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5. Metrics and measures on toric varieties [02ST]

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5. Metrics and measures on toric varieties

The aim of this section is to characterize the metrics on a toric line bundle over a toric variety that are, at the same time, invariant under the action of the compact torus and approachable or integrable. Moreover we study the associated measures.

5.1. The variety with corners XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0})

Let KK be either ℝ\mathbb{R}, ℂ\mathbb{C} or a complete field with respect to an absolute value associated to a nontrivial discrete valuation. When K=ℝK=\mathbb{R} we will use the technique of Remark 2.5 and in the non-Archimedean case we will use the notations of §2.3. Let 𝕋\mathbb{T} be an nn-dimensional split torus over KK and let NN and M=N∨M=N^{\vee} be the corresponding lattices. Let Σ\Sigma be a fan in NℝN_{\mathbb{R}}. For each cone σ∈Σ\sigma\in\Sigma, we will denote by XσanX_{\sigma}^{{\text{\rm an}}} the complex analytic space Xσ​(ℂ)X_{\sigma}(\mathbb{C}) in Archimedean case or the Berkovich analytic space associated to the scheme Xσ,KX_{\sigma,K} in the non-Archimedean case. These analytic spaces glue together in an analytic space XΣanX_{\Sigma}^{{\text{\rm an}}}.

Given any cone σ∈Σ\sigma\in\Sigma, we write

Xσ​(ℝ≥0)=Homsg⁡(Mσ,(ℝ≥0,×)).X_{\sigma}(\mathbb{R}_{\geq 0})=\operatorname{Hom}_{\operatorname{sg}}(M_{\sigma},(\mathbb{R}_{\geq 0},\times)).

On Xσ​(ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0}), we put the coarsest topology such that, for each m∈Mσm\in M_{\sigma}, the map Xσ​(ℝ≥0)→ℝ≥0X_{\sigma}(\mathbb{R}_{\geq 0})\to\mathbb{R}_{\geq 0} given by γ↦γ⁡(m)\gamma\mapsto\gamma(m) is continuous. Observe that if τ\tau is a face of σ\sigma, then there is a dense open immersion Xτ​(ℝ≥0)↪Xσ​(ℝ≥0)X_{\tau}(\mathbb{R}_{\geq 0})\hookrightarrow X_{\sigma}(\mathbb{R}_{\geq 0}). Hence the topological spaces Xσ​(ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0}) glue together to define a topological space XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}). This is the variety with corners associated to XΣX_{\Sigma}. Analogously to the algebraic case, one can prove that this topological space is Hausdorff and that the spaces Xσ​(ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0}) can be identified with open subspaces of XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}) satisfying

Xσ​(ℝ≥0)∩Xσ′​(ℝ≥0)=Xσ∩σ′​(ℝ≥0).X_{\sigma}(\mathbb{R}_{\geq 0})\cap X_{\sigma^{\prime}}(\mathbb{R}_{\geq 0})=X_{\sigma\cap\sigma^{\prime}}(\mathbb{R}_{\geq 0}).

For each σ∈Σ\sigma\in\Sigma there is a continuous map ρσ:Xσan→Xσ​(ℝ≥0)\rho_{\sigma}\colon X^{{\text{\rm an}}}_{\sigma}\to X_{\sigma}(\mathbb{R}_{\geq 0}). This map is given, in the Archimedean case, by

Xσan=Homsg⁡(Mσ,(ℂ,×))​⟶|⋅|​Homsg⁡(Mσ,(ℝ≥0,×))=Xσan​(ℝ≥0).X^{{\text{\rm an}}}_{\sigma}=\operatorname{Hom}_{\operatorname{sg}}(M_{\sigma},(\mathbb{C},\times))\overset{|\cdot|}{\longrightarrow}\operatorname{Hom}_{\operatorname{sg}}(M_{\sigma},(\mathbb{R}_{\geq 0},\times))=X^{{\text{\rm an}}}_{\sigma}(\mathbb{R}_{\geq 0}).

While, in the non-Archimedean case, since a point p∈Xσanp\in X_{\sigma}^{{\text{\rm an}}} corresponds to a multiplicative seminorm on K⁡[Mσ]K[M_{\sigma}] and a point in Xσ​(ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0}) corresponds to a semigroup homomorphism from MσM_{\sigma} to (ℝ≥0,×)(\mathbb{R}_{\geq 0},\times), we can define ρσ​(p)\rho_{\sigma}(p) as the semigroup homomorphism that, to an element m∈Mσm\in M_{\sigma}, corresponds |χm​(p)||\chi^{m}(p)|. These maps glue together to define a continuous map ρΣ:XΣan→XΣ​(ℝ≥0)\rho_{\Sigma}:X_{\Sigma}^{{\text{\rm an}}}\to X_{\Sigma}(\mathbb{R}_{\geq 0}).

Lemma 5.1.

The map ρΣ\rho_{\Sigma} satisfies ρΣ−1​(Xσ​(ℝ≥0))=Xσan\rho_{\Sigma}^{-1}(X_{\sigma}(\mathbb{R}_{\geq 0}))=X_{\sigma}^{{\text{\rm an}}}.

Proof.

By definition Xσan⊂ρΣ−1​(Xσ​(ℝ≥0))X_{\sigma}^{{\text{\rm an}}}\subset\rho_{\Sigma}^{-1}(X_{\sigma}(\mathbb{R}_{\geq 0})). For the reverse inclusion we will write only the non-Archimedean case. Assume that p∈ρΣ−1​(Xσ​(ℝ≥0))p\in\rho_{\Sigma}^{-1}(X_{\sigma}(\mathbb{R}_{\geq 0})). There is a σ′\sigma^{\prime} with p∈Xσ′anp\in X_{\sigma^{\prime}}^{{\text{\rm an}}}. Let τ=σ∩σ′\tau=\sigma\cap\sigma^{\prime} be the common face. Then pp is a multiplicative seminorm of K⁡[Mσ′]K[M_{\sigma^{\prime}}] and we show next that it can be extended to a multiplicative seminorm of K⁡[Mτ]K[M_{\tau}]. By [Ful93, §1.2 Proposition 2] there is an element u∈Mσ′u\in M_{\sigma^{\prime}} such that Mτ=Mσ′+ℤ≥0​(−u)M_{\tau}=M_{\sigma^{\prime}}+\mathbb{Z}_{\geq 0}(-u). Hence K⁡[Mτ]=K⁡[Mσ′+ℤ≥0​(−u)]K[M_{\tau}]=K[M_{\sigma^{\prime}}+\mathbb{Z}_{\geq 0}(-u)]. Since ρΣ​(p)∈Xτ​(ℝ≥0)\rho_{\Sigma}(p)\in X_{\tau}(\mathbb{R}_{\geq 0}) we have that |χu​(p)|≠0|\chi^{u}(p)|\not=0. Therefore pp extends to a multiplicative seminorm of K⁡[Mτ]K[M_{\tau}]. Hence p∈Xτan⊂Xσanp\in X^{{\text{\rm an}}}_{\tau}\subset X^{{\text{\rm an}}}_{\sigma}. ∎

When Σ\Sigma is complete, the analytic space XΣanX_{\Sigma}^{{\text{\rm an}}} is compact, and the map ρΣ\rho_{\Sigma} is proper. By Lemma 5.1, for each cone σ∈Σ\sigma\in\Sigma, the map ρσ\rho_{\sigma} is proper. Since every rational cone belongs to a complete fan, the map ρΣ\rho_{\Sigma} is proper even if Σ\Sigma is not complete. Of particular interest is the case when σ={0}\sigma=\{0\}. Then 𝕋an:=X0an\mathbb{T}^{{\text{\rm an}}}:=X_{0}^{{\text{\rm an}}} is an Abelian analytic group, that is, an Abelian group object in the category of analytic spaces. In particular, for any field extension K′K^{\prime} of KK, the set X0an​(K′)X_{0}^{{\text{\rm an}}}(K^{\prime}) is an Abelian group. Also 𝕋⁡(ℝ≥0):=X0​(ℝ≥0)≃(ℝ≥0)n\mathbb{T}(\mathbb{R}_{\geq 0}):=X_{0}(\mathbb{R}_{\geq 0})\simeq(\mathbb{R}_{\geq 0})^{n} is a topological Abelian group. Moreover, 𝕋an\mathbb{T}^{{\text{\rm an}}} acts on XΣanX^{{\text{\rm an}}}_{\Sigma}, 𝕋⁡(ℝ≥0)\mathbb{T}(\mathbb{R}_{\geq 0}) acts on XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}) and the map ρΣ\rho_{\Sigma} is equivariant with respect to these actions. The kernel of the map ρ0\rho_{0} is a closed subgroup, that we call the compact torus of 𝕋an\mathbb{T}^{{\text{\rm an}}} and we denote by 𝕊an\mathbb{S}^{{\text{\rm an}}}. In the Archimedean case it is isomorphic to (S1)n(S^{1})^{n}, while in the non-Archimedean case it is the compact torus of Example 2.8. In fact, the fibres of the map ρΣ\rho_{\Sigma} are orbits under the action of 𝕊an\mathbb{S}^{{\text{\rm an}}}. Therefore the space Xσ​(ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0}) is the quotient of XσanX_{\sigma}^{{\text{\rm an}}} by the action of the closed subgroup 𝕊an\mathbb{S}^{{\text{\rm an}}}. We warn the reader that the compact topological space underlying 𝕊an\mathbb{S}^{{\text{\rm an}}} is not an abstract group (see [Ber90, Chapter 5]).

The maps ρσ\rho_{\sigma}, σ∈Σ\sigma\in\Sigma, have canonical sections that we denote θσ\theta_{\sigma}. These sections glue together to give a section θΣ\theta_{\Sigma} of ρΣ\rho_{\Sigma}. In the Archimedean case θσ\theta_{\sigma} is induced by the semigroup inclusion ℝ≥0⊂ℂ\mathbb{R}_{\geq 0}\subset\mathbb{C}. In the non-Archimedean case θσ\theta_{\sigma} is defined by the following result.

Proposition-Definition 5.2.

