice of section and (ισ∗​L,zσ)(\iota^{\ast}_{\sigma}L,z_{\sigma}) is the induced toric line bundle. The following result follows easily from the constructions.

Proposition 4.34.

Let (L,z)(L,z) be a toric line bundle on XΣX_{\Sigma} and σ∈Σ\sigma\in\Sigma. Let Ψ\Psi be a virtual support function such that Ψ|σ=0\Psi|_{\sigma}=0 and (L,z)≃(LΨ,zΨ)(L,z)\simeq(L_{\Psi},z_{\Psi}) as toric line bundles. Then ισ∗​(L,z)≃(LΨ⁡(σ),zΨ⁡(σ))\iota^{\ast}_{\sigma}(L,z)\simeq(L_{\Psi(\sigma)},z_{\Psi(\sigma)}).

We next study the inverse image of a 𝕋\mathbb{T}-Cartier divisor with respect to equivariant morphisms as those in Theorem 4.9. Let NiN_{i}, Σi\Sigma_{i}, i=1,2i=1,2, and let H:N1→N2H\colon N_{1}\to N_{2} and p∈XΣ2,0​(K)p\in X_{\Sigma_{2},0}(K) be as in Theorem 4.9. Let φp,H\varphi_{p,H} be the associated equivariant morphism, Ψ\Psi a virtual support function on Σ2\Sigma_{2} and {mτ′′}τ′∈Σ2\{m^{\prime}_{\tau^{\prime}}\}_{\tau^{\prime}\in\Sigma_{2}} a set of defining vectors of Ψ\Psi. For each cone τ∈Σ1\tau\in\Sigma_{1} we choose a cone τ′∈Σ2\tau^{\prime}\in\Sigma_{2} such that H⁡(τ)⊂τ′H(\tau)\subset\tau^{\prime} and we write mτ=H∨​(mτ′′)m_{\tau}=H^{\vee}(m^{\prime}_{\tau^{\prime}}). The following result follows easily from the definitions

Proposition 4.35.

The divisor DΨD_{\Psi} intersects properly the image of φp,H\varphi_{p,H}. The function Ψ∘H\Psi\circ H is a virtual support function on Σ1\Sigma_{1} and

φp,H∗​DΨ=DΨ∘H.\varphi^{\ast}_{p,H}D_{\Psi}=D_{\Psi\circ H}.

Moreover, {mτ}τ∈Σ1\{m_{\tau}\}_{\tau\in\Sigma_{1}} is a set of defining vectors of Ψ∘H\Psi\circ H.

Remark 4.36.

If LL is a toric line bundle on XΣ2X_{\Sigma_{2}} and φ\varphi is a toric morphism, then φ∗​L\varphi^{\ast}L has an induced toric structure. Namely, φ∗​(L,z)=(φ∗​L,φ∗​z)\varphi^{\ast}(L,z)=(\varphi^{\ast}L,\varphi^{\ast}z). By contrast, if φ:XΣ1→XΣ2\varphi\colon X_{\Sigma_{1}}\to X_{\Sigma_{2}} is a general equivariant morphism that meets the principal open subset, there is no natural toric structure on φ∗​L\varphi^{\ast}L, because the image of the distinguished point x1,0x_{1,0} does not need to agree with x2,0x_{2,0}. If (L,s)(L,s) is a toric line bundle equipped with a toric section, then we set φ∗​(L,s)=((φ∗​L,(φ∗​s)​(x1,0)),φ∗​s)\varphi^{\ast}(L,s)=((\varphi^{\ast}L,(\varphi^{\ast}s)(x_{1,0})),\varphi^{\ast}s). However, the underlying toric bundle of φ∗​(L,s)\varphi^{\ast}(L,s) depends on the choice of the toric section.

4.4. Positivity properties of 𝕋\mathbb{T}-Cartier divisors

Let Σ\Sigma be a fan in NℝN_{\mathbb{R}} and Ψ\Psi a virtual support function on Σ\Sigma. In this section, we will assume that Σ\Sigma is complete or, equivalently, that the variety XΣX_{\Sigma} is proper.

Many geometric properties of the pair (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) can be read directly from Ψ\Psi. For instance, 𝒪⁡(DΨ)\mathcal{O}(D_{\Psi}) is generated by global sections if and only if the function Ψ\Psi is concave, and the line bundle 𝒪⁡(DΨ){\mathcal{O}}(D_{\Psi}) is ample if and only if Ψ\Psi is strictly concave on Σ\Sigma. In the latter case, the fan Σ\Sigma agrees with the polyhedral complex Π⁡(Ψ)\Pi(\Psi) (Definition 3.34) and the pair (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) is completely determined by Ψ\Psi. Thus, the variety XΣX_{\Sigma} is projective if and only if the fan Σ\Sigma is complete and regular (Definition 3.60).

We associate to Ψ\Psi the subset of MℝM_{\mathbb{R}}

ΔΨ={x∈Mℝ∣⟨x,u⟩≥Ψ(u) for all u∈Nℝ}.\Delta_{\Psi}=\{x\in M_{\mathbb{R}}\mid\langle x,u\rangle\geq\Psi(u)\mbox{ for all }u\in N_{\mathbb{R}}\}.

This set is either empty or a lattice polytope. When 𝒪⁡(DΨ){\mathcal{O}}(D_{\Psi}) is generated by global sections, the polytope ΔΨ\Delta_{\Psi} agrees with stab⁡(Ψ)\operatorname{stab}(\Psi), and Ψ\Psi is the support function of ΔΨ\Delta_{\Psi}.

The polytope ΔΨ\Delta_{\Psi} encodes a lot of information about the pair (XΣ,DΨ)(X_{\Sigma},D_{\Psi}). For instance, we can read from it the space of global sections of 𝒪⁡(DΨ)\mathcal{O}(D_{\Psi}). A monomial rational section χm∈𝒦XΣ\chi^{m}\in\mathcal{K}_{X_{\Sigma}}, m∈Mm\in M, is a regular global section of 𝒪⁡(DΨ)\mathcal{O}(D_{\Psi}) if and only if m∈ΔΨm\in\Delta_{\Psi}. Moreover, the set {χm}m∈M∩ΔΨ\{\chi^{m}\}_{m\in M\cap\Delta_{\Psi}} is a KK-basis of the space of global sections Γ⁡(XΣ,𝒪⁡(DΨ))\Gamma(X_{\Sigma},\mathcal{O}(D_{\Psi})). In the sequel we will see many more examples of this principle.

Proposition 4.37.

Let DΨiD_{\Psi_{i}}, i=1,…,ni=1,\dots,n, be 𝕋\mathbb{T}-Cartier divisors on XΣX_{\Sigma} generated by their global sections. Then

(4.38) (DΨ1⋅⋯⋅DΨn)=MVM⁡(ΔΨ1,…,ΔΨn).(D_{\Psi_{1}}\cdot\dots\cdot D_{\Psi_{n}})=\operatorname{MV}_{M}(\Delta_{\Psi_{1}},\dots,\Delta_{\Psi_{n}}).

where MVM\operatorname{MV}_{M} denotes the mixed volume function associated to the Haar measure volM\operatorname{vol}_{M} on MℝM_{\mathbb{R}} (Definition 3.109). In particular, for a 𝕋\mathbb{T}-Cartier divisor DΨD_{\Psi} generated by its global sections,

(4.39) degDΨ⁡(XΣ)=(DΨn)=n!​volM⁡(ΔΨ).\deg_{D_{\Psi}}(X_{\Sigma})=(D_{\Psi}^{n})=n!\operatorname{vol}_{M}(\Delta_{\Psi}).
Proof.

This follows from [Oda88, Proposition 2.10]. ∎

Remark 4.40.

The intersection multiplicity and the degree in the above Proposition only depend on the isomorphism class of the line bundles 𝒪⁡(DΨi){\mathcal{O}}(D_{\Psi_{i}}) and not on the 𝕋\mathbb{T}-Cartier divisors themselves. It is easy to check directly that the right-hand sides of (4.38) and (4.39) only depends on the isomorphism class of the line bundles. In fact, let LL be a toric line bundle generated by global sections and s1s_{1}, s2s_{2} two toric sections. For i=1,2i=1,2, set Di=div⁡(si)D_{i}=\operatorname{div}(s_{i}) and let Ψi\Psi_{i} be the corresponding support function and Δi\Delta_{i} the associated polytope. Then s2=χm​s1s_{2}=\chi^{m}s_{1} for some m∈Mm\in M. Thus Ψ2=Ψ1−m\Psi_{2}=\Psi_{1}-m and Δ2=Δ1−m\Delta_{2}=\Delta_{1}-m. Since the volume and the mixed volume are invariant under translation, we see that these formulae do not depend on the choice of sections.

Definition 4.41.

A polarized toric variety is a pair (XΣ,DΨ)(X_{\Sigma},D_{\Psi}), where XΣX_{\Sigma} is a toric variety and DΨD_{\Psi} is an ample 𝕋\mathbb{T}-Cartier divisor.

Polarized toric varieties can be classified in terms of their polytopes.

Theorem 4.42.

The correspondence (XΣ,DΨ)↦ΔΨ(X_{\Sigma},D_{\Psi})\mapsto\Delta_{\Psi} is a bijection between the set of polarized toric varieties and the set of lattice polytopes of dimension nn of MM. Two ample 𝕋\mathbb{T}-Cartier divisors DΨD_{\Psi} and DΨ′D_{\Psi^{\prime}} on a toric variety XΣX_{\Sigma} are rationally equivalent if and only if ΔΨ′\Delta_{\Psi^{\prime}} is the translated of ΔΨ\Delta_{\Psi} by an element of MM.

Proof.

If Ψ\Psi is a strictly concave function on Σ\Sigma, then ΔΨ\Delta_{\Psi} is an nn-dimensional lattice polytope. Conversely, if Δ\Delta is a lattice polytope in MℝM_{\mathbb{R}}, then ΨΔ\Psi_{\Delta}, the support function of Δ\Delta, is a strictly concave function on the complete fan ΣΔ=Π⁡(ΨΔ)\Sigma_{\Delta}=\Pi(\Psi_{\Delta}) (see examples 3.71 and 3.76). Therefore, the result follows from Theorem 4.18 and the construction of Remark 4.40. ∎

Remark 4.43.

When DΨD_{\Psi} is only generated by its global sections, the polytope ΔΨ\Delta_{\Psi} may not determine the variety XΣX_{\Sigma}, but it does determine a polarized toric variety that is the image of XΣX_{\Sigma} by a toric morphism. Write Δ=ΔΨ\Delta=\Delta_{\Psi} for short. Let M⁡(Δ)M(\Delta) be as in Notation 3.103 and choose m∈aff⁡(Δ)∩Mm\in\operatorname{aff}(\Delta)\cap M. Set N⁡(Δ)=M​(Δ)∨N(\Delta)=M(\Delta)^{\vee}. The translated polytope Δ−m\Delta-m has the same dimension as its ambient space LΔ=M​(Δ)ℝL_{\Delta}=M(\Delta)_{\mathbb{R}}. By the theorem above, it defines a complete fan ΣΔ\Sigma_{\Delta} in N​(Δ)ℝN(\Delta)_{\mathbb{R}} together with a support function ΨΔ:N⁡(Δ)→ℝ\Psi_{\Delta}\colon N(\Delta)\to\mathbb{R}. The projection N→N⁡(Δ)N\to N(\Delta) induces a toric morphism

φ:XΣ⟶XΣΔ,\varphi\colon X_{\Sigma}\longrightarrow X_{\Sigma_{\Delta}},

the divisor DΨΔD_{\Psi_{\Delta}} is ample, and DΨ=φ∗​DΨΔ+div⁡(χ−m)D_{\Psi}=\varphi^{*}D_{\Psi_{\Delta}}+\operatorname{div}(\chi^{-m}).

Example 4.44.

The projective morphisms associated to 𝕋\mathbb{T}-Cartier divisors generated by global sections can also be made explicit in terms of the lattice points of the associated polytope. Consider a complete toric variety XΣX_{\Sigma} of dimension nn equipped with a 𝕋\mathbb{T}-Cartier divisor DΨD_{\Psi} generated by global sections. Let m0,…,mr∈ΔΨ∩Mm_{0},\dots,m_{r}\in\Delta_{\Psi}\cap M be such that conv⁡(m0,…,mr)=ΔΨ\operatorname{conv}(m_{0},\dots,m_{r})=\Delta_{\Psi}. These vectors determine an H-representation Ψ=mini=0,…,r⁡mi\Psi=\min_{i=0,\dots,r}m_{i}. Let H:Nℝ→ℝrH\colon N_{\mathbb{R}}\to\mathbb{R}^{r} be the linear map defined by H⁡(u)=(mi​(u)−m0​(u))i=1,…,rH(u)=(m_{i}(u)-m_{0}(u))_{i=1,\dots,r}. By Lemma 3.79, Ψ=H∗​ΨΔr+m0\Psi=H^{\ast}\Psi_{\Delta^{r}}+m_{0}.

In ℝr\mathbb{R}^{r} we consider the fan ΣΔr\Sigma_{\Delta^{r}}, whose associated toric variety is ℙr\mathbb{P}^{r}. One easily verifies that, for each σ∈Σ\sigma\in\Sigma, there is σ′∈ΣΔr\sigma^{\prime}\in\Sigma_{\Delta^{r}} with H⁡(σ)⊂σ′H(\sigma)\subset\sigma^{\prime}. Let p=(p0:…:pr)p=(p_{0}:\dots:p_{r}) be an arbitrary rational point of the principal open subset of ℙr\mathbb{P}^{r}. The equivariant morphism φp,H:X→ℙKr\varphi_{p,H}\colon X\to\mathbb{P}^{r}_{K} can be written explicitly as (p0χm0:…:prχmr)(p_{0}\chi^{m_{0}}:\dots:p_{r}\chi^{m_{r}}). Moreover, DΨ=φp,H∗​DΨΔr+div⁡(χ−m0)D_{\Psi}=\varphi_{p,H}^{\ast}D_{\Psi_{\Delta^{r}}}+\operatorname{div}(\chi^{-m_{0}}).

The orbits of a polarized toric variety (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) are in one-to-one correspondence with the faces of ΔΨ\Delta_{\Psi}.

Proposition 4.45.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and Ψ\Psi a strictly concave function on Σ\Sigma. The correspondence F↦O⁡(σF)F\mapsto O(\sigma_{F}) is a bijection between the set of faces of ΔΨ\Delta_{\Psi} and the set of the orbits under the action of 𝕋\mathbb{T} on XΣX_{\Sigma}.

Proof.

This follows from Example 3.71. ∎

Equation (4.25) gives a formula for the Weil divisor [DΨ][D_{\Psi}] in terms of the virtual support function Ψ\Psi. When the line bundle 𝒪⁡(DΨ)\mathcal{O}(D_{\Psi}) is ample, we can interpret this formula in terms of the facets of the polytope ΔΨ\Delta_{\Psi}.

Let DΨD_{\Psi} be an ample line bundle on XΣX_{\Sigma}. The polytope ΔΨ\Delta_{\Psi} has maximal dimension nn. For each facet FF of ΔΨ\Delta_{\Psi}, let vFv_{F} be as in Notation 3.103. The ray τF=ℝ≥0​vF\tau_{F}=\mathbb{R}_{\geq 0}v_{F} is a cone of Σ\Sigma.

Proposition 4.46.

With the previous hypothesis,

div(sΨ)=[DΨ]=∑F−⟨vF,F⟩V(τF),\operatorname{div}(s_{\Psi})=[D_{\Psi}]=\sum_{F}-\langle v_{F},F\rangle V(\tau_{F}),

where the sum is over the facets FF of Δ\Delta.

Proof.

Since Ψ\Psi is strictly concave on Σ\Sigma, the Legendre-Fenchel correspondence shows that the set of rays of the form τF\tau_{F} agrees with the set Σ1\Sigma^{1}. Moreover, Ψ⁡(vF)=⟨vF,F⟩\Psi(v_{F})=\langle v_{F},F\rangle, because Ψ\Psi is the support function of Δ\Delta. The proposition then follows from (4.25). ∎

For a 𝕋\mathbb{T}-Cartier divisor generated by global sections, we can interpret its intersection with the closure of an orbit, and its inverse image with respect to an equivariant morphism, in terms of direct and inverse images of concave functions.

Proposition 4.47.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and Ψ:Nℝ→ℝ\Psi\colon N_{\mathbb{R}}\to\mathbb{R} a support function on Σ\Sigma.

  1. (1)

    Let σ∈Σ\sigma\in\Sigma, FσF_{\sigma} the associated face of ΔΨ\Delta_{\Psi}, and mσ′∈Fσ∩Mm_{\sigma}^{\prime}\in F_{\sigma}\cap M. Let πσ:Nℝ→N​(σ)ℝ\pi_{\sigma}\colon N_{\mathbb{R}}\to N(\sigma)_{\mathbb{R}} be the natural projection. Then

    (4.48) (Ψ−mσ′)​(σ)=(πσ)∗​(Ψ−mσ′).(\Psi-m^{\prime}_{\sigma})(\sigma)=(\pi_{\sigma})_{\ast}(\Psi-m_{\sigma}^{\prime}).

    In particular, the restriction of DΨ−mσ′D_{\Psi-m^{\prime}_{\sigma}} to V⁡(σ)V(\sigma) is given by the concave function (πσ)∗​(Ψ−mσ′)(\pi_{\sigma})_{\ast}(\Psi-m_{\sigma}^{\prime}). Moreover, the associated polytope is

    (4.49) Δ(Ψ−mσ′)​(σ)=Fσ−mσ′⊂M​(σ)ℝ=σ⊥.\Delta_{(\Psi-m_{\sigma}^{\prime})(\sigma)}=F_{\sigma}-m_{\sigma}^{\prime}\subset M(\sigma)_{\mathbb{R}}=\sigma^{\bot}.
  2. (2)

    Let H:N′→NH\colon N^{\prime}\to N be a linear map and H∨:M→M′H^{\vee}\colon M\to M^{\prime} its dual map, where M′=(N′)∨M^{\prime}=(N^{\prime})^{\vee}. Let Σ′\Sigma^{\prime} be a fan in Nℝ′N^{\prime}_{\mathbb{R}} such that, for each σ′∈Σ′\sigma^{\prime}\in\Sigma^{\prime} there is σ∈Σ\sigma\in\Sigma with H⁡(σ′)⊂σH(\sigma^{\prime})\subset\sigma, and let p∈XΣ,0​(K)p\in X_{\Sigma,0}(K). Then

    (4.50) φp,H∗​DΨ=DH∗​Ψ,\varphi_{p,H}^{\ast}D_{\Psi}=D_{H^{\ast}\Psi},

    and the associated polytope is

    (4.51) ΔH∗​Ψ=H∨​(ΔΨ)⊂Mℝ′.\Delta_{H^{\ast}\Psi}=H^{\vee}(\Delta_{\Psi})\subset M^{\prime}_{\mathbb{R}}.
Proof.

Equation (4.48) follows from (4.30), while equation (4.50) follows from Proposition 4.35. Then (4.49) and (4.51) follow from Proposition 3.78. ∎

As a consequence of the above construction, we can compute easily the degree of any orbit.

Corollary 4.52.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}}, Ψ:Nℝ→ℝ\Psi\colon N_{\mathbb{R}}\to\mathbb{R} a support function on Σ\Sigma, and σ∈Σ\sigma\in\Sigma a cone of dimension n−kn-k. Then

degDΨ⁡(V⁡(σ))=k!​volM⁡(Fσ)⁡(Fσ).\deg_{D_{\Psi}}(V(\sigma))=k!\operatorname{vol}_{M(F_{\sigma})}(F_{\sigma}).
Proof.

In view of equations (4.49) and (4.39), it is enough to prove that M⁡(σ)=M⁡(Fσ)M(\sigma)=M(F_{\sigma}). But this follows from the fact that LFσ=σ⟂L_{F_{\sigma}}=\sigma^{\perp} (see Notation 3.103). ∎

Example 4.53.

Let τ∈Σn−1\tau\in\Sigma^{n-1}. The degree of the curve V⁡(τ)V(\tau) agrees with the lattice length of FτF_{\tau}.

We will also need the toric version of the Nakai-Moishezon criterion.

Theorem 4.54.

Let XΣX_{\Sigma} be a proper toric variety and DΨD_{\Psi} a 𝕋\mathbb{T}-Cartier divisor on XΣX_{\Sigma}.

  1. (1)

    The following properties are equivalent:

    1. (a)

      DΨD_{\Psi} is ample;

    2. (b)

      (DΨ⋅C)>0(D_{\Psi}\cdot C)>0 for every curve CC in XΣX_{\Sigma};

    3. (c)

      (DΨ⋅V⁡(τ))>0(D_{\Psi}\cdot V(\tau))>0 for every τ∈Σn−1\tau\in\Sigma^{n-1}.

  2. (2)

    The following properties are equivalent:

    1. (a)

      DΨD_{\Psi} is generated by its global sections;

    2. (b)

      (DΨ⋅C)≥0(D_{\Psi}\cdot C)\geq 0 for every curve CC in XΣX_{\Sigma};

    3. (c)

      (DΨ⋅V⁡(τ))≥0(D_{\Psi}\cdot V(\tau))\geq 0 for every τ∈Σn−1\tau\in\Sigma^{n-1}.

Proof.

This follows from [Oda88, Theorem 2.18] for non singular toric varieties, and from [Mav00] for the general case. ∎

4.5. Toric schemes over a discrete valuation ring

In this section we recall some basic facts about the algebraic geometry of toric schemes over a DVR. These toric schemes were introduced in [KKMS73, Chapter IV, §3], and we refer to this reference for more details. They are described and classified in terms of fans in Nℝ×ℝ≥0N_{\mathbb{R}}\times\mathbb{R}_{\geq 0}. In this section we will mostly consider proper toric schemes over a DVR. As a consequence of Corollary 3.15, proper toric schemes over a DVR can be described and classified in terms of complete SCR polyhedral complexes in NℝN_{\mathbb{R}} as, for instance, in [NS06].

Let KK be a field equipped with a nontrivial discrete valuation val:K×↠ℤ{\operatorname{val}}\colon K^{\times}\twoheadrightarrow\mathbb{Z}. In this section we do not assume KK to be complete. As usual, we denote by K∘K^{\circ} the valuation ring, by K∘⁣∘K^{\circ\circ} its maximal ideal, by ϖ\varpi a generator of K∘⁣∘K^{\circ\circ} and by kk the residue field. We assume that val⁡(ϖ)=1{\operatorname{val}}(\varpi)=1. We denote by SS the base scheme S=Spec⁡(K∘)S=\operatorname{Spec}(K^{\circ}), by η\eta and oo the generic and the special points of SS and, for a scheme 𝒳\mathcal{X} over SS, we set 𝒳η=𝒳×SSpec⁡(K)\mathcal{X}_{\eta}=\mathcal{X}\times_{S}\operatorname{Spec}(K) and 𝒳o=𝒳×SSpec⁡(k)\mathcal{X}_{o}=\mathcal{X}\times_{S}\operatorname{Spec}(k) for its generic and special fibre respectively. We will denote by 𝕋S=𝕋K0≃𝔾m,Sn\mathbb{T}_{S}=\mathbb{T}_{K^{0}}\simeq\mathbb{G}_{m,S}^{n} a split torus over SS. Let 𝕋=𝕋K\mathbb{T}=\mathbb{T}_{K}, NN and MM be as in §4.1. We will write N~=N⊕ℤ{\widetilde{N}}=N\oplus\mathbb{Z} and M~=M⊕ℤ{\widetilde{M}}=M\oplus\mathbb{Z}.

Definition 4.55.

A toric scheme over SS of relative dimension nn is a normal integral separated SS-scheme of finite type, 𝒳{\mathcal{X}}, equipped with a dense open embedding 𝕋K↪𝒳η\mathbb{T}_{K}\hookrightarrow{\mathcal{X}}_{\eta} and an SS-action of 𝕋S\mathbb{T}_{S} over 𝒳{\mathcal{X}} that extends the action of 𝕋K\mathbb{T}_{K} on itself by translations. If we want to stress the torus acting on 𝒳{\mathcal{X}} we will call them toric schemes with torus 𝕋S\mathbb{T}_{S}.

If 𝒳{\mathcal{X}} is a toric scheme over SS, then 𝒳η{\mathcal{X}}_{\eta} is a toric variety over KK with torus 𝕋\mathbb{T}.

Definition 4.56.

Let XX be a toric variety over KK with torus 𝕋K\mathbb{T}_{K} and let 𝒳{\mathcal{X}} be a toric scheme over SS with torus 𝕋S\mathbb{T}_{S}. We say that 𝒳{\mathcal{X}} is a toric model of XX over SS if the identity of 𝕋K\mathbb{T}_{K} can be extended to an isomorphism from XX to 𝒳η{\mathcal{X}}_{\eta}.

If 𝒳{\mathcal{X}} and 𝒳′{\mathcal{X}}^{\prime} are toric models of XX and α:𝒳→𝒳′\alpha\colon{\mathcal{X}}\to{\mathcal{X}}^{\prime} is an SS-morphism, we say that α\alpha is a morphism of toric models if its restriction to 𝕋K\mathbb{T}_{K} is the identity.

Since, by definition, a toric scheme is integral and contains 𝕋\mathbb{T} as a dense open subset, it is flat over SS. Thus a toric model is a particular case of a model as in Definition 2.11.

Let Σ~{\widetilde{\Sigma}} be a fan in Nℝ×ℝ≥0N_{\mathbb{R}}\times\mathbb{R}_{\geq 0}. To the fan Σ~\widetilde{\Sigma} we associate a toric scheme 𝒳Σ~{\mathcal{X}}_{\widetilde{\Sigma}} over SS. Let σ∈Σ~\sigma\in{\widetilde{\Sigma}} be a cone and σ∨⊂M~ℝ\sigma^{\vee}\subset{\widetilde{M}}_{\mathbb{R}} its dual cone. Set M~σ=M~∩σ∨{\widetilde{M}}_{\sigma}={\widetilde{M}}\cap\sigma^{\vee}. Let K∘​[M~σ]K^{\circ}[{\widetilde{M}}_{\sigma}] be the semigroup K∘K^{\circ}-algebra of M~σ{\widetilde{M}}_{\sigma}. By definition, (0,1)∈M~σ(0,1)\in{\widetilde{M}}_{\sigma}. Thus (χ(0,1)−ϖ)(\chi^{(0,1)}-\varpi) is an ideal of K∘​[M~σ]K^{\circ}[{\widetilde{M}}_{\sigma}]. There is a natural isomorphism

(4.57) K∘[M~σ]/(χ(0,1)−ϖ)≃{∑(m,l)∈M~σαm,lϖlχm∣αm,l∈K∘ and, ∀∘(m,l),αm,l=0}K^{\circ}[{\widetilde{M}}_{\sigma}]/(\chi^{(0,1)}-\varpi)\simeq\Big\{\sum_{(m,l)\in{\widetilde{M}}_{\sigma}}\alpha_{m,l}\varpi^{l}\chi^{m}\mid\alpha_{m,l}\in K^{\circ}\text{ and, }\overset{\circ}{\forall}(m,l),\alpha_{m,l}=0\Big\}

that we use to identify both rings. The ring K∘​[M~σ]/(χ(0,1)−ϖ)K^{\circ}[{\widetilde{M}}_{\sigma}]/(\chi^{(0,1)}-\varpi) is an integrally closed domain. We set

𝒳σ=Spec⁡(K∘​[M~σ]/(χ(0,1)−ϖ)){\mathcal{X}}_{\sigma}=\operatorname{Spec}(K^{\circ}[{\widetilde{M}}_{\sigma}]/(\chi^{(0,1)}-\varpi))

for the associated affine toric scheme over SS. For short we will use the notation

(4.58) K∘​[𝒳σ]=K∘​[M~σ]/(χ(0,1)−ϖ).K^{\circ}[{\mathcal{X}}_{\sigma}]=K^{\circ}[{\widetilde{M}}_{\sigma}]/(\chi^{(0,1)}-\varpi).

For cones σ,σ′∈Σ~\sigma,\sigma^{\prime}\in{\widetilde{\Sigma}}, with σ⊂σ′\sigma\subset\sigma^{\prime} we have a natural open immersion of affine schemes 𝒳σ↪𝒳σ′{\mathcal{X}}_{\sigma}\hookrightarrow{\mathcal{X}}_{\sigma^{\prime}}. Using these open immersions as gluing data, we define the scheme

𝒳Σ~=⋃σ∈Σ~𝒳σ.{\mathcal{X}}_{\widetilde{\Sigma}}=\bigcup_{\sigma\in{\widetilde{\Sigma}}}{\mathcal{X}}_{\sigma}.

This is a reduced and irreducible normal scheme of finite type over SS of relative dimension nn.

There are two types of cones in Σ~{\widetilde{\Sigma}}. The ones that are contained in the hyperplane Nℝ×{0}N_{\mathbb{R}}\times\{0\}, and the ones that are not. If σ\sigma is contained in Nℝ×{0}N_{\mathbb{R}}\times\{0\}, then (0,−1)∈M~σ(0,-1)\in{\widetilde{M}}_{\sigma}, and ϖ\varpi is invertible in K∘​[𝒳σ]K^{\circ}[{\mathcal{X}}_{\sigma}]. Therefore K∘​[𝒳σ]≃K⁡[Mσ]K^{\circ}[{\mathcal{X}}_{\sigma}]\simeq K[M_{\sigma}]; hence 𝒳σ{\mathcal{X}}_{\sigma} is contained in the generic fibre and it agrees with the affine toric variety XσX_{\sigma}. If σ\sigma is not contained in Nℝ×{0}N_{\mathbb{R}}\times\{0\}, then 𝒳σ{\mathcal{X}}_{\sigma} is not contained in the generic fibre.