Assume that we are in the non-Archimedean case. For each γ∈Homsg⁡(Mσ,ℝ≥0)\gamma\in\operatorname{Hom}_{\operatorname{sg}}(M_{\sigma},\mathbb{R}_{\geq 0}), the seminorm that, to a function ∑αm​χm∈K⁡[Mσ]\sum\alpha_{m}\chi^{m}\in K[M_{\sigma}] assigns the value supm(|αm|​γ​(m))\sup_{m}(|\alpha_{m}|\gamma(m)), is a multiplicative seminorm on K⁡[Mσ]K[M_{\sigma}] that extends the norm of KK. Therefore it determines a point of XσanX^{{\text{\rm an}}}_{\sigma} that we denote as θσ​(γ)\theta_{\sigma}(\gamma). The maps θσ\theta_{\sigma} are injective, continuous and proper. Moreover, they glue together to define a map

θΣ:XΣ​(ℝ≥0)⟶XΣan\theta_{\Sigma}\colon X_{\Sigma}(\mathbb{R}_{\geq 0})\longrightarrow X_{\Sigma}^{{\text{\rm an}}}

that is injective, continuous and proper. Every point in the image of θΣ\theta_{\Sigma} is fixed under the action of 𝕊an\mathbb{S}^{{\text{\rm an}}}.

Proof.

The fact that the seminorm θσ​(γ)\theta_{\sigma}(\gamma) extends the norm of KK is clear. Let now f=∑mαm​χmf=\sum_{m}\alpha_{m}\chi^{m} and g=∑lβl​χlg=\sum_{l}\beta_{l}\chi^{l} and write f​g=∑kεk​χkfg=\sum_{k}\varepsilon_{k}\chi^{k} with εk=∑m+l=kαm​βl\varepsilon_{k}=\sum_{m+l=k}\alpha_{m}\beta_{l}. Then, since the absolute value of KK is ultrametric,

supk∈Mσ(|εk|​γ​(k))≤supm∈Mσ(|αm|​γ​(m))​supl∈Mσ(|βl|​γ​(l)).\sup_{k\in M_{\sigma}}(|\varepsilon_{k}|\gamma(k))\leq\sup_{m\in M_{\sigma}}(|\alpha_{m}|\gamma(m))\sup_{l\in M_{\sigma}}(|\beta_{l}|\gamma(l)).

Let Mf={m∈Mσ|supm′(|αm′|​γ​(m′))=|αm|​γ​(m)}M_{f}=\{m\in M_{\sigma}|\sup_{m^{\prime}}(|\alpha_{m^{\prime}}|\gamma(m^{\prime}))=|\alpha_{m}|\gamma(m)\}. We define MgM_{g} analogously. Let rr be a vertex of the Minkowski sum conv⁡(Mf)+conv⁡(Mg)\operatorname{conv}(M_{f})+\operatorname{conv}(M_{g}). Then there is a unique decomposition r=mr+lrr=m_{r}+l_{r} with mr∈Mfm_{r}\in M_{f} and lr∈Mgl_{r}\in M_{g}. Hence εr=αmr​βlr\varepsilon_{r}=\alpha_{m_{r}}\beta_{l_{r}}. Thus

supk∈Mσ(|εk|​γ​(k))≥|εr|​γ​(r)=supm∈Mσ(|αm|​γ​(m))​supl∈Mσ(|βl|​γ​(l)).\sup_{k\in M_{\sigma}}(|\varepsilon_{k}|\gamma(k))\geq|\varepsilon_{r}|\gamma(r)=\sup_{m\in M_{\sigma}}(|\alpha_{m}|\gamma(m))\sup_{l\in M_{\sigma}}(|\beta_{l}|\gamma(l)).

Thus θσ​(γ)​(f​g)=θσ​(γ)​(f)​θσ​(γ)​(g)\theta_{\sigma}(\gamma)(fg)=\theta_{\sigma}(\gamma)(f)\theta_{\sigma}(\gamma)(g). Hence, it is a multiplicative.

We show next that the map θσ\theta_{\sigma} is continuous. The topology of XσanX^{{\text{\rm an}}}_{\sigma} is the coarsest topology that makes the functions p→|f⁡(p)|p\to|f(p)| continuous for all f∈K⁡[Mσ]f\in K[M_{\sigma}]. Thus to show that θσ\theta_{\sigma} is continuous it is enough to show that the map γ→|f⁡(θσ​(γ))|\gamma\to|f(\theta_{\sigma}(\gamma))| is continuous on Xσ​(ℝ≥0)=Homsg⁡(Mσ,ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0})=\operatorname{Hom}_{\operatorname{sg}}(M_{\sigma},\mathbb{R}_{\geq 0}). The topology of Xσ​(ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0}) is the coarsest topology such that, for each m∈Mσm\in M_{\sigma}, the map γ→γ⁡(m)\gamma\to\gamma(m) is continuous. Since, for f=∑m∈Mσαm​χmf=\sum_{m\in M_{\sigma}}\alpha_{m}\chi^{m}, we have that

|f⁡(θσ​(γ))|=max⁡(|αm|​γ​(m)),|f(\theta_{\sigma}(\gamma))|=\max(|\alpha_{m}|\gamma(m)),

we obtain that θσ\theta_{\sigma} is continuous. Since each θσ\theta_{\sigma} is a section of ρσ\rho_{\sigma}, they are injective.

The fact that the maps θσ\theta_{\sigma} glue together to give a continuous map θΣ\theta_{\Sigma} and that θΣ\theta_{\Sigma} is a section of ρΣ\rho_{\Sigma} follows easily from the definitions. This implies in particular that θΣ\theta_{\Sigma} is injective. When Σ\Sigma is complete, since XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}) is compact and XΣanX^{{\text{\rm an}}}_{\Sigma} is Hausdorff, the map θΣ\theta_{\Sigma} is proper. We deduce that the map θΣ\theta_{\Sigma} is proper in general, by using the same argument that shows that the function ρΣ\rho_{\Sigma} is proper.

The last assertion is clear from the definition of θσ​(γ)\theta_{\sigma}(\gamma). ∎

Let now

(5.3) λK={1, if ​K=ℂ,−log⁡|ϖ|, otherwise.\lambda_{K}=\begin{cases}1,&\text{ if }K=\mathbb{C},\\ -\log|\varpi|,&\text{ otherwise.}\end{cases}

and denote by 𝐞K:ℝ→ℝ>0{\operatorname{\mathbf{e}}}_{K}\colon\mathbb{R}\to\mathbb{R}_{>0} the map u↦exp⁡(−λK​u)u\mapsto\exp(-\lambda_{K}u). This map induces an homeomorphism Nℝ→X0​(ℝ>0)N_{\mathbb{R}}\rightarrow X_{0}(\mathbb{R}_{>0}) that we also denote by 𝐞K{\operatorname{\mathbf{e}}}_{K}.

In the non-Archimedean case, the map val:𝕋⁡(K)→N{\operatorname{val}}\colon\mathbb{T}(K)\to N of Definition 4.71, can be extended to a map 𝕋an→Nℝ\mathbb{T}^{{\text{\rm an}}}\to N_{\mathbb{R}} that we denote valK{\operatorname{val}}_{K} or, when KK is clear from the context by val{\operatorname{val}}. For each p∈X0anp\in X^{{\text{\rm an}}}_{0} we denote by valK⁡(p)∈Homsg⁡(M,ℝ)=Nℝ{\operatorname{val}}_{K}(p)\in\operatorname{Hom}_{\operatorname{sg}}(M,\mathbb{R})=N_{\mathbb{R}} the morphism

(5.4) m⟼⟨m,valK⁡(p)⟩=−log⁡|χm​(p)|λK.m\longmapsto\langle m,{\operatorname{val}}_{K}(p)\rangle=\frac{-\log|\chi^{m}(p)|}{\lambda_{K}}.

In the Archimedean case we will denote by valℂ{\operatorname{val}}_{\mathbb{C}} or simply by val{\operatorname{val}} the map defined by the same equation. Then, the diagram

(5.5) X0an\textstyle{X_{0}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}valK\scriptstyle{{\operatorname{val}}_{K}}ρ0\scriptstyle{\rho_{0}}Nℝ\textstyle{N_{\mathbb{R}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}𝐞K\scriptstyle{{\operatorname{\mathbf{e}}}_{K}}X0​(ℝ≥0)\textstyle{X_{0}(\mathbb{R}_{\geq 0})}

is commutative.

The map 𝐞K{\operatorname{\mathbf{e}}}_{K} allows us to see XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}) as a partial compactification on NℝN_{\mathbb{R}}. Following [AMRT75, Chapter I, §1] we can give another description of the topology of XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}). For σ∈Σ\sigma\in\Sigma, we denote

Nσ=∐τ​ face of ​σN​(τ)ℝ.N_{\sigma}=\coprod_{\tau\text{ face of }\sigma}N(\tau)_{\mathbb{R}}.

We choose a positive definite bilinear pairing in NℝN_{\mathbb{R}}. Hence we can identify the quotient spaces N​(τ)ℝN(\tau)_{\mathbb{R}} with subspaces of NℝN_{\mathbb{R}}, that, for simplicity, we will denote also by N​(τ)ℝN(\tau)_{\mathbb{R}}. For a point u∈N​(τ)ℝu\in N(\tau)_{\mathbb{R}}, let U⊂N​(τ)ℝU\subset N(\tau)_{\mathbb{R}} be a neighbourhood of uu. For each τ′\tau^{\prime} face of τ\tau, τ\tau induces a cone πτ′​(τ)\pi_{\tau^{\prime}}(\tau) contained in N​(τ′)ℝN(\tau^{\prime})_{\mathbb{R}}. If p∈τp\in\tau its image πτ′​(p)\pi_{\tau^{\prime}}(p) in N​(τ′)ℝN(\tau^{\prime})_{\mathbb{R}}, is contained in πτ′​(τ)\pi_{\tau^{\prime}}(\tau). We write

(5.6) W⁡(τ,U,p)=∐τ′​ face of ​τπτ′​(U+p+τ).W(\tau,U,p)=\coprod_{\tau^{\prime}\text{ face of }\tau}\pi_{\tau^{\prime}}(U+p+\tau).