To stress the difference between both types of affine schemes we will follow the following notations. Let Π\Pi be the SCR polyhedral complex in NℝN_{\mathbb{R}} obtained by intersecting Σ~{\widetilde{\Sigma}} by the hyperplane Nℝ×{1}N_{\mathbb{R}}\times\{1\} as in Corollary 3.15, and Σ\Sigma the fan in NℝN_{\mathbb{R}} obtained by intersecting Σ~{\widetilde{\Sigma}} with Nℝ×{0}N_{\mathbb{R}}\times\{0\}. For Λ∈Π\Lambda\in\Pi, the cone c⁡(Λ)∈Σ~\operatorname{c}(\Lambda)\in\widetilde{\Sigma} is not contained in N×{0}N\times\{0\}. We will write M~Λ=M~c⁡(Λ){\widetilde{M}}_{\Lambda}={\widetilde{M}}_{\operatorname{c}(\Lambda)}, K∘​[M~Λ]=K∘​[M~c⁡(Λ)]K^{\circ}[{\widetilde{M}}_{\Lambda}]=K^{\circ}[{\widetilde{M}}_{\operatorname{c}(\Lambda)}], 𝒳Λ=𝒳c⁡(Λ){\mathcal{X}}_{\Lambda}={\mathcal{X}}_{\operatorname{c}(\Lambda)} and K∘​[𝒳Λ]=K∘​[𝒳c⁡(Λ)]K^{\circ}[{\mathcal{X}}_{\Lambda}]=K^{\circ}[{\mathcal{X}}_{\operatorname{c}(\Lambda)}].

Given polyhedrons Λ,Λ′∈Π\Lambda,\Lambda^{\prime}\in\Pi, with Λ⊂Λ′\Lambda\subset\Lambda^{\prime}, we have a natural open immersion of affine toric schemes 𝒳Λ↪𝒳Λ′{\mathcal{X}}_{\Lambda}\hookrightarrow{\mathcal{X}}_{\Lambda^{\prime}}. Moreover, if a cone σ∈Σ\sigma\in\Sigma is a face of a cone c⁡(Λ)\operatorname{c}(\Lambda) for some Λ∈Π\Lambda\in\Pi, then the affine toric variety XσX_{\sigma}, is also an open subscheme of 𝒳Λ{\mathcal{X}}_{\Lambda}. The open cover (4.58) can be written as

𝒳Σ~=⋃Λ∈Π𝒳Λ∪⋃σ∈ΣXσ.{\mathcal{X}}_{\widetilde{\Sigma}}=\bigcup_{\Lambda\in\Pi}{\mathcal{X}}_{\Lambda}\cup\bigcup_{\sigma\in\Sigma}X_{\sigma}.

We will reserve the notation 𝒳Λ{\mathcal{X}}_{\Lambda}, Λ∈Π\Lambda\in\Pi for the affine toric schemes that are not contained in the generic fibre and denote by XσX_{\sigma}, σ∈Σ\sigma\in\Sigma the affine toric schemes contained in the generic fibre, because they are toric varieties over KK.

The scheme 𝒳0{\mathcal{X}}_{0} corresponding to the polyhedron 0:={0}0:=\{0\} is a group SS-scheme which is canonically isomorphic to 𝕋S\mathbb{T}_{S}. The SS-action of 𝕋S\mathbb{T}_{S} over 𝒳Σ~{\mathcal{X}}_{\widetilde{\Sigma}} is constructed as in the case of varieties over a field. Moreover there are open immersions 𝕋K↪𝒳η↪𝒳Σ~\mathbb{T}_{K}\hookrightarrow{\mathcal{X}}_{\eta}\hookrightarrow{\mathcal{X}}_{\widetilde{\Sigma}} of schemes over SS and the action of 𝕋S\mathbb{T}_{S} on 𝒳Σ~{\mathcal{X}}_{\widetilde{\Sigma}} extends the action of 𝕋K\mathbb{T}_{K} on itself. Thus 𝒳Σ~{\mathcal{X}}_{\widetilde{\Sigma}} is a toric scheme over SS. Moreover, the fan Σ\Sigma defines a toric variety over KK which coincides with the generic fibre 𝒳Σ~,η{\mathcal{X}}_{\widetilde{\Sigma},\eta}. Thus, 𝒳Σ~{\mathcal{X}}_{\widetilde{\Sigma}} is a toric model of XΣX_{\Sigma}. The special fibre 𝒳Σ~,o=𝒳Σ~​×𝑆​Spec⁡(k){\mathcal{X}}_{\widetilde{\Sigma},o}={\mathcal{X}}_{\widetilde{\Sigma}}\underset{S}{\times}\operatorname{Spec}(k) has an induced action by 𝕋k\mathbb{T}_{k}, but, in general, it is not a toric variety over kk, because it is not irreducible nor reduced. The reduced schemes associated to its irreducible components are toric varieties over kk with this action.

Every toric scheme over SS can be obtained by the above construction. Indeed, this construction gives a classification of toric schemes by fans in Nℝ×ℝ≥0N_{\mathbb{R}}\times\mathbb{R}_{\geq 0} [KKMS73, §IV.3(e)].

If the fan Σ~{\widetilde{\Sigma}} is complete, then the scheme 𝒳Σ~{\mathcal{X}}_{{\widetilde{\Sigma}}} is proper over SS. In this case the set {𝒳Λ}Λ∈Π\{{\mathcal{X}}_{\Lambda}\}_{\Lambda\in\Pi} is an open cover of 𝒳Σ~{\mathcal{X}}_{{\widetilde{\Sigma}}}. Proper toric schemes over SS can also be classified by complete SCR polyhedral complexes in NℝN_{\mathbb{R}}. This is not the case for general toric schemes over SS as is shown in [BS10].

Theorem 4.59.

The correspondence Π↦𝒳c⁡(Π)\Pi\mapsto{\mathcal{X}}_{\operatorname{c}(\Pi)}, where c⁡(Π)\operatorname{c}(\Pi) is the fan introduced in Definition 3.7, is a bijection between the set of complete SCR polyhedral complexes in NℝN_{\mathbb{R}} and the set of isomorphism classes of proper toric schemes over SS of relative dimension nn.

Proof.

Follows from [KKMS73, §IV.3(e)] and Corollary 3.15. ∎

If we are interested in toric schemes as toric models of a toric variety, we can restate the previous result as follows.

Theorem 4.60.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}}. Then there is a bijective correspondence between equivariant isomorphism classes of proper toric models over SS of XΣX_{\Sigma} and complete SCR polyhedral complexes Π\Pi in NℝN_{\mathbb{R}} such that rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma.

Proof.

Follows easily from Theorem 4.59. ∎

For the rest of the section we will restrict ourselves to the proper case and we will denote by Π\Pi a complete SCR polyhedral complex. To it we associate a complete fan c⁡(Π)\operatorname{c}(\Pi) in Nℝ×ℝ≥0N_{\mathbb{R}}\times\mathbb{R}_{\geq 0} and a complete fan rec⁡(Π)\operatorname{rec}(\Pi) in NℝN_{\mathbb{R}}. For short, we will use the notation

(4.61) 𝒳Π=𝒳c⁡(Π),{\mathcal{X}}_{\Pi}={\mathcal{X}}_{\operatorname{c}(\Pi)},

and we will identify the generic fibre 𝒳Π,η{\mathcal{X}}_{\Pi,\eta} with the toric variety Xrec⁡(Π)X_{\operatorname{rec}(\Pi)}.

Example 4.62.

We continue with Example 4.3. The fan ΣΔn\Sigma_{\Delta^{n}} is in particular an SCR polyhedral complex and the associated toric scheme over SS is ℙSn\mathbb{P}^{n}_{S}, the projective space over SS.

This example can be generalized to any complete fan Σ\Sigma in NℝN_{\mathbb{R}}.

Definition 4.63.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}}. Then Σ\Sigma is also a complete SCR polyhedral complex. Clearly rec⁡(Σ)=Σ\operatorname{rec}({\Sigma})=\Sigma. The toric scheme 𝒳Σ{\mathcal{X}}_{{\Sigma}} is a model over SS of XΣX_{\Sigma} which is called the canonical model. Its special fibre

𝒳Σ,o=XΣ,k{\mathcal{X}}_{\Sigma,o}=X_{\Sigma,k}

is the toric variety over kk defined by the fan Σ\Sigma.

The description of toric orbits in the case of a toric scheme over a DVR is more involved than the case of toric varieties over a field, because we have to consider two kind of orbits.

In the first place, there is a bijection between rec⁡(Π)\operatorname{rec}(\Pi) and the set of orbits under the action of 𝕋K\mathbb{T}_{K} on 𝒳Π,η{\mathcal{X}}_{\Pi,\eta}, that sends a cone σ∈rec⁡(Π)\sigma\in\operatorname{rec}(\Pi) to the orbit O⁡(σ)⊂𝒳Π,η=Xrec⁡(Π)O(\sigma)\subset{\mathcal{X}}_{\Pi,\eta}=X_{\operatorname{rec}(\Pi)} as in the case of toric varieties over a field. We will denote by 𝒱⁡(σ){\mathcal{V}}(\sigma) the Zariski closure in 𝒳Π{\mathcal{X}}_{\Pi} of the orbit O⁡(σ)O(\sigma) with its structure of reduced closed subscheme. Then 𝒱⁡(σ){\mathcal{V}}(\sigma) is a horizontal SS-scheme, in the sense that the structure morphism 𝒱⁡(σ)→S{\mathcal{V}}(\sigma)\to S is dominant, of relative dimension n−dim(σ)n-\dim(\sigma).

Next we describe 𝒱⁡(σ){\mathcal{V}}(\sigma) as a toric scheme over SS. As before, we write N⁡(σ)=N/(N∩ℝ​σ)N(\sigma)=N/(N\cap\mathbb{R}\sigma) and let πσ:Nℝ→N​(σ)ℝ\pi_{\sigma}\colon N_{\mathbb{R}}\to N(\sigma)_{\mathbb{R}} be the linear projection. Each polyhedron Λ\Lambda such that σ⊂rec⁡(Λ)\sigma\subset\operatorname{rec}(\Lambda) defines a polyhedron πσ​(Λ)\pi_{\sigma}(\Lambda) in N​(σ)ℝN(\sigma)_{\mathbb{R}}. One verifies that these polyhedra form a complete SCR polyhedral complex in N​(σ)ℝN(\sigma)_{\mathbb{R}}, that we denote Π⁡(σ)\Pi(\sigma). This polyhedral complex is called the star of σ\sigma in Π\Pi.

Proposition 4.64.

There is a canonical isomorphism of toric schemes

𝒳Π⁡(σ)⟶𝒱⁡(σ).{\mathcal{X}}_{\Pi(\sigma)}\longrightarrow{\mathcal{V}}(\sigma).
Proof.

The proof is analogous to the proof of Proposition 4.6. ∎

In the second place, there is a bijection between Π\Pi and the set of orbits under the action of 𝕋k\mathbb{T}_{k} on 𝒳o{\mathcal{X}}_{o} over the closed point oo. Given a polyhedron Λ∈Π\Lambda\in\Pi, we set

N~​(Λ)=N~/(N~∩ℝ​c⁡(Λ)),M~​(Λ)=N~​(Λ)∨=M~∩c⁡(Λ)⊥.{\widetilde{N}}(\Lambda)={\widetilde{N}}/({\widetilde{N}}\cap\mathbb{R}\negthinspace\operatorname{c}(\Lambda)),\quad{\widetilde{M}}(\Lambda)={\widetilde{N}}(\Lambda)^{\vee}={\widetilde{M}}\cap\operatorname{c}(\Lambda)^{\bot}.

We denote O⁡(Λ)=Spec⁡(k⁡[M~​(Λ)])O(\Lambda)=\operatorname{Spec}(k[{\widetilde{M}}(\Lambda)]).This is a torus over the residue field kk of dimension n−dim(Λ)n-\dim(\Lambda). There is a surjection of rings

K∘​[M~Λ]⟶k⁡[M~​(Λ)],χ(m,l)⟼{χ(m,l) if ​(m,l)∈M~​(Λ),0 if ​(m,l)∉M~​(Λ).K^{\circ}[{\widetilde{M}}_{\Lambda}]\longrightarrow k[{\widetilde{M}}(\Lambda)],\quad\chi^{(m,l)}\longmapsto\begin{cases}\chi^{(m,l)}&\text{ if }(m,l)\in{\widetilde{M}}(\Lambda),\\ 0&\text{ if }(m,l)\notin{\widetilde{M}}(\Lambda).\end{cases}

Since the element (0,1)(0,1) does not belong to M~​(Λ){\widetilde{M}}(\Lambda), then this surjection sends the ideal (χ(0,1)−ϖ)(\chi^{(0,1)}-\varpi) to zero. Therefore, it factorizes through a surjection K∘​[𝒳Λ]→k⁡[M~​(Λ)]K^{\circ}[{\mathcal{X}}_{\Lambda}]\to k[{\widetilde{M}}(\Lambda)], that defines a closed immersion O⁡(Λ)↪𝒳ΛO(\Lambda)\hookrightarrow{\mathcal{X}}_{\Lambda}. The subscheme O⁡(Λ)O(\Lambda) is contained in the special fibre 𝒳Π,o{\mathcal{X}}_{\Pi,o}, because the surjection sends ϖ\varpi to zero. By this reason, the orbits of this type will be called vertical.

We will denote by V⁡(Λ)V(\Lambda) the Zariski closure of the orbit O⁡(Λ)O(\Lambda). Then, V⁡(Λ)V(\Lambda) is a vertical cycle in the sense that its image by the structure morphism is the closed point oo. We next describe its toric structure. For each polyhedron Λ′\Lambda^{\prime} such that Λ\Lambda is a face of Λ′\Lambda^{\prime}, the image of c⁡(Λ′)\operatorname{c}(\Lambda^{\prime}) under the projection πΛ:N~ℝ→N~​(Λ)ℝ\pi_{\Lambda}\colon{\widetilde{N}}_{\mathbb{R}}\to{\widetilde{N}}(\Lambda)_{\mathbb{R}} is a strongly convex rational cone that we denote σΛ′\sigma_{\Lambda^{\prime}}. The cones σΛ′\sigma_{\Lambda^{\prime}} form a fan of N~​(Λ)ℝ{\widetilde{N}}(\Lambda)_{\mathbb{R}} that we denote Π⁡(Λ)\Pi(\Lambda). Observe that the fan Π⁡(Λ)\Pi(\Lambda) is the analogue of the star of a cone defined in (4.5). For each cone σ∈Π⁡(Λ)\sigma\in\Pi(\Lambda) there is a unique polyhedron Λσ∈Π\Lambda_{\sigma}\in\Pi such that Λ\Lambda is a face of Λσ\Lambda_{\sigma} and σ=πΛ​(c⁡(Λσ))\sigma=\pi_{\Lambda}(\operatorname{c}(\Lambda_{\sigma})).