Moving UU and pp we obtain a basis of neighbourhoods of uu in NσN_{\sigma}. This defines a topology on NσN_{\sigma} such that the map 𝐞K:Nℝ→Xσ​(ℝ≥0){\operatorname{\mathbf{e}}}_{K}\colon N_{\mathbb{R}}\to X_{\sigma}(\mathbb{R}_{\geq 0}) extends to a homeomorphism Nσ→Xσ​(ℝ≥0)N_{\sigma}\to X_{\sigma}(\mathbb{R}_{\geq 0}).

We write

NΣ=∐σ∈ΣN​(σ)ℝ,N_{\Sigma}=\coprod_{\sigma\in\Sigma}N(\sigma)_{\mathbb{R}},

and put in NΣN_{\Sigma} the topology that makes {Nσ}σ∈Σ\{N_{\sigma}\}_{\sigma\in\Sigma} an open cover. Then the map 𝐞K{\operatorname{\mathbf{e}}}_{K} extends to a homeomorphism between NΣN_{\Sigma} and XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}) and the map valK{\operatorname{val}}_{K} extends to a proper continuous map XΣan→NΣX^{{\text{\rm an}}}_{\Sigma}\to N_{\Sigma} such that the diagram

(5.7) XΣan\textstyle{X_{\Sigma}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}valK\scriptstyle{{\operatorname{val}}_{K}}ρΣ\scriptstyle{\rho_{\Sigma}}NΣ\textstyle{N_{\Sigma}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}𝐞K\scriptstyle{{\operatorname{\mathbf{e}}}_{K}}XΣ​(ℝ≥0)\textstyle{X_{\Sigma}(\mathbb{R}_{\geq 0})}

is commutative.

Remark 5.8.

In case we are given a strictly concave support function Ψ\Psi on a fan Σ\Sigma, then NΣN_{\Sigma} is homeomorphic to the polytope ΔΨ\Delta_{\Psi} introduced in §4.4. An homeomorphism is obtained as the composition of 𝐞K{\operatorname{\mathbf{e}}}_{K} with the moment map μ:XΣ​(ℝ≥0)→ΔΨ\mu\colon X_{\Sigma}(\mathbb{R}_{\geq 0})\rightarrow\Delta_{\Psi} induced by Ψ\Psi:

NΣ⟶𝐞KXΣ​(ℝ≥0)⟶μΔΨu⟼𝐞K⁡(u)⟼∑exp⁡(−λK​⟨m,u⟩)​m∑exp⁡(−λK​⟨m,u⟩)\begin{matrix}N_{\Sigma}&\mathrel{\mathop{\kern 0.0pt\longrightarrow}\limits^{{\operatorname{\mathbf{e}}}_{K}}}&X_{\Sigma}(\mathbb{R}_{\geq 0})&\mathrel{\mathop{\kern 0.0pt\longrightarrow}\limits^{\mu}}&\Delta_{\Psi}\\[5.69054pt] u&\longmapsto&{\operatorname{\mathbf{e}}}_{K}(u)&\longmapsto&\frac{\sum\exp(-\lambda_{K}\langle m,u\rangle)m}{\sum\exp(-\lambda_{K}\langle m,u\rangle)}\end{matrix}

where the sums in the last expression are over the elements m∈M∩ΔΨm\in M\cap\Delta_{\Psi}.

We end this section stating the functorial properties of the space XΣ​(ℝ≥0)X_{\Sigma}(\mathbb{R}_{\geq 0}). The proofs are left to the reader. Let NN and Σ\Sigma be as before and σ∈Σ\sigma\in\Sigma. Recall that the associated closed subvariety V⁡(σ)V(\sigma) is canonically isomorphic to the toric variety XΣ⁡(σ)X_{\Sigma(\sigma)}.

Proposition 5.9.

The natural map N​(σ)ℝ↪NσN(\sigma)_{\mathbb{R}}\hookrightarrow N_{\sigma} extends to a continuous map XΣ⁡(σ)​(ℝ≥0)→XΣ​(ℝ≥0)X_{\Sigma(\sigma)}(\mathbb{R}_{\geq 0})\to X_{\Sigma}(\mathbb{R}_{\geq 0}). Moreover, there are commutative diagrams

XΣ⁡(σ)an\textstyle{X_{\Sigma(\sigma)}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ρΣ⁡(σ)\scriptstyle{\rho_{\Sigma(\sigma)}}XΣan\textstyle{X_{\Sigma}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ρΣ\scriptstyle{\rho_{\Sigma}}XΣ⁡(σ)​(ℝ≥0)\textstyle{X_{\Sigma(\sigma)}(\mathbb{R}_{\geq 0})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}XΣ​(ℝ≥0),\textstyle{X_{\Sigma}(\mathbb{R}_{\geq 0}),} XΣ⁡(σ)an\textstyle{X_{\Sigma(\sigma)}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}XΣan\textstyle{X_{\Sigma}^{{\text{\rm an}}}}XΣ⁡(σ)​(ℝ≥0)\textstyle{X_{\Sigma(\sigma)}(\mathbb{R}_{\geq 0})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}θΣ⁡(σ)\scriptstyle{\theta_{\Sigma(\sigma)}}XΣ​(ℝ≥0).\textstyle{X_{\Sigma}(\mathbb{R}_{\geq 0}).\ignorespaces\ignorespaces\ignorespaces\ignorespaces}θΣ\scriptstyle{\theta_{\Sigma}}

Let N1N_{1} and N2N_{2} be lattices and let Σ1\Sigma_{1} and Σ2\Sigma_{2} be complete fans in N1,ℝN_{1,\mathbb{R}} and N2,ℝN_{2,\mathbb{R}} respectively. Let H:N1→N2H\colon N_{1}\to N_{2} be a linear map such that, for each cone σ1∈Σ1\sigma_{1}\in\Sigma_{1}, there is a cone σ2∈Σ2\sigma_{2}\in\Sigma_{2} with H⁡(σ1)⊂σ2H(\sigma_{1})\subset\sigma_{2}. Let p∈XΣ2,0​(K)p\in X_{\Sigma_{2},0}(K) and let A:N1,ℝ→N2,ℝA\colon N_{1,\mathbb{R}}\to N_{2,\mathbb{R}} be the affine map A=H+val⁡(p)A=H+{\operatorname{val}}(p).

Proposition 5.10.

The affine map A:N1,ℝ→N2,ℝA\colon N_{1,\mathbb{R}}\to N_{2,\mathbb{R}} extends to a continuous map XΣ1​(ℝ≥0)→XΣ2​(ℝ≥0)X_{\Sigma_{1}}(\mathbb{R}_{\geq 0})\to X_{\Sigma_{2}}(\mathbb{R}_{\geq 0}) that we also denote by φp,H\varphi_{p,H}. Moreover, there are commutative diagrams

XΣ1an\textstyle{X_{\Sigma_{1}}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}φp,H\scriptstyle{\varphi_{p,H}}ρΣ1\scriptstyle{\rho_{\Sigma_{1}}}XΣ2an\textstyle{X_{\Sigma_{2}}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ρΣ2\scriptstyle{\rho_{\Sigma_{2}}}XΣ1​(ℝ≥0)\textstyle{X_{\Sigma_{1}}(\mathbb{R}_{\geq 0})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}φp,H\scriptstyle{\varphi_{p,H}}XΣ2​(ℝ≥0),\textstyle{X_{\Sigma_{2}}(\mathbb{R}_{\geq 0}),} XΣ1an\textstyle{X_{\Sigma_{1}}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}φp,H\scriptstyle{\varphi_{p,H}}XΣ2an\textstyle{X_{\Sigma_{2}}^{{\text{\rm an}}}}XΣ1​(ℝ≥0)\textstyle{X_{\Sigma_{1}}(\mathbb{R}_{\geq 0})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}φp,H\scriptstyle{\varphi_{p,H}}θΣ1\scriptstyle{\theta_{\Sigma_{1}}}XΣ2​(ℝ≥0).\textstyle{X_{\Sigma_{2}}(\mathbb{R}_{\geq 0}).\ignorespaces\ignorespaces\ignorespaces\ignorespaces}θΣ2\scriptstyle{\theta_{\Sigma_{2}}}

5.2. Toric metrics

From now on we assume that Σ\Sigma is complete. Let LL be a toric line bundle on XΣX_{\Sigma} and let ss be a toric section of LL (Definition 4.19). By Theorem 4.22 and Theorem 4.18, we can find a virtual support function Ψ\Psi on Σ\Sigma such that there is an isomorphism L≃𝒪⁡(DΨ)L\simeq\mathcal{O}(D_{\Psi}) that sends ss to sΨs_{\Psi}. The algebraic line bundle LL defines an analytic line bundle LanL^{{\text{\rm an}}} on XΣanX_{\Sigma}^{{\text{\rm an}}}. Let L¯=(L,∥⋅∥){\overline{L}}=(L,\|\cdot\|), where ∥⋅∥\|\cdot\| is a metric on LanL^{{\text{\rm an}}}.

Every toric object has a certain invariance property with respect to the action of 𝕋\mathbb{T}. This is also the case for metrics. Since 𝕋an\mathbb{T}^{{\text{\rm an}}} is non compact, we can not ask for a metric to be 𝕋an\mathbb{T}^{{\text{\rm an}}}-invariant, but we can impose 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariance. We need a preliminary result.

Proposition 5.11.

Let LL be a toric line bundle on XΣX_{\Sigma} and let ∥⋅∥\|\cdot\| be a metric on LanL^{{\text{\rm an}}}. If there is a toric section s0s_{0} such that the function p↦‖s0​(p)‖p\mapsto\|s_{0}(p)\| is 𝕊an\,\mathbb{S}^{{\text{\rm an}}}-invariant, then, for every toric section ss, the function p↦‖s⁡(p)‖p\mapsto\|s(p)\| is 𝕊an\,\mathbb{S}^{{\text{\rm an}}}-invariant.

Proof.