Proposition 4.65.

There is a canonical isomorphism of toric varieties over kk

XΠ⁡(Λ),k⟶V⁡(Λ).X_{\Pi(\Lambda),k}\longrightarrow V(\Lambda).
Proof.

Again, the proof is analogous to the proof of Proposition 4.6. ∎

The description of the adjacency relations between orbits is similar to the one for toric varieties over a field. The orbit V⁡(Λ)V(\Lambda) is contained in V⁡(Λ′)V(\Lambda^{\prime}) if and only if the polyhedron Λ′\Lambda^{\prime} is a face of the polyhedron Λ\Lambda. Similarly, 𝒱⁡(σ){\mathcal{V}}(\sigma) is contained in 𝒱⁡(σ′){\mathcal{V}}(\sigma^{\prime}) if and only if σ′\sigma^{\prime} is a face of σ\sigma. Finally, V⁡(Λ)V(\Lambda) is contained in 𝒱⁡(σ){\mathcal{V}}(\sigma) if and only if σ\sigma is a face of the cone rec⁡(Λ)\operatorname{rec}(\Lambda).

Remark 4.66.

As a consequence of the above construction, we see that there is a one-to-one correspondence between the vertexes of Π\Pi and the components of the special fibre. For each v∈Π0v\in\Pi^{0}, the component V⁡(v)V(v) is a toric variety over kk defined by the fan Π⁡(v)\Pi(v) in N~ℝ/ℝ⁡(v,1){\widetilde{N}}_{\mathbb{R}}/\mathbb{R}(v,1). The orbits contained in V⁡(v)V(v) correspond to the polyhedra Λ∈Π\Lambda\in\Pi containing vv. In particular, the components given by two vertexes v,v′∈Π0v,v^{\prime}\in\Pi^{0} share an orbit of dimension ll if and only if there exists a polyhedron of dimension n−ln-l containing both vv and v′v^{\prime}.

To each polyhedron Λ∈Π\Lambda\in\Pi, hence to each vertical orbit, we can associate a combinatorial invariant, which we call its multiplicity. For a vertex v∈Π0v\in\Pi^{0}, this invariant agrees with the order of vanishing of ϖ\varpi along the component V⁡(v)V(v) (see (4.87)).

Denote by ȷ:N→N~\operatorname{\jmath}\colon N\to{\widetilde{N}} the inclusion ȷ⁡(u)=(u,0)\operatorname{\jmath}(u)=(u,0) and by pr:M~→M\operatorname{pr}\colon{\widetilde{M}}\to M the projection pr⁡(m,l)=m\operatorname{pr}(m,l)=m. We identify NN with its image. We set

N⁡(Λ)=N/(N∩ℝ​c⁡(Λ)),M⁡(Λ)=M∩pr⁡(c⁡(Λ)⊥).N(\Lambda)=N/(N\cap\mathbb{R}\negthinspace\operatorname{c}(\Lambda)),\quad M(\Lambda)=M\cap\operatorname{pr}(\operatorname{c}(\Lambda)^{\bot}).
Remark 4.67.

The lattice M⁡(Λ)M(\Lambda) can also be described as M⁡(Λ)=M∩LΛ⊥M(\Lambda)=M\cap L_{\Lambda}^{\bot}. Therefore, for a cone σ⊂Nℝ\sigma\subset N_{\mathbb{R}}, the notation just introduced agrees with the one in (4.4). Here, the polytope Λ\Lambda is contained in NℝN_{\mathbb{R}}. By contrast, for a polyhedron Γ⊂Mℝ\Gamma\subset M_{\mathbb{R}}, we follow Notation 3.103, so M⁡(Γ)=M∩LΓM(\Gamma)=M\cap L_{\Gamma}.

Then ȷ\operatorname{\jmath} and pr\operatorname{pr} induce inclusions of lattices of finite index N​(Λ)→N~​(Λ)N(\Lambda)\to{\widetilde{N}}(\Lambda) and M~​(Λ)→M​(Λ){\widetilde{M}}(\Lambda)\to M(\Lambda), that we denote also by ȷ\operatorname{\jmath} and pr\operatorname{pr}, respectively. These inclusions are dual of each other and in particular, their indexes agree.

Definition 4.68.

The multiplicity of a polyhedron Λ∈Π\Lambda\in\Pi is defined as

mult(Λ)=[M(Λ):pr(M~(Λ))]=[N~(Λ):ȷ(N(Λ))].\operatorname{mult}(\Lambda)=[M(\Lambda):\operatorname{pr}({\widetilde{M}}(\Lambda))]=[{\widetilde{N}}(\Lambda):\operatorname{\jmath}(N(\Lambda))].
Lemma 4.69.

If Λ∈Π\Lambda\in\Pi, then mult(Λ)=min{n≥1∣∃p∈aff(Λ),np∈N}\operatorname{mult}(\Lambda)=\min\{n\geq 1\mid\exists p\in\operatorname{aff}(\Lambda),\ np\in N\}.

Proof.

We consider the inclusion ℤ→N~​(Λ)\mathbb{Z}\to{\widetilde{N}}(\Lambda) that sends n∈ℤn\in\mathbb{Z} to the class of (0,n)(0,n). There is a commutative diagram with exact rows and columns

0\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}0\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}0\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}N⁡(Λ)∩ℤ\textstyle{N(\Lambda)\cap\mathbb{Z}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ℤ\textstyle{\mathbb{Z}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ℤ/(N⁡(Λ)∩ℤ)\textstyle{\mathbb{Z}/(N(\Lambda)\cap\mathbb{Z})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}0\textstyle{0}0\textstyle{0\ignorespaces\ignorespaces\ignorespaces\ignorespaces}N⁡(Λ)\textstyle{N(\Lambda)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}N~​(Λ)\textstyle{{\widetilde{N}}(\Lambda)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}N~​(Λ)/N​(Λ)\textstyle{{\widetilde{N}}(\Lambda)/N(\Lambda)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}0\textstyle{0}N⁡(Λ)/(N⁡(Λ)∩ℤ)\textstyle{N(\Lambda)/(N(\Lambda)\cap\mathbb{Z})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}N~​(Λ)/ℤ\textstyle{{\widetilde{N}}(\Lambda)/\mathbb{Z}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}0\textstyle{0}0\textstyle{0}

It is easy to see that the bottom arrow in the diagram is an isomorphism. By the Snake lemma the right vertical arrow is an isomorphism. Therefore

mult(Λ)=[ℤ:N(Λ)∩ℤ].\operatorname{mult}(\Lambda)=[\mathbb{Z}:N(\Lambda)\cap\mathbb{Z}].

We verify that N(Λ)∩ℤ={n∈ℤ∣∃p∈aff(Λ),np∈N},N(\Lambda)\cap\mathbb{Z}=\{n\in\mathbb{Z}\mid\exists p\in\operatorname{aff}(\Lambda),\ np\in N\}, from which the lemma follows. ∎

We now discuss equivariant morphisms of toric schemes.

Definition 4.70.

Let 𝕋i\mathbb{T}_{i}, i=1,2i=1,2, be split tori over SS and ρ:𝕋1→𝕋2\rho\colon\mathbb{T}_{1}\to\mathbb{T}_{2} a morphism of algebraic group schemes. Let 𝒳i{\mathcal{X}}_{i} be toric schemes over SS with torus 𝕋i\mathbb{T}_{i} and let μi\mu_{i} denote the corresponding action. A morphism φ:𝒳1→𝒳2\varphi\colon{\mathcal{X}}_{1}\to{\mathcal{X}}_{2} is ρ\rho-equivariant if the diagram

𝕋1×𝒳1\textstyle{\mathbb{T}_{1}\times{\mathcal{X}}_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}μ1\scriptstyle{\mu_{1}}ρ×φ\scriptstyle{\rho\times\varphi}𝒳1\textstyle{{\mathcal{X}}_{1}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}φ\scriptstyle{\varphi}𝕋2×𝒳2\textstyle{\mathbb{T}_{2}\times{\mathcal{X}}_{2}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}μ2\scriptstyle{\mu_{2}}𝒳2\textstyle{{\mathcal{X}}_{2}}

commutes. A morphism φ:𝒳1→𝒳2\varphi\colon{\mathcal{X}}_{1}\to{\mathcal{X}}_{2} is ρ\rho-toric if its restriction to 𝕋1,η\mathbb{T}_{1,\eta}, the torus over KK, coincides with that of ρ\rho.

It can be verified that a toric morphism of schemes over SS is also equivariant. In the sequel, we extend the construction of equivariant morphisms in §4.2 to proper toric schemes. Before that, we need to relate rational points on the open orbit of the toric variety with lattice points in NN.

Definition 4.71.

The valuation map of the field, val:K×→ℤ{\operatorname{val}}\colon K^{\times}\to\mathbb{Z}, induces a valuation map on 𝕋⁡(K)\mathbb{T}(K), also denoted val:𝕋⁡(K)→N{\operatorname{val}}\colon\mathbb{T}(K)\to N, by the identifications 𝕋⁡(K)=Hom⁡(M,K×)\mathbb{T}(K)=\operatorname{Hom}(M,K^{\times}) and N=Hom⁡(M,ℤ)N=\operatorname{Hom}(M,\mathbb{Z}).

Let 𝕋S,i\mathbb{T}_{S,i}, i=1,2i=1,2, be split tori over SS. For each ii, let NiN_{i} be the corresponding lattice and Πi\Pi_{i} a complete SCR polyhedral complex in Ni,ℝN_{i,\mathbb{R}}. Let A:N1→N2A\colon N_{1}\to N_{2} be an affine map such that, for every Λ1∈Π1\Lambda_{1}\in\Pi_{1}, there exists Λ2∈Π2\Lambda_{2}\in\Pi_{2} with A⁡(Λ1)⊂Λ2A(\Lambda_{1})\subset\Lambda_{2}. Let p∈𝒳Π2,0​(K)=𝕋2​(K)p\in{\mathcal{X}}_{\Pi_{2},0}(K)=\mathbb{T}_{2}(K) such that val⁡(p)=A⁡(0){\operatorname{val}}(p)=A(0). Write A=H+val⁡(p)A=H+{\operatorname{val}}(p), where H:N1→N2H\colon N_{1}\to N_{2} is a linear map. HH induces a morphism of algebraic groups

ρH:𝕋S,1⟶𝕋S,2.\rho_{H}\colon\mathbb{T}_{S,1}\longrightarrow\mathbb{T}_{S,2}.

Let Σi=rec⁡(Πi)\Sigma_{i}=\operatorname{rec}(\Pi_{i}). For each cone σ1∈Σ1\sigma_{1}\in\Sigma_{1}, there exists a cone σ2∈Σ2\sigma_{2}\in\Sigma_{2} with H⁡(σ1)⊂σ2H(\sigma_{1})\subset\sigma_{2}. Therefore HH and pp define an equivariant morphism φp,H:XΣ1→XΣ2\varphi_{p,H}\colon X_{\Sigma_{1}}\to X_{\Sigma_{2}} of toric varieties over KK as in Theorem 4.9.

Proposition 4.72.

With the above hypothesis, the morphism φp,H\varphi_{p,H} can be extended to a ρH\rho_{H}-equivariant morphism

Φp,A:𝒳Π1⟶𝒳Π2.\Phi_{p,A}\colon{\mathcal{X}}_{\Pi_{1}}\longrightarrow{\mathcal{X}}_{\Pi_{2}}.
Proof.

Let Λi∈Πi\Lambda_{i}\in\Pi_{i} such that A⁡(Λ1)⊂Λ2A(\Lambda_{1})\subset\Lambda_{2}. Then the map M~2→M~1{\widetilde{M}}_{2}\to{\widetilde{M}}_{1} given by (m,l)↦(H∨​m,⟨val⁡(p),m⟩+l)(m,l)\mapsto(H^{\vee}m,\langle{\operatorname{val}}(p),m\rangle+l) for m∈Mm\in M and l∈ℤl\in\mathbb{Z} (which is just the dual of the linearization of AA) induces a morphism of semigroups M~2,Λ2→M~1,Λ1{\widetilde{M}}_{2,\Lambda_{2}}\to{\widetilde{M}}_{1,\Lambda_{1}}. Since χm​(p)​ϖ−⟨val⁡(p),m⟩\chi^{m}(p)\varpi^{-\langle{\operatorname{val}}(p),m\rangle} belongs to K∘K^{\circ}, the assignment

χ(m,l)⟼(χm​(p)​ϖ−⟨val⁡(p),m⟩)​χ(H∨​m,⟨val⁡(p),m⟩+l)\chi^{(m,l)}\longmapsto(\chi^{m}(p)\varpi^{-\langle{\operatorname{val}}(p),m\rangle})\chi^{(H^{\vee}m,\langle{\operatorname{val}}(p),m\rangle+l)}

defines a ring morphism K∘​[M~2,Λ2]→K∘​[M~1,Λ1]K^{\circ}[{\widetilde{M}}_{2,\Lambda_{2}}]\to K^{\circ}[{\widetilde{M}}_{1,\Lambda_{1}}]. This morphism sends χ(0,1)−ϖ\chi^{(0,1)}-\varpi to χ(0,1)−ϖ\chi^{(0,1)}-\varpi, hence induces a morphism K∘​[𝒳Λ2]→K∘​[𝒳Λ1]K^{\circ}[{\mathcal{X}}_{\Lambda_{2}}]\to K^{\circ}[{\mathcal{X}}_{\Lambda_{1}}] and a map 𝒳Λ1→𝒳Λ2{\mathcal{X}}_{\Lambda_{1}}\to{\mathcal{X}}_{\Lambda_{2}}. Varying Λ1\Lambda_{1} and Λ2\Lambda_{2} we obtain maps, that glue together into a map

Φp,A:𝒳Π1⟶𝒳Π2.\Phi_{p,A}\colon{\mathcal{X}}_{\Pi_{1}}\longrightarrow{\mathcal{X}}_{\Pi_{2}}.

By construction, this map extends φp,H\varphi_{p,H} and is equivariant with respect to the morphism ρH\rho_{H}. ∎

As an example of the above construction, we consider the toric subschemes associated to orbits under the action of subtori. Let NN be a lattice, Π\Pi a complete SCR polyhedral complex in NℝN_{\mathbb{R}} and set Σ=rec⁡(Π)\Sigma=\operatorname{rec}(\Pi). Let Q⊂NQ\subset N be a saturated sublattice and let p∈XΣ,0​(K)p\in X_{\Sigma,0}(K). We set u0=val⁡(p)u_{0}={\operatorname{val}}(p). We consider the affine map A:Qℝ→NℝA\colon Q_{\mathbb{R}}\to N_{\mathbb{R}} given by A⁡(v)=v+u0A(v)=v+u_{0}. Recall that the sublattice QQ and the point pp induce maps of toric varieties (4.11)

XΣQ⟶YΣQ,p⸦⟶XΣ.X_{\Sigma_{Q}}\longrightarrow Y_{\Sigma_{Q},p}\lhook\joinrel\longrightarrow X_{\Sigma}.