If ss and s′s^{\prime} are two toric sections, then there is an element m∈Mm\in M such that s′=χm​ss^{\prime}=\chi^{m}s. Since for any element t∈𝕊ant\in\mathbb{S}^{{\text{\rm an}}} we have |χm​(t)|=1|\chi^{m}(t)|=1, if the function ‖s⁡(p)‖\|s(p)\| is 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariant, then the function ‖s′​(p)‖=‖χm​(p)​s​(p)‖\|s^{\prime}(p)\|=\|\chi^{m}(p)s(p)\| is also 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariant. ∎

Definition 5.12.

Let LL be a toric line bundle on XΣX_{\Sigma}. A metric on LanL^{{\text{\rm an}}} is called toric if, for any toric section ss of LL over X0X_{0}, the function p⟼‖s⁡(p)‖p\longmapsto\|s(p)\| is 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariant.

To the metrized line bundle L¯{\overline{L}} and the section ss we associate the function gL¯,s:X0an→ℝg_{{\overline{L}},s}\colon X_{0}^{{\text{\rm an}}}\to\mathbb{R} given by gL¯,s​(p)=log⁡(‖s⁡(p)‖)/λKg_{{\overline{L}},s}(p)=\log(\|s(p)\|)/\lambda_{K}. In the Archimedean case, the function gL¯,sg_{{\overline{L}},s} is −1/2-1/2 times the usual Green function associated to the metrized line bundle L¯{\overline{L}} and the section ss. The metric ∥⋅∥\|\cdot\| is toric if and only if the function gL¯,sg_{{\overline{L}},s} is 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariant. In this case we can form the commutative diagram

(5.13) X0an\textstyle{X_{0}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}gL¯,s\scriptstyle{g_{{\overline{L}},s}}valK\scriptstyle{{\operatorname{val}}_{K}}ℝ\textstyle{\mathbb{R}}Nℝ\textstyle{N_{\mathbb{R}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

The dashed arrow exists as a continuous function because ρ0\rho_{0}, hence valK{\operatorname{val}}_{K}, is a proper surjective map and, by 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariance, gL¯,sg_{{\overline{L}},s} is constant along the fibres. This justifies the following definition.

Definition 5.14.

Let LL be a toric line bundle, ss a toric section of LL and let ∥⋅∥\|\cdot\| be a toric metric. Denote L¯=(L,∥⋅∥){\overline{L}}=(L,\|\cdot\|). We define the function ψL¯,s:Nℝ→ℝ\psi_{{\overline{L}},s}\colon N_{\mathbb{R}}\to\mathbb{R} by

(5.15) ψL¯,s​(u)=log⁡‖s⁡(p)‖λK\psi_{{\overline{L}},s}(u)=\frac{\log\|s(p)\|}{\lambda_{K}}

for any p∈X0anp\in X_{0}^{{\text{\rm an}}} with valK⁡(p)=u{\operatorname{val}}_{K}(p)=u. When the line bundle and the section are clear from the context, we will alternatively denote this function as ψ∥⋅∥\psi_{\|\cdot\|}.

Proposition 5.16.

Let Ψ\Psi be a virtual support function on Σ\Sigma, L=𝒪⁡(DΨ)L=\mathcal{O}(D_{\Psi}) and s=sΨs=s_{\Psi}. Then the correspondence ∥⋅∥↦ψ∥⋅∥\|\cdot\|\mapsto\psi_{\|\cdot\|} determines a bijection between the set of toric metrics on LanL^{{\text{\rm an}}} and the set of continuous functions ψ\psi on NℝN_{\mathbb{R}} with the property that ψ−Ψ\psi-\Psi can be extended to a continuous function on NΣN_{\Sigma}. The metric associated to a function ψ\psi will be denoted ∥⋅∥ψ\|\cdot\|_{\psi}.

Proof.

Let ∥⋅∥\|\cdot\| be a toric metric on LanL^{{\text{\rm an}}}. Since ss is a regular nowhere vanishing section on X0anX_{0}^{{\text{\rm an}}}, ψ∥⋅∥\psi_{\|\cdot\|} is a well defined continuous function on NℝN_{\mathbb{R}}. Let {mσ}\{m_{\sigma}\} be a set of defining vectors of Ψ\Psi. For each cone σ∈Σ\sigma\in\Sigma, the section χmσ​s\chi^{m_{\sigma}}s is a regular nowhere vanishing section on XσanX_{\sigma}^{{\text{\rm an}}}. Therefore log⁡(‖(χmσ​s)​(p)‖)\log(\|(\chi^{m_{\sigma}}s)(p)\|) is a continuous function on XσanX_{\sigma}^{{\text{\rm an}}} that is 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariant. So it defines a continuous function on Xσ​(ℝ≥0)X_{\sigma}(\mathbb{R}_{\geq 0}). By equation (5.4),

ψ∥⋅∥(val(p))−mσ(val(p))\displaystyle\psi_{\|\cdot\|}({\operatorname{val}}(p))-m_{\sigma}({\operatorname{val}}(p)) =1λK​(log⁡(‖s⁡(p)‖)−log⁡(|χ−mσ​(p)|))\displaystyle=\frac{1}{\lambda_{K}}\left(\log(\|s(p)\|)-\log(|\chi^{-m_{\sigma}}(p)|)\right)
=1λK​log⁡(‖(χmσ​s)​(p)‖).\displaystyle=\frac{1}{\lambda_{K}}\log(\|(\chi^{m_{\sigma}}s)(p)\|).

Therefore ψ∥⋅∥−mσ\psi_{\|\cdot\|}-m_{\sigma} extends to a continuous function on Nσ≃Xσ​(ℝ≥0)N_{\sigma}\simeq X_{\sigma}(\mathbb{R}_{\geq 0}). If we see that Ψ−mσ\Psi-m_{\sigma} extends also to a continuous function on NσN_{\sigma} we will be able to extend ψ∥⋅∥−Ψ\psi_{\|\cdot\|}-\Psi to a continuous function on NσN_{\sigma} for every σ∈Σ\sigma\in\Sigma and therefore to NΣN_{\Sigma}.

Let τ\tau be a face of σ\sigma and let u∈N​(τ)ℝu\in N(\tau)_{\mathbb{R}}. Let W⁡(τ,U,p)W(\tau,U,p) be a neighbourhood of uu as in (5.6). By taking UU small enough and pp big enough we can assume that W⁡(τ,U,p)∩NℝW(\tau,U,p)\cap N_{\mathbb{R}} is contained in the set of cones that have τ\tau as a face. Since Ψ\Psi and mσm_{\sigma} agree when restricted to σ\sigma (hence when restricted to τ\tau) it follows that, if w+t∈W⁡(τ,U,p)∩Nℝw+t\in W(\tau,U,p)\cap N_{\mathbb{R}} with w∈Uw\in U and t∈p+τt\in p+\tau, then (Ψ−mσ)​(w+t)(\Psi-m_{\sigma})(w+t) only depends on ww and not on tt. Hence it can be extended to a continuous function on the whole W⁡(τ,U,p)W(\tau,U,p). By moving τ\tau, uu, UU and pp we see that it can be extended to a continuous function on NσN_{\sigma}.

Let now ψ\psi be a function on NℝN_{\mathbb{R}} such that ψ−Ψ\psi-\Psi extends to a continuous function on NΣN_{\Sigma}. We define a toric metric ∥⋅∥ψ\|\cdot\|_{\psi} on LanL^{{\text{\rm an}}} over the set X0anX_{0}^{{\text{\rm an}}} by the formula

‖s⁡(p)‖ψ=exp⁡(λK​ψ​(valK⁡(p))).\|s(p)\|_{\psi}=\exp(\lambda_{K}\psi({\operatorname{val}}_{K}(p))).

Then, by the argument before, ψ−mσ\psi-m_{\sigma} extends to a continuous function on NσN_{\sigma}, which proves that ∥⋅∥ψ\|\cdot\|_{\psi} extends to a metric over XσanX_{\sigma}^{{\text{\rm an}}}. Varying σ∈Σ\sigma\in\Sigma we obtain that ∥⋅∥ψ\|\cdot\|_{\psi} extends to a metric over XΣanX_{\Sigma}^{{\text{\rm an}}}. ∎

Corollary 5.17.

For any toric metric ∥⋅∥\|\cdot\|, the function |ψ∥⋅∥−Ψ||\psi_{\|\cdot\|}-\Psi| is bounded.

Proof.

Since we are assuming that Σ\Sigma is complete, the space NΣ≃XΣ​(ℝ≥0)N_{\Sigma}\simeq X_{\Sigma}(\mathbb{R}_{\geq 0}) is compact. Thus the corollary follows from Proposition 5.16. ∎

Example 5.18.

With the notation in Example 3.65, consider the standard simplex Δn\Delta^{n} with fan Σ=ΣΔn\Sigma=\Sigma_{\Delta^{n}} and support function Ψ=ΨΔn\Psi=\Psi_{\Delta^{n}}. The corresponding toric variety is XΣ=ℙnX_{\Sigma}=\mathbb{P}^{n} with toric line bundle LΨ=𝒪⁡(1)L_{\Psi}=\mathcal{O}(1) and toric section sΨ=s∞s_{\Psi}=s_{\infty}.

  1. (1)

    The canonical metrics ∥⋅∥can\|\cdot\|_{{\operatorname{can}}} in examples 2.25 and 2.32 are toric and both correspond to the function ψ∥⋅∥can=Ψ\psi_{\|\cdot\|_{{\operatorname{can}}}}=\Psi.

  2. (2)

    The Fubini-Study metric ∥⋅∥FS\|\cdot\|_{{\operatorname{FS}}} in Example 2.2 is also toric and corresponds to the differentiable function ψ∥⋅∥FS=fFS\psi_{\|\cdot\|_{{\operatorname{FS}}}}=f_{{\operatorname{FS}}} introduced in Example 3.53.

Proposition 5.19.

The correspondence (L¯,s)↦ψL¯,s({\overline{L}},s)\mapsto\psi_{{\overline{L}},s} satisfies the following properties.

  1. (1)

    Let L¯i=(Li,∥⋅∥i){\overline{L}}_{i}=(L_{i},\|\cdot\|_{i}), i=1,2i=1,2, be toric line bundles equipped with toric metrics and let sis_{i} be a toric section of LiL_{i}. Then

    ψL¯1⊗L¯2,s1⊗s2=ψL¯1,s1+ψL¯2,s2.\psi_{{\overline{L}}_{1}\otimes{\overline{L}}_{2},s_{1}\otimes s_{2}}=\psi_{{\overline{L}}_{1},s_{1}}+\psi_{{\overline{L}}_{2},s_{2}}.
  2. (2)

    Let L¯=(L,∥⋅∥){\overline{L}}=(L,\|\cdot\|) be a toric line bundle equipped with a toric metric and let ss be a toric section of LL. Then

    ψL¯−1,s−1=−ψL¯,s.\psi_{{\overline{L}}^{-1},s^{-1}}=-\psi_{{\overline{L}},s}.
Proof.

This follows easily from the definitions. ∎

A consequence of Proposition 5.16 is that every toric line bundle has a distinguished metric.

Proposition-Definition 5.20.

Let Σ\Sigma be a complete fan, XΣX_{\Sigma} the corresponding toric variety, and LL a toric line bundle on XΣX_{\Sigma}. Let ss be a toric section of LL and Ψ\Psi the virtual support function on Σ\Sigma associated to (L,s)(L,s) by theorems 4.22 and 4.18. The metric on LanL^{{\text{\rm an}}} associated to the function Ψ\Psi by Proposition 5.16 only depends on the structure of toric line bundle of LL. This metric is called the canonical metric of LanL^{{\text{\rm an}}} and is denoted ∥⋅∥can\|\cdot\|_{{\operatorname{can}}}. We write L¯can=(L,∥⋅∥can){\overline{L}}^{{\operatorname{can}}}=(L,\|\cdot\|_{{\operatorname{can}}}).

Proof.

Let s′s^{\prime} be another toric section of LL. Then there is an element m∈Mm\in M such that s′=χm​ss^{\prime}=\chi^{m}s. The corresponding virtual support function is Ψ′=Ψ−m\Psi^{\prime}=\Psi-m. Denote by ∥⋅∥\|\cdot\| and ∥⋅∥′\|\cdot\|^{\prime} the metrics associated to s,Ψs,\Psi and to s′,Ψ′s^{\prime},\Psi^{\prime} respectively. Then

‖s⁡(p)‖′=‖χ−m​s′​(p)‖′=eλK​(m+Ψ′)​(val⁡(p))=eλK​Ψ​(val⁡(p))=‖s⁡(p)‖.\|s(p)\|^{\prime}=\|\chi^{-m}s^{\prime}(p)\|^{\prime}=\operatorname{e}^{\lambda_{K}(m+\Psi^{\prime})({\operatorname{val}}(p))}=\operatorname{e}^{\lambda_{K}\Psi({\operatorname{val}}(p))}=\|s(p)\|.

Thus both metrics agree. ∎

The canonical metrics ∥⋅∥can\|\cdot\|_{{\operatorname{can}}} in examples 2.25 and 2.32 are particular cases of the canonical metric of Proposition-Definition 5.20.

Proposition 5.21.

The canonical metric is compatible with the tensor product of line bundles.

  1. (1)

    Let LiL_{i}, i=1,2i=1,2, be toric line bundles. Then L1⊗L2¯can=L1¯can⊗L2¯can{\overline{L_{1}\otimes L_{2}}}^{{\operatorname{can}}}={\overline{L_{1}}}^{{\operatorname{can}}}\otimes{\overline{L_{2}}}^{{\operatorname{can}}}.

  2. (2)

    Let LL be a toric line bundle. Then L−1¯can=(L¯can)−1{\overline{L^{-1}}}^{{\operatorname{can}}}=({\overline{L}}^{{\operatorname{can}}})^{-1}.

Proof.

This follows easily from the definitions. ∎

Next we describe the behaviour of the correspondence of Proposition 5.16 with respect to equivariant morphisms. We start with the case of orbits. Let Σ\Sigma be a complete fan in NN and Ψ\Psi a virtual support function on Σ\Sigma. Let LL and ss be the associated toric line bundle and toric section, and {mσ}σ∈Σ\{m_{\sigma}\}_{\sigma\in\Sigma} a set of defining vectors of Ψ\Psi. Let σ∈Σ\sigma\in\Sigma and let V⁡(σ)V(\sigma) be the corresponding closed subvariety. As in Proposition 4.34, the restriction of LL to V⁡(σ)V(\sigma) is a toric line bundle. Since V⁡(σ)V(\sigma) and div⁡(s)\operatorname{div}(s) may not intersect properly we can not restrict ss directly to V⁡(σ)V(\sigma). By contrast, DΨ−mσ=div⁡(χmσ​s)D_{\Psi-m_{\sigma}}=\operatorname{div}(\chi^{m_{\sigma}}s) intersects properly V⁡(σ)V(\sigma) and we can restrict the section χmσ​s\chi^{m_{\sigma}}s to V⁡(σ)V(\sigma) to obtain a toric section of 𝒪⁡(D(Ψ−mσ)​(σ))≃L∣V⁡(σ)\mathcal{O}(D_{(\Psi-m_{\sigma})(\sigma)})\simeq L\mid_{V(\sigma)}. Denote ι:V⁡(σ)→XΣ\iota\colon V(\sigma)\to X_{\Sigma} the closed immersion. For short, we write s′=χmσ​ss^{\prime}=\chi^{m_{\sigma}}s. Then ι∗​s′\iota^{\ast}s^{\prime} is a nowhere vanishing section on O⁡(σ)O(\sigma). Recall that V⁡(σ)V(\sigma) has a structure of toric variety given by the fan Σ⁡(σ)\Sigma(\sigma) on N⁡(σ)N(\sigma) (Proposition 4.6). The principal open subset of V⁡(σ)V(\sigma) is the orbit O⁡(σ)O(\sigma).

Let ∥⋅∥\|\cdot\| be a toric metric on LanL^{{\text{\rm an}}} and write L¯=(L,∥⋅∥){\overline{L}}=(L,\|\cdot\|). By the proof of Proposition 5.16, the function ψL¯,s−mσ=ψL¯,s′\psi_{{\overline{L}},s}-m_{\sigma}=\psi_{{\overline{L}},s^{\prime}} can be extended to a continuous function on NσN_{\sigma} that we denote ψ¯L¯,s′{\overline{\psi}}_{{\overline{L}},s^{\prime}}.

Proposition 5.22.

The function ψι∗​L¯,ι∗​s′:N​(σ)ℝ→ℝ\psi_{\iota^{\ast}{\overline{L}},\iota^{\ast}s^{\prime}}\colon N(\sigma)_{\mathbb{R}}\to\mathbb{R} agrees with the restriction of ψ¯L¯,s′{\overline{\psi}}_{{\overline{L}},s^{\prime}} to N​(σ)ℝ⊂NσN(\sigma)_{\mathbb{R}}\subset N_{\sigma}.

Proof.

The section s′s^{\prime} is a nowhere vanishing section over XΣ,σX_{\Sigma,\sigma}. Therefore, the function gL¯,s′:XΣ,σan→ℝg_{{\overline{L}},s^{\prime}}\colon X^{{\text{\rm an}}}_{\Sigma,\sigma}\to\mathbb{R} of diagram (5.13) can be extended to a continuous function on XΣ,σX_{\Sigma,\sigma} that we also denote gL¯,s′g_{{\overline{L}},s^{\prime}}. By the definition of the inverse image of a metric, there is a commutative diagram

O​(σ)an\textstyle{O(\sigma)^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ι\scriptstyle{\iota}gι∗​L¯,ι∗​s′\scriptstyle{g_{\iota^{\ast}{\overline{L}},\iota^{\ast}s^{\prime}}}XΣ,σan\textstyle{X^{{\text{\rm an}}}_{\Sigma,\sigma}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}gL¯,s′\scriptstyle{g_{{\overline{L}},s^{\prime}}}ℝ\textstyle{\mathbb{R}}

Then the result is a consequence of the definition of ψι∗​L¯,ι∗​s′\psi_{\iota^{\ast}{\overline{L}},\iota^{\ast}s^{\prime}} and of the commutativity of the diagram

O​(σ)an\textstyle{O(\sigma)^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}XΣ,σan\textstyle{X_{\Sigma,\sigma}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}N​(σ)ℝ\textstyle{N(\sigma)_{\mathbb{R}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Nσ,\textstyle{N_{\sigma},}

that follows from Proposition 5.9. ∎

Corollary 5.23.

Let L¯{\overline{L}} be a toric line bundle on XΣX_{\Sigma} equipped with the canonical metric, let σ∈Σ\sigma\in\Sigma and ι:V⁡(σ)→XΣ\iota\colon V(\sigma)\to X_{\Sigma} the closed immersion. Then the restriction ι∗​L¯\iota^{\ast}{\overline{L}} is a toric line bundle equipped with the canonical metric.

Proof.

Choose a toric section ss of LL whose divisor meets V⁡(σ)V(\sigma) properly. Let Ψ\Psi be the corresponding virtual support function. The condition of proper intersection is equivalent to Ψ|σ=0\Psi|_{\sigma}=0. Then Ψ\Psi extends to a continuous function Ψ¯{\overline{\Psi}} on NσN_{\sigma} and the restriction of Ψ¯→N⁡(σ){\overline{\Psi}}\to N(\sigma) is equal to Ψ⁡(σ)\Psi(\sigma). Hence the result follows from Proposition 5.22. ∎

We end with the case of an equivariant morphism whose image intersect the principal open subset. Let NiN_{i}, Σi\Sigma_{i}, i=1,2i=1,2, HH, pp and AA be as in Proposition 5.10. Let Ψ2\Psi_{2} be a virtual support function on Σ2\Sigma_{2} and let Ψ1=Ψ2∘H\Psi_{1}=\Psi_{2}\circ H. This is a virtual support function on Σ1\Sigma_{1}. Let (Li,si)(L_{i},s_{i}) be the corresponding toric line bundles and sections. By Proposition 4.35 and Theorem 4.22, there is an isomorphism φp.H∗​L2≃L1\varphi_{p.H}^{\ast}L_{2}\simeq L_{1} that sends φp.H∗​s2\varphi_{p.H}^{\ast}s_{2} to s1s_{1}. We use this isomorphism to identify them. Let ∥⋅∥\|\cdot\| be a toric metric on L2anL_{2}^{{\text{\rm an}}} and write L¯2=(L2,∥⋅∥){\overline{L}}_{2}=(L_{2},\|\cdot\|), L¯1=(L1,φp.H∗∥⋅∥){\overline{L}}_{1}=(L_{1},\varphi_{p.H}^{\ast}\|\cdot\|). The following result follows from Proposition 5.10 and is left to the reader.