We want to identify the toric model of XΣQX_{\Sigma_{Q}} induced by the toric model 𝒳Π{\mathcal{X}}_{\Pi} of XΣX_{\Sigma}. We define the complete SCR polyhedral complex ΠQ,u0=A−1​Π\Pi_{Q,u_{0}}=A^{-1}\Pi of QℝQ_{\mathbb{R}}. Then, rec⁡(ΠQ,u0)=ΣQ\operatorname{rec}(\Pi_{Q,u_{0}})=\Sigma_{Q}. Applying the construction of Proposition 4.72, we obtain an equivariant morphism of schemes over SS

(4.73) 𝒳ΠQ,u0⟶𝒳Π.{\mathcal{X}}_{\Pi_{Q,u_{0}}}\longrightarrow{\mathcal{X}}_{\Pi}.

The image of this map is the Zariski closure of YΣQ,pY_{\Sigma_{Q},p} and 𝒳ΠQ,u0{\mathcal{X}}_{\Pi_{Q,u_{0}}} is a toric model of XΣQX_{\Sigma_{Q}}. This map will be denoted either as Φp,A\Phi_{p,A} or Φp,Q\Phi_{p,Q}. Observe that the abstract toric scheme 𝒳ΠQ,u0{\mathcal{X}}_{\Pi_{Q,u_{0}}} only depends on QQ and on val⁡(p){\operatorname{val}}(p).

4.6. 𝕋\mathbb{T}-Cartier divisors on toric schemes

The theory of 𝕋\mathbb{T}-Cartier divisors carries over to the case of toric schemes over a DVR. Let 𝒳{\mathcal{X}} be a toric scheme over SS with torus 𝕋S\mathbb{T}_{S}. There are two morphisms from 𝕋S×𝒳\mathbb{T}_{S}\times{\mathcal{X}} to 𝒳{\mathcal{X}}: the toric action, that we denote by μ\mu, and the second projection, that we denote by π2\pi_{2}. A Cartier divisor DD on 𝒳{\mathcal{X}} is called a 𝕋\mathbb{T}-Cartier divisor if μ∗​D=π2∗​D.\mu^{\ast}D=\pi_{2}^{\ast}D.

𝕋\mathbb{T}-Cartier divisors over a toric scheme can be described combinatorially. For simplicity, we will discuss only the case of proper schemes. So, let Π\Pi be a complete SCR polyhedral complex in NℝN_{\mathbb{R}}, and 𝒳Π{\mathcal{X}}_{\Pi} the corresponding toric scheme. Let ψ\psi be an H-lattice function on Π\Pi (Definitions 3.88 and 3.60). Then ψ\psi defines a 𝕋\mathbb{T}-Cartier divisor in a way similar to the one for toric varieties over a field. We recall that the schemes {𝒳Λ}Λ∈Π\{{\mathcal{X}}_{\Lambda}\}_{\Lambda\in\Pi} form an open cover of 𝒳Π{\mathcal{X}}_{\Pi}. Choose a set of defining vectors {(mΛ,lΛ)}Λ∈Π\{(m_{\Lambda},l_{\Lambda})\}_{\Lambda\in\Pi} of ψ\psi. Then we set

Dψ={(𝒳Λ,ϖ−lΛ​χ−mΛ)}Λ∈Π,D_{\psi}=\{({\mathcal{X}}_{\Lambda},\varpi^{-l_{\Lambda}}\chi^{-m_{\Lambda}})\}_{\Lambda\in\Pi},

where we are using the identification (4.57). The divisor DψD_{\psi} only depends on ψ\psi and not on a particular choice of defining vectors.

We consider now toric varieties and 𝕋\mathbb{T}-Cartier divisors over SS as models of toric varieties and 𝕋\mathbb{T}-Cartier divisors over KK.

Definition 4.74.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and Ψ\Psi a virtual support function on Σ\Sigma. Let (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) be the associated toric variety and 𝕋\mathbb{T}-Cartier divisor defined over KK. A toric model of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) is a triple (𝒳,D,e)({\mathcal{X}},D,e), where 𝒳{\mathcal{X}} is a toric model over SS of XX, DD is a 𝕋\mathbb{T}-Cartier divisor on 𝒳{\mathcal{X}} and e>0e>0 is an integer such that the isomorphism ι:XΣ→𝒳η\iota\colon X_{\Sigma}\to{\mathcal{X}}_{\eta} that extends the identity of 𝕋K\mathbb{T}_{K} satisfies ι∗​(D)=e​DΨ\iota^{\ast}(D)=eD_{\Psi}. When e=1e=1, the toric model (𝒳,D,1)({\mathcal{X}},D,1) will be denoted simply by (𝒳,D)({\mathcal{X}},D). A toric model will be called proper whenever the scheme 𝒳{\mathcal{X}} is proper over SS.

Example 4.75.

We continue with Example 4.62. The function ΨΔn\Psi_{\Delta^{n}} is an H-lattice concave function on ΣΔn\Sigma_{\Delta^{n}} and (ℙSn,DΨΔn)(\mathbb{P}^{n}_{S},D_{\Psi_{\Delta^{n}}}) is a proper toric model of (ℙKn,DΨΔn)(\mathbb{P}^{n}_{K},D_{\Psi_{\Delta^{n}}}).

This example can be generalized as follows.

Definition 4.76.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and let Ψ\Psi be a virtual support function on Σ\Sigma. Then Σ\Sigma is a complete SCR polyhedral complex in NℝN_{\mathbb{R}} and Ψ\Psi is a rational piecewise affine function on Σ\Sigma. Then (𝒳Σ,DΨ)({\mathcal{X}}_{{\Sigma}},D_{\Psi}) is a model over SS of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}), which is called the canonical model.

Definition 4.77.

Let 𝒳{\mathcal{X}} be a toric scheme and ℒ{\mathcal{L}} a line bundle on 𝒳{\mathcal{X}}. A toric structure on ℒ{\mathcal{L}} is the choice of an element zz of the fibre ℒx0{\mathcal{L}}_{x_{0}}, where x0∈𝒳ηx_{0}\in{\mathcal{X}}_{\eta} is the distinguished point. A toric line bundle on 𝒳{\mathcal{X}} is a pair (ℒ,z)({\mathcal{L}},z), where ℒ{\mathcal{L}} is a line bundle over 𝒳{\mathcal{X}} and vv is a toric structure on ℒ{\mathcal{L}}. Frequently, when the toric structure is clear from the context, the element zz will be omitted from the notation and a toric line bundle will be denoted by the underlying line bundle. A toric section is a rational section that is regular and non vanishing over the principal open subset X0⊂𝒳ηX_{0}\subset{\mathcal{X}}_{\eta} and such that s⁡(x0)=zs(x_{0})=z. Exactly as in the case of toric varieties over a field, each 𝕋\mathbb{T}-Cartier divisor defines a toric line bundle 𝒪⁡(D){\mathcal{O}}(D) together with a toric section. When the 𝕋\mathbb{T}-Cartier divisor comes from an H-lattice function ψ\psi, the toric line bundle and toric section will be denoted ℒψ{\mathcal{L}}_{\psi} and sψs_{\psi} respectively.

In this section we will mainly use the language of 𝕋\mathbb{T}-Cartier divisors, but in §6 we will prefer the language of toric line bundles.

The following result follows directly form the definitions.

Proposition 4.78.

Let (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) be a toric variety with a 𝕋\mathbb{T}-Cartier divisor. Every toric model (𝒳,D,e)({\mathcal{X}},D,e) of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) induces a model (𝒳,𝒪⁡(D),e)({\mathcal{X}},\mathcal{O}(D),e) of (XΣ,LΨ)(X_{\Sigma},L_{\Psi}), in the sense of Definition 2.16, where the identification of 𝒪⁡(D)|XΣ\mathcal{O}(D)|_{X_{\Sigma}} with LΨ⊗eL_{\Psi}^{\otimes e} matches the toric sections. Such models will be called toric models.

Proposition-Definition 4.79.

We say that two toric models (𝒳i,Di,ei)({\mathcal{X}}_{i},D_{i},e_{i}), i=1,2i=1,2, are equivalent, if there exists a toric model (𝒳′,D′,e′)({\mathcal{X}}^{\prime},D^{\prime},e^{\prime}) of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) and morphisms of toric models αi:𝒳′→𝒳i\alpha_{i}\colon{\mathcal{X}}^{\prime}\to{\mathcal{X}}_{i}, i=1,2i=1,2, such that e′​αi∗​Di=ei​D′e^{\prime}\alpha_{i}^{\ast}D_{i}=e_{i}D^{\prime}. This is an equivalence relation.

Proof.

Symmetry and reflexivity are straightforward. For transitivity assume that we have toric models (𝒳i,Di,ei)({\mathcal{X}}_{i},D_{i},e_{i}), i=1,2,3i=1,2,3, that the first and second model are equivalent through (𝒳′,D′,e′)({\mathcal{X}}^{\prime},D^{\prime},e^{\prime}) and that the second and the third are equivalent through (𝒳′′,D′′,e′′)({\mathcal{X}}^{\prime\prime},D^{\prime\prime},e^{\prime\prime}). Then, by Theorem 4.60, 𝒳′{\mathcal{X}}^{\prime} and 𝒳′′{\mathcal{X}}^{\prime\prime} are defined by SCR polyhedral complexes Π′\Pi^{\prime} and Π′′\Pi^{\prime\prime} respectively, with rec⁡(Π′)=rec⁡(Π′′)=Σ\operatorname{rec}(\Pi^{\prime})=\operatorname{rec}(\Pi^{\prime\prime})=\Sigma. Let Π′′′=Π′⋅Π′′\Pi^{\prime\prime\prime}=\Pi^{\prime}\cdot\Pi^{\prime\prime}. By Lemma 3.11, rec⁡(Π′′′)=Σ\operatorname{rec}(\Pi^{\prime\prime\prime})=\Sigma. Thus Π′′′\Pi^{\prime\prime\prime} determines a model 𝒳′′′{\mathcal{X}}^{\prime\prime\prime} of XΣX_{\Sigma}. This model has morphisms β′\beta^{\prime} and β′′\beta^{\prime\prime} to 𝒳′{\mathcal{X}}^{\prime} and 𝒳′′{\mathcal{X}}^{\prime\prime} respectively. We put e′′′=e′​e′′e^{\prime\prime\prime}=e^{\prime}e^{\prime\prime} and D′′′=e′′β′∗D′=e′β′′∗D′′D^{\prime\prime\prime}=e^{\prime\prime}\beta^{\prime}{}^{\ast}D^{\prime}=e^{\prime}\beta^{\prime\prime}{}^{\ast}D^{\prime\prime}. Now it is easy to verify that (𝒳′′′,D′′′,e′′′)({\mathcal{X}}^{\prime\prime\prime},D^{\prime\prime\prime},e^{\prime\prime\prime}) provides the transitivity property. ∎

We are interested in proper toric models and equivalence classes because, by Definition 2.17, a proper toric model of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) induces an algebraic metric on LΨanL_{\Psi}^{{\text{\rm an}}}. By Proposition 2.18, equivalent toric models define the same algebraic metric.

We can classify proper models of 𝕋\mathbb{T}-Cartier divisors (and therefore of toric line bundles) in terms of H-lattice functions. We first recall the classification of 𝕋\mathbb{T}-Cartier divisors.

Theorem 4.80.

Let Π\Pi be a complete SCR polyhedral complex in NℝN_{\mathbb{R}} and let 𝒳Π{\mathcal{X}}_{\Pi} be the associated toric scheme over SS. The correspondence ψ↦Dψ\psi\mapsto D_{\psi} is an isomorphism between the group of H-lattice functions on Π\Pi and the group of 𝕋\mathbb{T}-Cartier divisors on 𝒳Π{\mathcal{X}}_{\Pi}. Moreover, if ψ1\psi_{1} and ψ2\psi_{2} are two H-lattice functions on Π\Pi, then the divisors Dψ1D_{\psi_{1}} and Dψ2D_{\psi_{2}} are rationally equivalent if and only if ψ1−ψ2\psi_{1}-\psi_{2} is affine.

Proof.

The result follows from [KKMS73, §IV.3(h)]. ∎

We next derive the classification theorem for models of 𝕋\mathbb{T}-Cartier divisors.

Theorem 4.81.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and Ψ\Psi a virtual support function on Σ\Sigma. Then the correspondence (Π,ψ)↦(𝒳Π,Dψ)(\Pi,\psi)\mapsto({\mathcal{X}}_{\Pi},D_{\psi}) is a bijection between:

  • ∙\bullet

    the set of pairs (Π,ψ)(\Pi,\psi), where Π\Pi is a complete SCR polyhedral complex in NℝN_{\mathbb{R}} with rec⁡(Π)\operatorname{rec}(\Pi)= Σ\Sigma and ψ\psi is an H-lattice function on Π\Pi such that rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi;

  • ∙\bullet

    the set of isomorphism classes of toric models (𝒳,D)({\mathcal{X}},D) of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}).

Proof.

Denote by ι:XΣ=Xrec⁡(Π)→𝒳Π\iota\colon X_{\Sigma}=X_{\operatorname{rec}(\Pi)}\to{\mathcal{X}}_{\Pi} the open immersion of the generic fibre. The recession function (Definition 3.85) determines the restriction of the 𝕋\mathbb{T}-Cartier divisor to the fibre over the generic point. Therefore, when ψ\psi is an H-lattice function on Π\Pi with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi, we have that

(4.82) ι∗​Dψ=Drec⁡(ψ)=DΨ.\iota^{\ast}D_{\psi}=D_{\operatorname{rec}(\psi)}=D_{\Psi}.

Thus (𝒳Π,Dψ)({\mathcal{X}}_{\Pi},D_{\psi}) is a toric model of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}). The statement follows from Theorem 4.60 and Theorem 4.80. ∎

Remark 4.83.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and Ψ\Psi a virtual support function on Σ\Sigma. Let (𝒳,D,e)({\mathcal{X}},D,e) be a toric model of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}). Then, by Theorem 4.81, there exists a complete SCR polyhedral complex Π\Pi in NℝN_{\mathbb{R}} with rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma and a rational piecewise affine function ψ\psi on Π\Pi such that e​ψe\psi is an H-lattice function, rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi and (𝒳,D,e)=(𝒳Π,De​ψ,e)({\mathcal{X}},D,e)=({\mathcal{X}}_{\Pi},D_{e\psi},e). Moreover, if (𝒳′,D′,e′)({\mathcal{X}}^{\prime},D^{\prime},e^{\prime}) is another toric model that gives the function ψ′\psi^{\prime}, then both models are equivalent if and only if ψ=ψ′\psi=\psi^{\prime}. Thus, to every toric model we have associated a rational piecewise affine function ψ\psi on Π\Pi such that rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi. Two equivalent models give rise to the same function.