Proposition 5.24.

The equality ψL¯1,s1=ψL¯2,s2∘A\psi_{{\overline{L}}_{1},s_{1}}=\psi_{{\overline{L}}_{2},s_{2}}\circ A holds.

In the case of toric morphism, the canonical metric is stable by inverse image. The following result follows easily from the definitions.

Corollary 5.25.

Assume furthermore that p=x0p=x_{0} and so the equivariant morphism φp,H=φH:XΣ1→XΣ2\varphi_{p,H}=\varphi_{H}\colon X_{\Sigma_{1}}\to X_{\Sigma_{2}} is a toric morphism. If L¯{\overline{L}} is a toric line bundle on XΣ2X_{\Sigma_{2}} equipped with the canonical metric, then φH∗​L¯\varphi_{H}^{\ast}{\overline{L}} is a toric line bundle equipped with the canonical metric.

The inverse image of the canonical metric by an equivariant map does not need to be the canonical metric. In fact, the analogue of Example 4.109 in terms of metrics shows that many different metrics can be obtained as the inverse image of the canonical metric on the projective space.

Example 5.26.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and XΣX_{\Sigma} the corresponding toric variety. Recall the description of the projective space ℙr\mathbb{P}^{r} as a toric variety given in Example 4.3. Let H:N→ℤrH\colon N\to\mathbb{Z}^{r} be a linear map such that, for each σ∈Σ\sigma\in\Sigma there exist τ∈ΣΔr\tau\in\Sigma_{\Delta^{r}} with H⁡(σ)⊂τH(\sigma)\subset\tau. Let p∈ℙ0r​(K)p\in\mathbb{P}^{r}_{0}(K). Then we have an equivariant morphism φp,H:XΣ→ℙr\varphi_{p,H}\colon X_{\Sigma}\to\mathbb{P}^{r}. Consider the support function ΨΔr\Psi_{\Delta^{r}} on ΣΔr\Sigma_{\Delta^{r}}. Then LΨΔr=𝒪ℙr​(1)L_{\Psi_{\Delta^{r}}}=\mathcal{O}_{\mathbb{P}^{r}}(1). Write L=φp,H∗​LΨΔrL=\varphi^{\ast}_{p,H}L_{\Psi_{\Delta^{r}}}, s=φp,H∗​sΨΔrs=\varphi^{\ast}_{p,H}s_{\Psi_{\Delta^{r}}} and Ψ=H∗​ΨΔr\Psi=H^{\ast}\Psi_{\Delta^{r}}. Thus (L,s)=(LΨ,sΨ)(L,s)=(L_{\Psi},s_{\Psi}).

Set A=H+valK⁡(p)A=H+{\operatorname{val}}_{K}(p) for the affine map. Let ∥⋅∥\|\cdot\| be the metric on LanL^{{\text{\rm an}}} induced by the canonical metric of 𝒪​(DΨΔr)an\mathcal{O}(D_{\Psi_{\Delta^{r}}})^{{\text{\rm an}}} and let ψ\psi be the function associated to it by Proposition 5.16. By Proposition 5.24, ψ=A∗​ΨΔr\psi=A^{\ast}\Psi_{\Delta^{r}}. This is a piecewise affine concave function on NℝN_{\mathbb{R}} with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi that can be made explicit as follows.

Let {e1,…,er}\{e_{1},\dots,e_{r}\} be the standard basis of ℤr\mathbb{Z}^{r} and let {e1∨,…,er∨}\{e_{1}^{\vee},\dots,e_{r}^{\vee}\} be the dual basis. Write mi=ei∨∘H∈Mm_{i}=e_{i}^{\vee}\circ H\in M and li=ei∨​(valK⁡(p))∈ℝl_{i}=e_{i}^{\vee}({\operatorname{val}}_{K}(p))\in\mathbb{R}. Then

Ψ\displaystyle\Psi =min⁡{0,m1,…,mr}\displaystyle=\min\{0,m_{1},\dots,m_{r}\}
ψ\displaystyle\psi =min⁡{0,m1+l1,…,mr+lr}\displaystyle=\min\{0,m_{1}+l_{1},\dots,m_{r}+l_{r}\}

We want to characterize all the functions that can be obtained with a slight generalization of the previous construction.

Proposition 5.27.

Let Σ\Sigma be a complete fan in NN and Ψ\Psi a support function on Σ\Sigma. Write L=LΨL=L_{\Psi} and s=sΨs=s_{\Psi}. Let ψ:Nℝ→ℝ\psi\colon N_{\mathbb{R}}\to\mathbb{R} a piecewise affine concave function with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi, that has an HH-representation

ψ=mini=0,…,r⁡{mi+li},\psi=\min_{i=0,\dots,r}\{m_{i}+l_{i}\},

with mi∈Mℚm_{i}\in M_{\mathbb{Q}} and li∈ℝl_{i}\in\mathbb{R} in the Archimedean case and li∈ℚl_{i}\in\mathbb{Q} in the non-Archimedean case. Then there is an equivariant morphism φ:XΣ→ℙr\varphi\colon X_{\Sigma}\to\mathbb{P}^{r}, an integer e>0e>0 and an isomorphism L⊗e≃φ∗​𝒪​(1)L^{\otimes e}\simeq\varphi^{\ast}\mathcal{O}(1) such that the metric induced on LanL^{{\text{\rm an}}} by the canonical metric of 𝒪​(1)an\mathcal{O}(1)^{{\text{\rm an}}} agrees with ∥⋅∥ψ\|\cdot\|_{\psi}.

Proof.

First observe that the condition li∈ℝl_{i}\in\mathbb{R} in the Archimedean case and li∈ℚl_{i}\in\mathbb{Q} in the non-Archimedean case is equivalent to the condition li∈ℚ​valK⁡(K×)l_{i}\in\mathbb{Q}\,{\operatorname{val}}_{K}(K^{\times}). Let e>0e>0 be an integer such that e​mi∈Mem_{i}\in M and e​li∈valK⁡(K×)el_{i}\in{\operatorname{val}}_{K}(K^{\times}) for i=0,…,ri=0,\dots,r.

Consider the linear map H:Nℝ→ℝrH\colon N_{\mathbb{R}}\to\mathbb{R}^{r} given by H⁡(u)=(e​mi​(u)−e​m0​(u))i=1,…,rH(u)=(em_{i}(u)-em_{0}(u))_{i=1,\dots,r} and the affine map A=H+𝒍A=H+\boldsymbol{l} with 𝒍=(e​li−e​l0)i=1,…,r\boldsymbol{l}=(el_{i}-el_{0})_{i=1,\dots,r}. By Lemma 3.79,

e​ψ=A∗​ΨΔr+e​m0+e​l0.e\psi=A^{\ast}\Psi_{\Delta^{r}}+em_{0}+el_{0}.

We claim that, for each σ∈Σ\sigma\in\Sigma there exists σi0∈ΣΔr\sigma_{i_{0}}\in\Sigma_{\Delta^{r}} such that H⁡(σ)⊂σi0H(\sigma)\subset\sigma_{i_{0}}. Indeed, Ψ⁡(u)=mini⁡{mi​(u)}\Psi(u)=\min_{i}\{m_{i}(u)\}. Since Ψ\Psi is a support function on Σ\Sigma, for each σ∈Σ\sigma\in\Sigma, there exists an i0i_{0} such that Ψ​(u)=mi0​(u)\Psi(u)=m_{i_{0}}(u) for all u∈σu\in\sigma. Writing e0∨=0e_{0}^{\vee}=0, this condition implies

min0≤i≤r⁡{ei∨​(H⁡(u))}=ei0∨​(H⁡(u))for all ​u∈σ.\min_{0\leq i\leq r}\{e_{i}^{\vee}(H(u))\}=e_{i_{0}}^{\vee}(H(u))\quad\text{for all }u\in\sigma.

Hence, H⁡(σ)⊂σi0H(\sigma)\subset\sigma_{i_{0}}, where σi0∈ΣΔr\sigma_{i_{0}}\in\Sigma_{\Delta^{r}} is the cone {v|min0≤i≤r⁡{ei∨​(v)}=ei0∨​(v)}\{v|\min_{0\leq i\leq r}\{e_{i}^{\vee}(v)\}=e_{i_{0}}^{\vee}(v)\} and the claim is proved.

Therefore, we can apply Theorem 4.9 and given a point p∈ℙrr​(K)p\in\mathbb{P}^{r}_{r}(K) such that valK⁡(p)=𝒍{\operatorname{val}}_{K}(p)=\boldsymbol{l}, there is an equivariant map φp,H:XΣ→ℙr\varphi_{p,H}\colon X_{\Sigma}\to\mathbb{P}^{r}. By Example 4.44, there is an isomorphism L⊗e≃φp,H∗​𝒪​(1)L^{\otimes e}\simeq\varphi_{p,H}^{*}\mathcal{O}(1) and a∈K×a\in K^{\times} with valK⁡(a)=l0{\operatorname{val}}_{K}(a)=l_{0} such that (a−1​χ−m0​s)⊗e(a^{-1}\chi^{-m_{0}}s)^{\otimes e} corresponds to φp,H∗​(sΨΔr)\varphi_{p,H}^{*}(s_{\Psi_{\Delta^{r}}}).

Let L¯{\overline{L}} be the line bundle LL equipped with the metric induced by the above isomorphism and the canonical metric of 𝒪​(1)an\mathcal{O}(1)^{{\text{\rm an}}}. Then

ψL¯,s=ψL¯,a−1​χ−m0​s+m0+l0=1e​A∗​ΨΔr+m0+l0=ψ,\psi_{{\overline{L}},s}=\psi_{{\overline{L}},a^{-1}\chi^{-m_{0}}s}+m_{0}+l_{0}=\frac{1}{e}A^{\ast}\Psi_{\Delta^{r}}+m_{0}+l_{0}=\psi,

as stated. ∎

Corollary 5.28.

Let ψ\psi be as in Proposition 5.27. Then the metric ∥⋅∥ψ\|\cdot\|_{\psi} is approachable.

Proof.

This follows readily from the previous result together with Example 2.32 in the Archimedean case and Example 2.25 in the non-Archimedean case and the fact that the inverse image of an approachable metric is also approachable. ∎

5.3. Smooth metrics and their associated measures

We now discuss the relationship between semipositivity of smooth metrics and concavity of the associated function in the Archimedean case. Moreover we will determine the associated measure.

In this section KK is either ℝ\mathbb{R} or ℂ\mathbb{C} and we fix a lattice NN of rank nn, a complete fan Σ\Sigma in NℝN_{\mathbb{R}} and a virtual support function Ψ\Psi on Σ\Sigma, with LL and ss the corresponding toric line bundle and section. Let XΣanX_{\Sigma}^{{\text{\rm an}}} be the complex analytic space associated to XΣX_{\Sigma} and LanL^{{\text{\rm an}}} the analytic line bundle associated to LL.

Proposition 5.29.

Let ∥⋅∥\|\cdot\| be a smooth toric metric on LanL^{{\text{\rm an}}}. Then ∥⋅∥\|\cdot\| is semipositive if and only if the function ψ=ψ∥⋅∥\psi=\psi_{\|\cdot\|} is concave.

Proof.

Since the condition of being semipositive is closed, it is enough to check it in the open set X0anX_{0}^{{\text{\rm an}}}. We choose an integral basis of M=N∨M=N^{\vee}. This determines isomorphisms

X0an≃(ℂ×)n,X0​(ℝ≥0)≃(ℝ>0)n,Nℂ≃ℂn,Nℝ≃ℝn.X_{0}^{{\text{\rm an}}}\simeq(\mathbb{C}^{\times})^{n},\quad X_{0}(\mathbb{R}_{\geq 0})\simeq(\mathbb{R}_{>0})^{n},\quad N_{\mathbb{C}}\simeq\mathbb{C}^{n},\quad N_{\mathbb{R}}\simeq\mathbb{R}^{n}.

Let z1,…,znz_{1},\dots,z_{n} be the coordinates of X0anX_{0}^{{\text{\rm an}}} and u1,…,unu_{1},\dots,u_{n} the coordinates of NℝN_{\mathbb{R}} determined by these isomorphisms. With these coordinates the map

val:X0an→Nℝ{\operatorname{val}}\colon X_{0}^{{\text{\rm an}}}\to N_{\mathbb{R}}

is given by

val⁡(z1,…,zn)=−12​(log⁡(z1​z¯1),…,log⁡(zn​z¯n)).{\operatorname{val}}(z_{1},\dots,z_{n})=\frac{-1}{2}(\log(z_{1}\bar{z}_{1}),\dots,\log(z_{n}\bar{z}_{n})).

As usual, we denote L¯=(L,∥⋅∥){\overline{L}}=(L,\|\cdot\|). Set g=gL¯,s=log⁡‖s‖g=g_{{\overline{L}},s}=\log\|s\|. Then, the integral valued first Chern class is given by

(5.30) 12​π​i​c1​(L¯)=1π​i​∂∂¯​g=−iπ​∑k,l∂2g∂zk​∂z¯l​d​zk∧d​z¯l.\frac{1}{2\pi i}c_{1}(\overline{L})=\frac{1}{\pi i}\partial\bar{\partial}g=\frac{-i}{\pi}\sum_{k,l}\frac{\partial^{2}g}{\partial z_{k}\partial\bar{z}_{l}}\,\text{\rm d}z_{k}\land\,\text{\rm d}\bar{z}_{l}.

The standard orientation of the unit disk 𝔻⊂ℂ\mathbb{D}\subset\mathbb{C} is given by d​x∧d​y=(i/2)​d​z∧d​z¯\,\text{\rm d}x\land\,\text{\rm d}y=(i/2)\,\text{\rm d}z\land\,\text{\rm d}\bar{z}. Hence, the metric of L¯{\overline{L}} is semipositive if and only if the matrix G=(∂2g∂zk​∂z¯l)k,lG=(\frac{\partial^{2}g}{\partial z_{k}\partial\bar{z}_{l}})_{k,l} is semi-negative definite. Since

(5.31) ∂2g∂zk​∂z¯l=14​zk​z¯l​∂2ψ∂uk​∂u¯l,\frac{\partial^{2}g}{\partial z_{k}\partial\bar{z}_{l}}=\frac{1}{4z_{k}\bar{z}_{l}}\frac{\partial^{2}\psi}{\partial u_{k}\partial\bar{u}_{l}},

if we write Hess⁡(ψ)=(∂2ψ∂uk​∂u¯l)k,l\operatorname{Hess}(\psi)=(\frac{\partial^{2}\psi}{\partial u_{k}\partial\bar{u}_{l}})_{k,l} and Z=diag⁡((2​z1)−1,…,(2​zn)−1)Z=\operatorname{diag}((2z_{1})^{-1},\dots,(2z_{n})^{-1}), then G=Z¯t​Hess⁡(ψ)​ZG=\bar{Z}^{t}\operatorname{Hess}(\psi)Z. Therefore GG is semi-negative definite if and only if Hess⁡(ψ)\operatorname{Hess}(\psi) is semi-negative definite, hence, if and only if ψ\psi is concave. ∎

The line bundle LanL^{{\text{\rm an}}} admits a semipositive metric is and only if Ψ\Psi is concave. Thus, from now on we assume that Ψ\Psi is a support function, that is, a concave support function.

Definition 5.32.

Let ψ:Nℝ→ℝ\psi\colon N_{\mathbb{R}}\to\mathbb{R} be a concave function such that |Ψ−ψ||\Psi-\psi| is bounded. Let ℳM​(ψ)\mathcal{M}_{M}(\psi) be the Monge-Ampère measure associated to ψ\psi and the lattice MM. We will denote by ℳ¯M​(ψ){\overline{\mathcal{M}}}_{M}(\psi) the measure on NΣN_{\Sigma} given by

ℳ¯M​(ψ)​(E)=ℳM​(ψ)​(E∩Nℝ){\overline{\mathcal{M}}}_{M}(\psi)(E)=\mathcal{M}_{M}(\psi)(E\cap N_{\mathbb{R}})

for any Borel subset of NΣN_{\Sigma}.

By its very definition, the measure ℳ¯M​(ψ){\overline{\mathcal{M}}}_{M}(\psi) is bounded with total mass

ℳ¯M​(ψ)​(NΣ)=volM⁡(ΔΨ){\overline{\mathcal{M}}}_{M}(\psi)(N_{\Sigma})=\operatorname{vol}_{M}(\Delta_{\Psi})

and the set NΣ∖NℝN_{\Sigma}\setminus N_{\mathbb{R}} has measure zero.

Theorem 5.33.

Let ∥⋅∥\|\cdot\| be a semipositive smooth toric metric on LanL^{{\text{\rm an}}}. Let c1​(L¯)n∧δXΣc_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}} be the measure defined by L¯{\overline{L}}. Then,

(5.34) val∗⁡(c1​(L¯)n∧δXΣ)=n!​ℳ¯M​(ψ),{\operatorname{val}}_{\ast}(c_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}})=n!{\overline{\mathcal{M}}}_{M}(\psi),

where val{\operatorname{val}} is the map of diagram (5.7). In addition, this measure is uniquely characterized by equation (5.34) and the property of being 𝕊an\mathbb{S}^{{\text{\rm an}}}-invariant.

Proof.

Since the measure c1​(L¯)n∧δXΣc_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}} is given by a smooth volume form and XΣan∖X0anX^{{\text{\rm an}}}_{\Sigma}\setminus X^{{\text{\rm an}}}_{0} is a set of Lebesgue measure zero, the measure c1​(L¯)n∧δXΣc_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}} is determined by its restriction to the dense open subset X0anX_{0}^{{\text{\rm an}}}. Thus, to prove equation (5.34) it is enough to show that

(5.35) val∗⁡(c1​(L¯)n∧δXΣ|X0an)=n!​ℳM​(ψ).{\operatorname{val}}_{\ast}(c_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}}|_{X^{{\text{\rm an}}}_{0}})=n!\mathcal{M}_{M}(\psi).

We use the coordinate system of the proof of Proposition 5.29. We denote by 𝐞~:Nℂ→X0​(ℂ){\widetilde{{\operatorname{\mathbf{e}}}}}\colon N_{\mathbb{C}}\to X_{0}(\mathbb{C}) the map induced by the morphism ℂ→ℂ×\mathbb{C}\to\mathbb{C}^{\times} given by z↦exp⁡(−z)z\mapsto\exp(-z). We write uk+i​vku_{k}+iv_{k} for the complex coordinates of NℂN_{\mathbb{C}}. Then

(5.36) 𝐞~∗​(d​zk∧d​z¯kzk​z¯k)=(−2​i)​d​uk∧d​vk.{\widetilde{{\operatorname{\mathbf{e}}}}}^{\ast}\left(\frac{\,\text{\rm d}z_{k}\land\,\text{\rm d}\bar{z}_{k}}{z_{k}\bar{z}_{k}}\right)=(-2i)\,\text{\rm d}u_{k}\land\,\text{\rm d}v_{k}.