The converse is not true. Given a rational piecewise affine function ψ\psi, with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi, we can find a complete SCR polyhedral complex Π\Pi such that ψ\psi is piecewise affine on Π\Pi. But, in general rec⁡(Π)\operatorname{rec}(\Pi) does not agree with Σ\Sigma. What we can expect is that Σ′:=rec⁡(Π)\Sigma^{\prime}:=\operatorname{rec}(\Pi) is a refinement of Σ\Sigma. Therefore the function ψ\psi gives us an equivalence class of toric models of (XΣ′,DΨ)(X_{\Sigma^{\prime}},D_{\Psi}). But ψ\psi may not determine an equivalence class of toric models of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}). In Corollary 5.43 in next section we will give a necessary condition for a function ψ\psi to define an equivalence class of toric models of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) and in Example 5.44 we will exhibit a function that does not satisfy this necessary condition. By contrast, as we will see in Theorem 4.97, the concave case is much more transparent.

The correspondence between 𝕋\mathbb{T}-Cartier divisors and 𝕋\mathbb{T}-Weil divisors has to take into account that we have two types of orbits. Each vertex v∈Π0v\in\Pi^{0} defines a vertical invariant prime Weil divisor V⁡(v)V(v) and every ray τ∈rec⁡(Π)1\tau\in\operatorname{rec}(\Pi)^{1} defines a horizontal prime Weil divisor 𝒱⁡(τ){\mathcal{V}}(\tau). If v∈Π0v\in\Pi^{0} is a vertex, by Lemma 4.69, its multiplicity mult⁡(v)\operatorname{mult}(v) is the smallest positive integer ν≥1\nu\geq 1 such that ν​v∈N\nu v\in N. If τ\tau is a ray, we denote by vτv_{\tau} the smallest lattice point of τ∖{0}\tau\setminus\{0\}.

Proposition 4.84.

Let ψ\psi be an H-lattice function on Π\Pi. Let DψD_{\psi} be the associated 𝕋\mathbb{T}-Cartier divisor. Then the corresponding 𝕋\mathbb{T}-Weil divisor is given by

(4.85) [Dψ]=∑v∈Π0−mult(v)ψ(v)V(v)+∑τ∈rec⁡(Π)1−rec(ψ)(vτ)𝒱(τ).[D_{\psi}]=\sum_{v\in\Pi^{0}}-\operatorname{mult}(v)\psi(v)V(v)+\sum_{\tau\in\operatorname{rec}(\Pi)^{1}}-\operatorname{rec}(\psi)(v_{\tau}){\mathcal{V}}(\tau).
Proof.

By Lemma 4.69, for v∈Π0v\in\Pi^{0}, the vector mult⁡(v)​v\operatorname{mult}(v)v is the minimal lattice vector in the ray c⁡(v)\operatorname{c}(v). Now it is easy to adapt the proof of [Ful93, §3.3, Lemma] to prove this proposition. ∎

Example 4.86.

Consider the constant H-lattice function ψϖ​(u)=−1\psi_{\varpi}(u)=-1. This function corresponds to the principal divisor div⁡(ϖ)\operatorname{div}(\varpi). Then

(4.87) div⁡(ϖ)=∑v∈Π0mult⁡(v)​V​(v).\operatorname{div}(\varpi)=\sum_{v\in\Pi^{0}}\operatorname{mult}(v)V(v).

Thus, for a vertex vv, the multiplicity of vv agrees with the multiplicity of the divisor V⁡(v)V(v) in the special fibre div⁡(ϖ)\operatorname{div}(\varpi). In particular, the special fibre 𝒳Π,o{\mathcal{X}}_{\Pi,o} is reduced if and only if all vertexes of Π0\Pi^{0} belong to NN.

We next study the restriction of 𝕋\mathbb{T}-Cartier divisors to orbits and their inverse image by equivariant morphisms. Let Π\Pi be a complete SCR polyhedral complex in NℝN_{\mathbb{R}}, and ψ\psi an H-lattice function on Π\Pi. Set Σ=rec⁡(Π)\Sigma=\operatorname{rec}(\Pi), and Ψ=rec⁡(ψ)\Psi=\operatorname{rec}(\psi). Choose sets of defining vectors {(mΛ,lΛ)}Λ∈Π\{(m_{\Lambda},l_{\Lambda})\}_{\Lambda\in\Pi} and {mσ}σ∈Σ\{m_{\sigma}\}_{\sigma\in\Sigma} for ψ\psi and Ψ\Psi, respectively.

Let σ∈Σ\sigma\in\Sigma. We describe the restriction of DψD_{\psi} to 𝒱⁡(σ){\mathcal{V}}(\sigma), the closure of a horizontal orbit. As in the case of toric varieties over a field, we first consider the case when Ψ|σ=0\Psi|_{\sigma}=0. Recall that 𝒱⁡(σ){\mathcal{V}}(\sigma) agrees with the toric scheme associated to the polyhedral complex Π⁡(σ)\Pi(\sigma) and that each element of Π⁡(σ)\Pi(\sigma) is the image by πσ:Nℝ→N​(σ)ℝ\pi_{\sigma}\colon N_{\mathbb{R}}\to N(\sigma)_{\mathbb{R}} of a polyhedron Λ∈Π\Lambda\in\Pi with σ⊂rec⁡(Λ)\sigma\subset\operatorname{rec}(\Lambda). The condition Ψ|σ=0\Psi|_{\sigma}=0 implies that we can define

(4.88) ψ⁡(σ):N​(σ)ℝ⟶ℝ,u+ℝ​σ⟼ψ⁡(u+v)\psi(\sigma)\colon N(\sigma)_{\mathbb{R}}\longrightarrow\mathbb{R},\quad u+\mathbb{R}\sigma\longmapsto\psi(u+v)

for any v∈ℝ​σv\in\mathbb{R}\sigma such that u+v∈⋃rec⁡(Λ)⊃σΛu+v\in\bigcup_{\operatorname{rec}(\Lambda)\supset\sigma}\Lambda. The function ψ⁡(σ)\psi(\sigma) can also be described in terms of defining vectors. For each Λ∈Π\Lambda\in\Pi with σ⊂rec⁡(Λ)\sigma\subset\operatorname{rec}(\Lambda), we will denote Λ¯∈Π⁡(σ){\overline{\Lambda}}\in\Pi(\sigma) for its image by πσ\pi_{\sigma}. For each Λ\Lambda as before, the condition Ψ|σ=0\Psi|_{\sigma}=0 implies that mΛ∈M⁡(σ)m_{\Lambda}\in M(\sigma). Hence we define (mΛ¯,lΛ¯)=(mΛ,lΛ)(m_{{\overline{\Lambda}}},l_{{\overline{\Lambda}}})=(m_{\Lambda},l_{\Lambda}) for Λ∈Π\Lambda\in\Pi with rec⁡(Λ)⊃σ\operatorname{rec}(\Lambda)\supset\sigma.

Proposition 4.89.

If Ψ|σ=0\Psi|_{\sigma}=0 then the divisor DψD_{\psi} and the horizontal orbit 𝒱⁡(σ){\mathcal{V}}(\sigma) intersect properly. Moreover, the set {(mΛ¯,lΛ¯)}Λ¯∈Π⁡(σ)\{(m_{{\overline{\Lambda}}},l_{{\overline{\Lambda}}})\}_{{\overline{\Lambda}}\in\Pi(\sigma)} is a set of defining vectors of ψ⁡(σ)\psi(\sigma) and the restriction of DψD_{\psi} to 𝒱⁡(σ){\mathcal{V}}(\sigma) is Dψ⁡(σ)D_{\psi(\sigma)}.

Proof.

The proof is analogous to the proof of Proposition 4.31. ∎

If Ψ|σ≠0\Psi|_{\sigma}\not=0, then 𝒱⁡(σ){\mathcal{V}}(\sigma) and DψD_{\psi} do not intersect properly and we can only restrict DψD_{\psi} with 𝒱⁡(σ){\mathcal{V}}(\sigma) up to rational equivalence. To this end, we consider the divisor Dψ−mσD_{\psi-m_{\sigma}}, that is rationally equivalent to DψD_{\psi} and intersects properly with 𝒱⁡(σ){\mathcal{V}}(\sigma). The restriction of this divisor to 𝒱⁡(σ){\mathcal{V}}(\sigma) corresponds to the H-lattice function (ψ−mσ)​(σ)(\psi-m_{\sigma})(\sigma) as defined above.

Let now Λ∈Π\Lambda\in\Pi be a polyhedron. We will denote by π~Λ:N~→N~​(Λ){\widetilde{\pi}}_{\Lambda}\colon{\widetilde{N}}\to{\widetilde{N}}(\Lambda) and πΛ:N→N⁡(Λ)\pi_{\Lambda}\colon N\to N(\Lambda) the projections and by π~Λ∨:M~​(Λ)→M~{\widetilde{\pi}}_{\Lambda}^{\vee}\colon{\widetilde{M}}(\Lambda)\to{\widetilde{M}} and πΛ∨:M⁡(Λ)→M\pi_{\Lambda}^{\vee}\colon M(\Lambda)\to M the dual maps. We will use the same notation for the linear maps obtained by tensoring with ℝ\mathbb{R}.

We first assume that ψ|Λ=0\psi|_{\Lambda}=0. If u∈N~​(Λ)ℝu\in{\widetilde{N}}(\Lambda)_{\mathbb{R}}, then there exists a polyhedron Λ′\Lambda^{\prime} with Λ\Lambda a face of Λ′\Lambda^{\prime} and a point (v,r)∈c⁡(Λ′)(v,r)\in\operatorname{c}(\Lambda^{\prime}) that is sent to uu under the projection π~Λ{\widetilde{\pi}}_{\Lambda}. Then we set

(4.90) ψ⁡(Λ):N~​(Λ)ℝ⟶ℝ,u⟼r​ψ​(v/r)=mΛ′​(v)+r​lΛ′.\psi(\Lambda)\colon{\widetilde{N}}(\Lambda)_{\mathbb{R}}\longrightarrow\mathbb{R},\quad u\longmapsto r\psi(v/r)=m_{\Lambda^{\prime}}(v)+rl_{\Lambda^{\prime}}.

The condition ψ|Λ=0\psi|_{\Lambda}=0 implies that the above equation does not depend on the choice of (v,r)(v,r).

We can describe also ψ⁡(Λ)\psi(\Lambda) in terms of defining vectors. For each cone σ∈Π⁡(Λ)\sigma\in\Pi(\Lambda) let Λσ∈Π\Lambda_{\sigma}\in\Pi be the polyhedron that has Λ\Lambda as a face and such that c⁡(Λ)\operatorname{c}(\Lambda) is mapped to σ\sigma by π~Λ{\widetilde{\pi}}_{\Lambda}. The condition ψ|Λ=0\psi|_{\Lambda}=0 implies that (mΛσ,lΛσ)∈M~​(Λ)(m_{\Lambda_{\sigma}},l_{\Lambda_{\sigma}})\in{\widetilde{M}}(\Lambda). We set mσ=(mΛσ,lΛσ)m_{\sigma}=(m_{\Lambda_{\sigma}},l_{\Lambda_{\sigma}}).

Proposition 4.91.

If ψ|Λ=0\psi|_{\Lambda}=0 then the divisor DψD_{\psi} intersects properly the orbit V⁡(Λ)V(\Lambda). Moreover, the set {mσ}σ∈Π⁡(Λ)\{m_{\sigma}\}_{\sigma\in\Pi(\Lambda)} is a set of defining vectors of ψ⁡(Λ)\psi(\Lambda) and the restriction of DψD_{\psi} to V⁡(Λ)V(\Lambda) is the divisor Dψ⁡(Λ)D_{\psi(\Lambda)}.

Proof.

The proof is analogous to that of Proposition 4.31. ∎

As before, when ψ|Λ≠0\psi|_{\Lambda}\not=0, we can only restrict DψD_{\psi} to V⁡(Λ)V(\Lambda) up to rational equivalence. In this case we just apply the previous proposition to the function ψ−mΛ−lΛ\psi-m_{\Lambda}-l_{\Lambda}.

Example 4.92.

We particularize (4.90) to the case of one-dimensional vertical orbits. Let Λ\Lambda be a (n−1)(n-1)-dimensional polyhedron. Hence V⁡(Λ)V(\Lambda) is a vertical curve. Let Λ1\Lambda_{1} and Λ2\Lambda_{2} be the two nn-dimensional polyhedron that have Λ\Lambda as a common face. Let v∈Nℚv\in N_{\mathbb{Q}} such that the class [(v,0)][(v,0)] is a generator of the lattice N~​(Λ){\widetilde{N}}(\Lambda) and the affine space (v,0)+ℝ​c⁡(Λ)(v,0)+\mathbb{R}\operatorname{c}(\Lambda) meets c⁡(Λ1)\operatorname{c}(\Lambda_{1}). This second condition fixes one of the two generators of N~​(Λ){\widetilde{N}}(\Lambda). Then, by equation (4.25)

(4.93) degDψ⁡(V⁡(Λ))=deg⁡([Dψ|V⁡(Λ)])=mΛ2​(v)−mΛ1​(v).\deg_{D_{\psi}}(V(\Lambda))=\deg([D_{\psi}|_{V(\Lambda)}])=m_{\Lambda_{2}}(v)-m_{\Lambda_{1}}(v).

We end this section discussing the inverse image of a 𝕋\mathbb{T}-Cartier divisor by an equivariant morphisms. With the notation of Proposition 4.72, let ψ\psi be an H-lattice function on Π2\Pi_{2}, and {(mΛ,lΛ)}Λ∈Π2\{(m_{\Lambda},l_{\Lambda})\}_{\Lambda\in\Pi_{2}} a set of defining vectors of ψ\psi. For each Γ∈Π1\Gamma\in\Pi_{1} we choose a polyhedron Γ′∈Π2\Gamma^{\prime}\in\Pi_{2} such that A⁡(Γ)⊂Γ′A(\Gamma)\subset\Gamma^{\prime}. We set mΓ=H∨​(mΓ′)m_{\Gamma}=H^{\vee}(m_{\Gamma^{\prime}}) and lΓ=mΓ′​(val⁡(p))+lΓ′l_{\Gamma}=m_{\Gamma^{\prime}}({\operatorname{val}}(p))+l_{\Gamma^{\prime}}. The following proposition follows easily.

Proposition 4.94.

The divisor DψD_{\psi} intersects properly the image of Φp,A\Phi_{p,A}. The function ψ∘A\psi\circ A is an H-lattice function on Π1\Pi_{1} and

Φp,A∗​Dψ=Dψ∘A.\Phi^{\ast}_{p,A}D_{\psi}=D_{\psi\circ A}.

Moreover, {(mΓ,lΓ)}Γ∈Π1\{(m_{\Gamma},l_{\Gamma})\}_{\Gamma\in\Pi_{1}} is a set of defining vectors of ψ∘A\psi\circ A.

4.7. Positivity on toric schemes

The relationship between the positivity of the line bundle and the concavity of the virtual support function can be extended to the case of toric schemes over a DVR. In particular, we have the following version of the Nakai-Moishezon criterion.

Theorem 4.95.

Let Π\Pi be a complete SCR complex in NℝN_{\mathbb{R}} and 𝒳Π{\mathcal{X}}_{\Pi} its associate toric scheme over SS. Let ψ\psi be an H-lattice function on Π\Pi and DψD_{\psi} the corresponding 𝕋\mathbb{T}-Cartier divisor on 𝒳Π{\mathcal{X}}_{\Pi}.

  1. (1)

    The following properties are equivalent:

    1. (a)

      DψD_{\psi} is ample;

    2. (b)

      Dψ⋅C>0D_{\psi}\cdot C>0 for every vertical curve CC contained in XΠ,oX_{\Pi,o};

    3. (c)

      Dψ⋅V⁡(Λ)>0D_{\psi}\cdot V(\Lambda)>0 for every (n−1)(n-1)-dimensional polyhedron Λ∈Π\Lambda\in\Pi;

    4. (d)

      The function ψ\psi is strictly concave on Π\Pi.

  2. (2)

    The following properties are equivalent:

    1. (a)

      DψD_{\psi} is generated by global sections;

    2. (b)

      Dψ⋅C≥0D_{\psi}\cdot C\geq 0 for every vertical curve CC contained in XΣ,oX_{\Sigma,o};

    3. (c)

      Dψ⋅V⁡(Λ)≥0D_{\psi}\cdot V(\Lambda)\geq 0 for every (n−1)(n-1)-dimensional polyhedron Λ∈Π\Lambda\in\Pi;

    4. (d)

      The function ψ\psi is concave.

Proof.

In both cases, the fact that (a) implies (b) and that (b) implies (c) is clear. The fact that (c) implies (d) follows from equation (4.93). The fact that (1d) implies (1a) is [KKMS73, §IV.3(k)].

Finally, we prove that (2d) implies (2a). Let ψ\psi be an H-lattice concave function. Each pair (m,l)∈M~(m,l)\in{\widetilde{M}} defines a rational section ϖl​χm​sψ\varpi^{l}\chi^{m}s_{\psi} of DψD_{\psi}. The section is regular if and only if the function m⁡(u)+lm(u)+l lies above ψ\psi. Moreover, for a polyhedron Λ∈Π\Lambda\in\Pi, this section does not vanish on 𝒳Λ{\mathcal{X}}_{\Lambda} if and only if ψ⁡(u)=m⁡(u)+l\psi(u)=m(u)+l for all u∈Λu\in\Lambda. Therefore, the affine pieces of the graph of ψ\psi define a set of global sections that generate 𝒪⁡(Dψ)\mathcal{O}(D_{\psi}). ∎

Definition 4.96.

We will say that a 𝕋\mathbb{T}-Cartier divisor on a toric scheme is semipositive if it is generated by global sections. Let XΣX_{\Sigma} be a proper toric variety over KK and let DΨD_{\Psi} be a 𝕋\mathbb{T}-Cartier divisor generated by global sections. A toric model (𝒳,D,e)({\mathcal{X}},D,e) is called semipositive if DD is semipositive.

Observe that, by Theorem 4.95, a toric model is semipositive if the associated metric is semipositive as in Definition 2.26. Equivalence classes of semipositive toric models are classified by rational concave functions.

Theorem 4.97.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}}. Let Ψ\Psi be a support function on Σ\Sigma. Then the correspondence of Theorem 4.81 induces a bijective correspondence between the set of rational piecewise affine concave functions ψ\psi with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi and the set of equivalence classes of semipositive toric models of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) over SS.

Proof.

Let (𝒳,D,e)({\mathcal{X}},D,e) be a semipositive toric model. By Theorem 4.81, to the pair (𝒳,D)({\mathcal{X}},D) corresponds a pair (Π,ψ′)(\Pi,\psi^{\prime}), where ψ′\psi^{\prime} is an H-lattice function on Π\Pi, rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma and rec⁡(ψ′)=e​Ψ\operatorname{rec}(\psi^{\prime})=e\Psi. By Theorem 4.95, the function ψ′\psi^{\prime} is concave. We put ψ=1e​ψ′\psi=\frac{1}{e}\psi^{\prime}. It is clear that equivalent models produce the same function.

Conversely, let ψ\psi be a rational piecewise affine concave function. Let Π′=Π⁡(ψ)\Pi^{\prime}=\Pi(\psi). This is a rational polyhedral complex. Let Σ′=rec⁡(Π′)\Sigma^{\prime}=\operatorname{rec}(\Pi^{\prime}). This is a conic rational polyhedral complex. By Proposition 3.72, Σ′=Π⁡(Ψ)\Sigma^{\prime}=\Pi(\Psi). Since Ψ\Psi is a support function on Σ\Sigma, we deduce that Σ\Sigma is a refinement of Σ′\Sigma^{\prime}. Put Π=Π′⋅Σ\Pi=\Pi^{\prime}\cdot\Sigma (Definition 3.10). Since Π′\Pi^{\prime} is a rational polyhedral complex and Σ\Sigma is a fan, then Π\Pi is an SCR polyhedral complex. Moreover, by Lemma 3.11, we have

rec⁡(Π)=rec⁡(Π′⋅Σ)=rec⁡(Π′)⋅rec⁡(Σ)=Σ′⋅Σ=Σ.\operatorname{rec}(\Pi)=\operatorname{rec}(\Pi^{\prime}\cdot\Sigma)=\operatorname{rec}(\Pi^{\prime})\cdot\operatorname{rec}(\Sigma)=\Sigma^{\prime}\cdot\Sigma=\Sigma.

Let e>0e>0 be an integer such that e​ψe\psi is an H-lattice function. Then (𝒳Π,De​ψ,e)({\mathcal{X}}_{\Pi},D_{e\psi},e) is a toric model of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}). Both procedures are inverse of each other. ∎

Recall that, for toric varieties over a field, a 𝕋\mathbb{T}-Cartier divisor generated by global sections can be determined, either by the support function Ψ\Psi or by its stability set ΔΨ\Delta_{\Psi}. In the case of toric schemes over a DVR, if ψ\psi is a concave rational piecewise affine function on Π\Pi and Ψ=rec⁡(ψ)\Psi=\operatorname{rec}(\psi), then the stability set of ψ\psi agrees with the stability set of Ψ\Psi. Then the equivalence class of toric models determined by ψ\psi is also determined by the Legendre-Fenchel dual function ψ∨\psi^{\vee}.

Corollary 4.98.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and Ψ\Psi a support function on Σ\Sigma. There is a bijection between equivalence classes of semipositive toric models of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) and rational piecewise affine concave functions on MℝM_{\mathbb{R}}, with effective support ΔΨ\Delta_{\Psi}.

Proof.

This follows from Theorem 4.97, Proposition 3.75 and Proposition 3.77. ∎

When DψD_{\psi} is generated by global sections, that is, when ψ\psi is concave, we can interpret its restriction to toric orbits in terms of direct and inverse images of concave functions.

Proposition 4.99.

Let Π\Pi be a complete SCR polyhedral complex in NℝN_{\mathbb{R}} and ψ\psi an H-lattice concave function on Π\Pi. Set Σ=rec⁡(Π)\Sigma=\operatorname{rec}(\Pi) and Ψ=rec⁡(ψ)\Psi=\operatorname{rec}(\psi). Let σ∈Σ\sigma\in\Sigma and mσ∈Mm_{\sigma}\in M such that Ψ|σ=mσ|σ\Psi|_{\sigma}=m_{\sigma}|_{\sigma}. Let πσ:Nℝ→N​(σ)ℝ\pi_{\sigma}\colon N_{\mathbb{R}}\to N(\sigma)_{\mathbb{R}} be the projection and πσ∨:M​(σ)ℝ→Mℝ\pi^{\vee}_{\sigma}\colon M(\sigma)_{\mathbb{R}}\to M_{\mathbb{R}} the dual inclusion. Then

(4.100) (ψ−mσ)​(σ)=(πσ)∗​(ψ−mσ),(\psi-m_{\sigma})(\sigma)=(\pi_{\sigma})_{\ast}(\psi-m_{\sigma}),

Hence the restriction of the divisor Dψ−mσD_{\psi-m_{\sigma}} to 𝒱⁡(σ){\mathcal{V}}(\sigma) corresponds to the H-lattice concave function (πσ)∗​(ψ−mσ)(\pi_{\sigma})_{\ast}(\psi-m_{\sigma}). Dually,

(4.101) (ψ−mσ)​(σ)∨=(πσ∨+mσ)∗​ψ∨.(\psi-m_{\sigma})(\sigma)^{\vee}=(\pi^{\vee}_{\sigma}+m_{\sigma})^{\ast}\psi^{\vee}.

In other words, the Legendre-Fenchel dual of (ψ−mσ)​(σ)(\psi-m_{\sigma})(\sigma) is the restriction of ψ∨\psi^{\vee} to the face FσF_{\sigma} translated by −mσ-m_{\sigma}.

Proof.

For equation (4.100), we suppose without loss of generality that mσ=0m_{\sigma}=0, and hence Ψ|σ=0\Psi|_{\sigma}=0. Let u∈N​(σ)ℝu\in N(\sigma)_{\mathbb{R}}. Then, the function ψ|πσ−1​(u)\psi|_{\pi^{-1}_{\sigma}(u)} is concave. Let Λ∈Π\Lambda\in\Pi such that rec⁡(Λ)=σ\operatorname{rec}(\Lambda)=\sigma and πσ−1​(u)∩Λ≠∅\pi^{-1}_{\sigma}(u)\cap\Lambda\not=\emptyset. Then, πσ−1​(u)∩Λ\pi^{-1}_{\sigma}(u)\cap\Lambda is a polyhedron of maximal dimension in πσ−1​(u)\pi^{-1}_{\sigma}(u). The restriction of ψ\psi to this polyhedron is constant and, by (4.88), agrees with ψ​(σ)​(u)\psi(\sigma)(u). Therefore, by concavity,

(πσ)∗​ψ​(u)=maxv∈πσ−1​(u)⁡ψ⁡(v),(\pi_{\sigma})_{\ast}\psi(u)=\max_{v\in\pi^{-1}_{\sigma}(u)}\psi(v),

agrees with ψ​(σ)​(u)\psi(\sigma)(u). Thus we obtain equation (4.100). Equation (4.101) follows from the previous equation and Proposition 3.78(2). To prove equation (4.101) when mσ≠0m_{\sigma}\not=0 we use Proposition 3.40(4). ∎

We now consider the case of a vertical orbit. For a function ψ\psi as before, with Ψ=rec⁡(ψ)\Psi=\operatorname{rec}(\psi), we denote by c⁡(ψ):N~ℝ→ℝ¯\operatorname{c}(\psi)\colon{\widetilde{N}}_{\mathbb{R}}\to\underline{\mathbb{R}} the concave function given by

c⁡(ψ)​(u,r)={r​ψ​(u/r), if ​r>0,Ψ⁡(u), if ​r=0,−∞, if ​r<0.\operatorname{c}(\psi)(u,r)=\begin{cases}r\psi(u/r),&\text{ if }r>0,\\ \Psi(u),&\text{ if }r=0,\\ -\infty,&\text{ if }r<0.\end{cases}

The function c⁡(ψ)\operatorname{c}(\psi) is a support function on c⁡(Π)\operatorname{c}(\Pi).

Lemma 4.102.

The stability set of c⁡(ψ)\operatorname{c}(\psi) is the epigraph epi⁡(−ψ∨)⊂M~ℝ\operatorname{epi}(-\psi^{\vee})\subset{\widetilde{M}}_{\mathbb{R}}.

Proof.

The H-representation of c⁡(ψ)\operatorname{c}(\psi) is

dom⁡(c⁡(ψ))\displaystyle{\operatorname{dom}}(\operatorname{c}(\psi)) ={(u,r)∈N~ℝ∣r≥0},\displaystyle=\{(u,r)\in{\widetilde{N}}_{\mathbb{R}}\mid r\geq 0\},
c⁡(ψ)​(u,r)\displaystyle\operatorname{c}(\psi)(u,r) =minΛ⁡(mΛ​(u)+lΛ​r).\displaystyle=\min_{\Lambda}(m_{\Lambda}(u)+l_{\Lambda}r).

By Proposition 3.64

stab⁡(c⁡(ψ))=ℝ≥0​(0,1)+conv⁡({(mΛ,lΛ)}Λ∈Π).\operatorname{stab}(\operatorname{c}(\psi))=\mathbb{R}_{\geq 0}(0,1)+\operatorname{conv}(\{(m_{\Lambda},l_{\Lambda})\}_{\Lambda\in\Pi}).

Furthermore, by the same proposition, for x∈stab⁡(ψ)x\in\operatorname{stab}(\psi),

ψ∨(x)=sup{∑Λ−λΛlΛ|λΛ≥0,∑ΛλΛ=1,∑ΛλΛmΛ=x}.\psi^{\vee}(x)=\sup\left\{\sum_{\Lambda}-\lambda_{\Lambda}l_{\Lambda}\bigg|\lambda_{\Lambda}\geq 0,\sum_{\Lambda}\lambda_{\Lambda}=1,\sum_{\Lambda}\lambda_{\Lambda}m_{\Lambda}=x\right\}.

Hence epi⁡(−ψ∨)=ℝ≥0​(0,1)+conv⁡({(mΛ,lΛ)}Λ∈Π),\operatorname{epi}(-\psi^{\vee})=\mathbb{R}_{\geq 0}(0,1)+\operatorname{conv}(\{(m_{\Lambda},l_{\Lambda})\}_{\Lambda\in\Pi}), which proves the statement. ∎

Proposition 4.103.

Let Π\Pi and ψ\psi be as before and let Λ∈Π\Lambda\in\Pi. Let mΛ∈Mm_{\Lambda}\in M and lΛ∈ℤl_{\Lambda}\in\mathbb{Z} be such that ψ|Λ=(mΛ+lΛ)|Λ\psi|_{\Lambda}=(m_{\Lambda}+l_{\Lambda})|_{\Lambda}. Let π~Λ:N~ℝ→N~​(Λ)ℝ{\widetilde{\pi}}_{\Lambda}\colon{\widetilde{N}}_{\mathbb{R}}\to{\widetilde{N}}(\Lambda)_{\mathbb{R}} be the projection, and π~Λ∨:M~​(Λ)ℝ→M~ℝ{\widetilde{\pi}}^{\vee}_{\Lambda}\colon{\widetilde{M}}(\Lambda)_{\mathbb{R}}\to{\widetilde{M}}_{\mathbb{R}} the dual map. Then

(4.104) (ψ−mΛ−lΛ)​(Λ)=(π~Λ)∗​(c⁡(ψ−mΛ−lΛ)).(\psi-m_{\Lambda}-l_{\Lambda})(\Lambda)=({\widetilde{\pi}}_{\Lambda})_{\ast}(\operatorname{c}(\psi-m_{\Lambda}-l_{\Lambda})).

Moreover, this is a support function on the fan Π⁡(Λ)\Pi(\Lambda). Its stability set is the polytope Δψ,Λ:=(π~Λ∨+(mΛ,lΛ))−1​epi⁡(−ψ∨)\Delta_{\psi,\Lambda}:=({\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\Lambda}))^{-1}\operatorname{epi}(-\psi^{\vee}). Hence, the restriction of the divisor Dψ−mΛ−lΛD_{\psi-m_{\Lambda}-l_{\Lambda}} to the variety V⁡(Λ)V(\Lambda) is the divisor associated to the support function of Δψ,Λ\Delta_{\psi,\Lambda}

Proof.

To prove equation (4.104) we may assume that mΛ=0m_{\Lambda}=0 and lΛ=0l_{\Lambda}=0. Let u∈N~​(Λ)ℝu\in{\widetilde{N}}(\Lambda)_{\mathbb{R}}. Then, the function c⁡(ψ)|π~Λ−1​(u)\operatorname{c}(\psi)|_{{\widetilde{\pi}}^{-1}_{\Lambda}(u)} is concave. Let Λ′∈Π\Lambda^{\prime}\in\Pi such that Λ\Lambda is a face of Λ′\Lambda^{\prime} and π~Λ−1​(u)∩c⁡(Λ′)≠∅{\widetilde{\pi}}^{-1}_{\Lambda}(u)\cap\operatorname{c}(\Lambda^{\prime})\not=\emptyset. Then, π~Λ−1​(u)∩c⁡(Λ′){\widetilde{\pi}}^{-1}_{\Lambda}(u)\cap\operatorname{c}(\Lambda^{\prime}) is a polyhedron of maximal dimension of π~Λ−1​(u){\widetilde{\pi}}^{-1}_{\Lambda}(u) and the restriction of c⁡(ψ)\operatorname{c}(\psi) to this polyhedron is constant and, by equation (4.90), agrees with ψ​(Λ)​(u)\psi(\Lambda)(u). Therefore, by concavity,

(π~Λ)∗​c⁡(ψ)​(u)=maxv∈πσ−1​(u)​c​(ψ)​(v),({\widetilde{\pi}}_{\Lambda})_{\ast}\operatorname{c}(\psi)(u)=\max_{v\in\pi^{-1}_{\sigma}(u)}\operatorname{c}(\psi)(v),

agrees with ψ​(Λ)​(u)\psi(\Lambda)(u). This proves equation (4.104).

Back in the general case when mΛm_{\Lambda} and lΛl_{\Lambda} may be different from zero, by Proposition 3.78, Proposition 3.40(4) and Lemma 4.102 we have

stab⁡((π~Λ)∗​(c⁡(ψ−mΛ−lΛ)))\displaystyle\operatorname{stab}(({\widetilde{\pi}}_{\Lambda})_{\ast}(\operatorname{c}(\psi-m_{\Lambda}-l_{\Lambda}))) =(π~Λ∨)−1​stab⁡(c⁡(ψ−mΛ−lΛ))\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda})^{-1}\operatorname{stab}(\operatorname{c}(\psi-m_{\Lambda}-l_{\Lambda}))
=(π~Λ∨)−1​(stab⁡(c⁡(ψ))−(mΛ,lΛ))\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda})^{-1}(\operatorname{stab}(\operatorname{c}(\psi))-(m_{\Lambda},l_{\Lambda}))
=(π~Λ∨+(mΛ,lΛ))−1​stab⁡(c⁡(ψ))\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\Lambda}))^{-1}\operatorname{stab}(\operatorname{c}(\psi))
=(π~Λ∨+(mΛ,lΛ))−1​epi⁡(−ψ∨).\displaystyle=({\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\Lambda}))^{-1}\operatorname{epi}(-\psi^{\vee}).

The remaining statements are clear. ∎

We next interpret the above result in terms of dual polyhedral complexes. Let Π⁡(ψ)\Pi(\psi) and Π⁡(ψ∨)\Pi(\psi^{\vee}) be the pair of dual polyhedral complexes associated to ψ\psi. Since ψ\psi is piecewise affine on Π\Pi, then Π\Pi is a refinement of Π⁡(ψ)\Pi(\psi). For each Λ∈Π\Lambda\in\Pi we will denote by Λ¯∈Π⁡(ψ)\overline{\Lambda}\in\Pi(\psi) the smallest element of Π⁡(ψ)\Pi(\psi) that contains Λ\Lambda. It is characterized by the fact that ri⁡(Λ)∩ri⁡(Λ¯)≠∅.\operatorname{ri}(\Lambda)\cap\operatorname{ri}(\overline{\Lambda})\not=\emptyset. Let Λ∗∈Π⁡(ψ∨)\Lambda^{\ast}\in\Pi(\psi^{\vee}) be the polyhedron Λ∗=ℒ​ψ​(Λ¯)\Lambda^{\ast}={\mathcal{L}}\psi(\overline{\Lambda}). This polyhedron agrees with ∂ψ⁡(u0)\partial\psi(u_{0}) for any u0∈ri⁡(Λ)u_{0}\in\operatorname{ri}(\Lambda). Then the function ψ∨|Λ∗\psi^{\vee}|_{\Lambda^{\ast}} is affine. The polyhedron Λ∗−mΛ\Lambda^{\ast}-m_{\Lambda} is contained in M​(Λ)ℝM(\Lambda)_{\mathbb{R}}. The polyhedron

Λ∗~={(x,−ψ∨​(x))|x∈Λ∗}{\widetilde{\Lambda^{\ast}}}=\{(x,-\psi^{\vee}(x))|x\in\Lambda^{\ast}\}

is a face of epi⁡(−ψ∨)\operatorname{epi}(-\psi^{\vee}) and it agrees with the intersection of the image of πΛ∨+(mΛ,lΛ)\pi^{\vee}_{\Lambda}+(m_{\Lambda},l_{\Lambda}) with this epigraph. We consider the commutative diagram of lattices

M~​(Λ)\textstyle{{\widetilde{M}}(\Lambda)\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π~Λ∨+(mΛ,lλ)\scriptstyle{{\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\lambda})}pr\scriptstyle{\operatorname{pr}}M~\textstyle{{\widetilde{M}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}pr\scriptstyle{\operatorname{pr}}M⁡(Λ)\textstyle{M(\Lambda)\ignorespaces\ignorespaces\ignorespaces\ignorespaces}πΛ∨+mΛ\scriptstyle{\pi^{\vee}_{\Lambda}+m_{\Lambda}}M,\textstyle{M,}

where πΛ∨\pi^{\vee}_{\Lambda} is the inclusion M⁡(Λ)⊂MM(\Lambda)\subset M, and the corresponding commutative diagram of real vector spaces obtained by tensoring with ℝ\mathbb{R}. This diagram induces a commutative diagram of polytopes

Δψ,Λ\textstyle{\Delta_{\psi,\Lambda}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}π~Λ∨+(mΛ,lλ)\scriptstyle{{\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\lambda})}pr\scriptstyle{\operatorname{pr}}Λ∗~\textstyle{{\widetilde{\Lambda^{\ast}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}pr\scriptstyle{\operatorname{pr}}Λ∗−mΛ\textstyle{\Lambda^{\ast}-m_{\Lambda}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}πΛ∨+mΛ\scriptstyle{\pi^{\vee}_{\Lambda}+m_{\Lambda}}Λ∗,\textstyle{\Lambda^{\ast},}

where all the arrows are isomorphisms.

In other words, the polytope Δψ,Λ\Delta_{\psi,\Lambda} associated to the restriction of Dψ−mΛ−lΛD_{\psi-m_{\Lambda}-l_{\Lambda}} to V⁡(Λ)V(\Lambda) is obtained as follows. We include M~​(Λ)ℝ{\widetilde{M}}(\Lambda)_{\mathbb{R}} in M~ℝ{\widetilde{M}}_{\mathbb{R}} throughout the affine map π~Λ∨+(mΛ,lλ){\widetilde{\pi}}^{\vee}_{\Lambda}+(m_{\Lambda},l_{\lambda}). The image of this map intersects the polyhedron epi⁡(−ψ∨)\operatorname{epi}(-\psi^{\vee}) in the face of it that lies above Λ∗\Lambda^{\ast}. The inverse image of this face agrees with Δψ,Λ\Delta_{\psi,\Lambda}.

Since we have an explicit description of the polytope Δψ,Λ\Delta_{\psi,\Lambda}, we can easily calculate the degree with respect to DψD_{\psi} of an orbit V⁡(Λ)V(\Lambda).

Proposition 4.105.

Let Π\Pi be a complete SCR polyhedral complex in NℝN_{\mathbb{R}} and ψ\psi an H-lattice concave function on Π\Pi. Let Λ∈Π\Lambda\in\Pi be a polyhedron of dimension n−kn-k, u0∈ri⁡(Λ)u_{0}\in\operatorname{ri}(\Lambda) and Λ∗=∂ψ⁡(u0)\Lambda^{\ast}=\partial\psi(u_{0}). Then

(4.106) mult⁡(Λ)​degDψ⁡(V⁡(Λ))=k!​volM⁡(Λ)⁡(Λ∗),\operatorname{mult}(\Lambda)\deg_{D_{\psi}}(V(\Lambda))=k!\operatorname{vol}_{M(\Lambda)}(\Lambda^{\ast}),

where mult⁡(Λ)\operatorname{mult}(\Lambda) is the multiplicity of Λ\Lambda (see Definition 4.68).

Proof.

From the description of Dψ|V⁡(Λ)D_{\psi}|_{V(\Lambda)} and Proposition 4.37, we know that

degDψ⁡(V⁡(Λ))=k!​volM~​(Λ)⁡(Δψ,Λ).\deg_{D_{\psi}}(V(\Lambda))=k!\operatorname{vol}_{{\widetilde{M}}(\Lambda)}(\Delta_{\psi,\Lambda}).

Since

volM~​(Λ)(Δψ,Λ)=1[M(Λ):M~(Λ)]volM⁡(Λ)(Λ∗),\operatorname{vol}_{{\widetilde{M}}(\Lambda)}(\Delta_{\psi,\Lambda})=\frac{1}{[M(\Lambda):{\widetilde{M}}(\Lambda)]}\operatorname{vol}_{M(\Lambda)}(\Lambda^{\ast}),

the result follows from the definition of the multiplicity. ∎

Remark 4.107.

If dim(Λ∗)<k\dim(\Lambda^{\ast})<k, then both sides of (4.106) are zero. If dim(Λ∗)=k\dim(\Lambda^{\ast})=k, then M⁡(Λ)=M⁡(Λ∗)M(\Lambda)=M(\Lambda^{\ast}) and volM⁡(Λ)⁡(Λ∗)\operatorname{vol}_{M(\Lambda)}(\Lambda^{\ast}) agrees with the lattice volume of Λ∗\Lambda^{\ast}.

We now interpret the inverse image of a semipositive 𝕋\mathbb{T}-Cartier divisor by an equivariant morphism in terms of direct and inverse images of concave functions.

Proposition 4.108.

With the hypothesis of Proposition 4.72, let ψ2\psi_{2} be an H-lattice concave function on Π2\Pi_{2} and let Dψ2D_{\psi_{2}} be the corresponding semipositive 𝕋\mathbb{T}-Cartier divisor. Then Φp,A∗​Dψ2\Phi_{p,A}^{\ast}D_{\psi_{2}} is the semipositive 𝕋\mathbb{T}-Cartier divisor associated to the H-lattice concave function ψ1=A∗​ψ2\psi_{1}=A^{\ast}\psi_{2}. Moreover the Legendre-Fenchel dual is given by

ψ1∨=(H∨)∗​(ψ2∨−val⁡(p)).\psi_{1}^{\vee}=(H^{\vee})_{\ast}(\psi_{2}^{\vee}-{\operatorname{val}}(p)).
Proof.

The first statement is Proposition 4.94. The second statement follows from Proposition 3.78(1). ∎

Example 4.109.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and Ψ\Psi a support function on Σ\Sigma. By Theorem 4.97, any equivalence class of semipositive models of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) is determined by a rational piecewise affine concave function ψ\psi with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi. By Lemma 3.79, any such function can be realized as the inverse image by an affine map of the support function of a standard simplex. Using the previous proposition, any equivalence class of semipositive toric models can be induced by an equivariant projective morphism.

More explicitly, let e>0e>0 be an integer such that e​ψe\psi is an H-lattice concave function. Let Π\Pi be a complete SCR complex in NℝN_{\mathbb{R}} compatible by e​ψe\psi and such that rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma (see the proof of Theorem 4.97). Then, (𝒳Π,De​ψ,e)({\mathcal{X}}_{\Pi},D_{e\psi},e) is a toric model of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) in the class determined by ψ\psi.

Choose an H-representation e​ψ​(u)=min0≤i≤r⁡(mi​(u)+li)e\psi(u)=\min_{0\leq i\leq r}(m_{i}(u)+l_{i}) with (mi,li)∈M~(m_{i},l_{i})\in{\widetilde{M}} for i=0,…,ri=0,\dots,r. Put 𝜶=(l1−l0,…,lr−l0)\boldsymbol{\alpha}=(l_{1}-l_{0},\dots,l_{r}-l_{0}). Let HH and AA be as in Lemma 3.79. In our case, HH is a morphism of lattices and

(4.110) e​ψ=A∗​ΨΔr+m0+l0.e\psi=A^{\ast}\Psi_{\Delta^{r}}+m_{0}+l_{0}.

We follow examples 4.3, 4.26, 4.44 and 4.75, and consider ℙSr\mathbb{P}^{r}_{S} as a toric scheme over SS. Let p=(p0:…:pr)p=(p_{0}:\dots:p_{r}) be a rational point in the principal open subset of ℙKr\mathbb{P}^{r}_{K} such that val⁡(p)=𝜶{\operatorname{val}}(p)=\boldsymbol{\alpha}. One can verify that the hypothesis of Proposition 4.72 are satisfied. Let Φp,A:𝒳Π→ℙSr\Phi_{p,A}\colon{\mathcal{X}}_{\Pi}\to\mathbb{P}^{r}_{S} be the associated morphism. Then

De​ψ=Φp,A∗​DΨΔr+div⁡(ϖ−l0​χ−m0).D_{e\psi}=\Phi_{p,A}^{\ast}D_{\Psi_{\Delta^{r}}}+\operatorname{div}(\varpi^{-l_{0}}\chi^{-m_{0}}).

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