Using now equations (5.30), (5.31) and (5.36), we obtain that,

1(2​π​i)n​𝐞~∗​c1​(L¯)n\displaystyle\frac{1}{(2\pi i)^{n}}{\widetilde{{\operatorname{\mathbf{e}}}}}^{\ast}c_{1}({\overline{L}})^{n} =𝐞~∗​(1(i​π)n​n!​detG​d​z1∧d​z¯1∧⋯∧d​zn∧d​z¯n)\displaystyle={\widetilde{{\operatorname{\mathbf{e}}}}}^{\ast}\left(\frac{1}{(i\pi)^{n}}n!\det G\,\text{\rm d}z_{1}\land\,\text{\rm d}\bar{z}_{1}\land\dots\land\,\text{\rm d}z_{n}\land\,\text{\rm d}\bar{z}_{n}\right)
=(−1)n(2​π)n​n!​detHess⁡(ψ)​d​u1∧d​v1∧⋯∧d​un∧d​un.\displaystyle=\frac{(-1)^{n}}{(2\pi)^{n}}n!\det\operatorname{Hess}(\psi)\,\text{\rm d}u_{1}\land\,\text{\rm d}v_{1}\land\dots\land\,\text{\rm d}u_{n}\land\,\text{\rm d}u_{n}.

Since the map val{\operatorname{val}} is the composition of 𝐞~−1{\widetilde{{\operatorname{\mathbf{e}}}}}^{-1} with the projection Nℂ→NℝN_{\mathbb{C}}\to N_{\mathbb{R}}, integrating with respect to the variables v1,…,vnv_{1},\dots,v_{n} in the domain [0,2​π]n[0,2\pi]^{n}, taking into account the natural orientation of ℂn\mathbb{C}^{n} and the orientation of NℝN_{\mathbb{R}} given by the coordinate system, and the fact that the normalization factor 1/(2​π​i)n1/(2\pi i)^{n} is implicit in the current δXΣ\delta_{X_{\Sigma}}, we obtain

val∗⁡(c1​(L¯)n∧δXΣ|X0an)=(−1)n​n!​detHess⁡(ψ)​d​u1∧⋯∧d​un.{\operatorname{val}}_{\ast}(c_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}}|_{X_{0}^{{\text{\rm an}}}})=(-1)^{n}n!\det\operatorname{Hess}(\psi)\,\text{\rm d}u_{1}\land\dots\land\,\text{\rm d}u_{n}.

Thus equation (5.35) follows from Proposition 3.94. Finally, the last statement follows from the fact that, in a compact Abelian group there is a unique Haar measure with fixed total volume. ∎

We end this section recalling how to obtain a toric metric from a non-toric one. Let LL be a toric line bundle on the toric variety XΣX_{\Sigma} and let ss be a toric section. If ∥⋅∥\|\cdot\| is a smooth, non-necessarily toric, metric, we can average it to obtain a toric metric. This averaging process preserves smoothness and semipositivity. Let μHaar\mu_{\operatorname{Haar}} be the Haar measure of 𝕊an\mathbb{S}^{{\text{\rm an}}} of total volume 1. Then we define the metric ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} over X0anX_{0}^{{\text{\rm an}}} by

(5.37) log⁡‖s⁡(p)‖𝕊=∫𝕊anlog⁡‖s⁡(t⋅p)‖​d​μHaar​(t).\log\|s(p)\|_{\mathbb{S}}=\int_{\mathbb{S}^{{\text{\rm an}}}}\log\|s(t\cdot p)\|\,\text{\rm d}\mu_{\operatorname{Haar}}(t).
Proposition 5.38.

The metric ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} extends to a toric smooth metric over XΣanX^{{\text{\rm an}}}_{\Sigma}. Moreover, if ∥⋅∥\|\cdot\| is semipositive then ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} is semipositive.

Proof.

Let ∥⋅∥′\|\cdot\|^{\prime} be any toric smooth metric. Then ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} extends to a smooth metric if and only if log⁡(‖s‖𝕊/‖s‖′)\log(\|s\|_{\mathbb{S}}/\|s\|^{\prime}) can be extended to a smooth function on XΣanX_{\Sigma}^{{\text{\rm an}}}. But we have

log⁡(‖s‖𝕊/‖s‖′)=∫𝕊anlog⁡(‖s⁡(t⋅p)‖/‖s⁡(t⋅p)‖′)​d​μHaar​(t)\log(\|s\|_{\mathbb{S}}/\|s\|^{\prime})=\int_{\mathbb{S}^{{\text{\rm an}}}}\log(\|s(t\cdot p)\|/\|s(t\cdot p)\|^{\prime})\,\text{\rm d}\mu_{\operatorname{Haar}}(t)

and the right-hand side can be extended to a smooth function on the whole XΣanX_{\Sigma}^{{\text{\rm an}}}. Clearly the metric ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} is toric. Moreover

c1(L,∥⋅∥𝕊)=∫𝕊ant∗c1(L,∥⋅∥)dμHaar(t).c_{1}(L,\|\cdot\|_{\mathbb{S}})=\int_{\mathbb{S}^{{\text{\rm an}}}}t^{\ast}c_{1}(L,\|\cdot\|)\,\text{\rm d}\mu_{\operatorname{Haar}}(t).

Therefore, if (L,∥⋅∥)(L,\|\cdot\|) is semipositive, then (L,∥⋅∥𝕊)(L,\|\cdot\|_{\mathbb{S}}) is semipositive. ∎

5.4. Algebraic metrics from toric models

Next we study some properties of the algebraic metrics that arise from toric models. This kind of metrics will be called toric algebraic metrics. Thus, we assume that KK is a complete field with respect to an absolute value associated to a nontrivial discrete valuation. We keep the usual notations. We fix a complete fan Σ\Sigma in NℝN_{\mathbb{R}}.

We begin by studying the relationship between the maps val{\operatorname{val}} and red{\operatorname{red}}.

Lemma 5.39.

Let Π\Pi be a complete SCR polyhedral complex of NℝN_{\mathbb{R}} such that rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma. Let 𝒳:=𝒳Π{\mathcal{X}}:={\mathcal{X}}_{\Pi} be the model of XΣX_{\Sigma} determined by Π\Pi. Let Λ∈Π\Lambda\in\Pi and p∈X0anp\in X_{0}^{{\text{\rm an}}}. Then red⁡(p)∈𝒳Λ{\operatorname{red}}(p)\in{\mathcal{X}}_{\Lambda} if and only if valK⁡(p)∈Λ{\operatorname{val}}_{K}(p)\in\Lambda.

Proof.

By the definition of the semigroup M~Λ{\widetilde{M}}_{\Lambda}, the condition val⁡(p)∈Λ{\operatorname{val}}(p)\in\Lambda holds if and only in ⟨m,val⁡(p)⟩+l≥0\langle m,{\operatorname{val}}(p)\rangle+l\geq 0 for all (m,l)∈M~Λ(m,l)\in{\widetilde{M}}_{\Lambda}. This is equivalent to log⁡|χ−m​(p)|+log⁡|ϖ|−l≥0\log|\chi^{-m}(p)|+\log|\varpi|^{-l}\geq 0 for all (m,l)∈M~Λ(m,l)\in{\widetilde{M}}_{\Lambda}. In turn, this is equivalent to |χm​(p)​ϖl|≤1|\chi^{m}(p)\varpi^{l}|\leq 1, for all (m,l)∈M~Λ(m,l)\in{\widetilde{M}}_{\Lambda}. Hence, val⁡(p)∈Λ{\operatorname{val}}(p)\in\Lambda if and only if |a⁡(p)|≤1|a(p)|\leq 1 for all a∈K∘​[𝒳Λ]a\in K^{\circ}[{\mathcal{X}}_{\Lambda}], which is exactly the condition red⁡(p)∈𝒳Λ{\operatorname{red}}(p)\in{\mathcal{X}}_{\Lambda} (see (2.12)). ∎

Corollary 5.40.

With the same hypothesis as Lemma 5.39, red⁡(p)∈O⁡(Λ){\operatorname{red}}(p)\in O(\Lambda) if and only if val⁡(p)∈ri⁡(Λ){\operatorname{val}}(p)\in\operatorname{ri}(\Lambda).

Proof.

This follows from Lemma 5.39 and the fact that the special fibre is

𝒳Λ,o=∐Λ′​ face of ​ΛO⁡(Λ′),{\mathcal{X}}_{\Lambda,o}=\coprod_{\Lambda^{\prime}\text{ face of }\Lambda}O(\Lambda^{\prime}),

and ri(Λ)=Λ∖⋃Λ′ proper face of ΛΛ′\operatorname{ri}(\Lambda)=\Lambda\setminus\bigcup_{\Lambda^{\prime}\text{ proper face of }\Lambda}\Lambda^{\prime}. ∎

Let Ψ\Psi be a virtual support function on Σ\Sigma, and (L,s)(L,s) the corresponding toric line bundle and section. Let Π\Pi be a complete SCR polyhedral complex in NℝN_{\mathbb{R}} such that rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma and let ψ\psi be a rational piecewise affine function on Π\Pi with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi. Let e>0e>0 be an integer such that e​ψe\psi is an H-lattice function. By Theorem 4.81, the pair (Π,e​ψ)(\Pi,e\psi) determines a toric model (𝒳Π,ℒe​ψ,e)({\mathcal{X}}_{\Pi},{\mathcal{L}}_{e\psi},e) of (XΣ,L)(X_{\Sigma},L). We will write ℒ=ℒe​ψ{\mathcal{L}}={\mathcal{L}}_{e\psi}. Definition 2.17 gives us an algebraic metric ∥⋅∥ℒ\|\cdot\|_{{\mathcal{L}}} on LanL^{{\text{\rm an}}}. In its turn, the metric ∥⋅∥ℒ\|\cdot\|_{{\mathcal{L}}} defines a function ψ∥⋅∥ℒ\psi_{\|\cdot\|_{{\mathcal{L}}}}. The following proposition closes the circle.

Proposition 5.41.

The equality ψ∥⋅∥ℒ=ψ\psi_{\|\cdot\|_{{\mathcal{L}}}}=\psi holds. Hence ψ−Ψ\psi-\Psi extends to a continuous function on NΣN_{\Sigma} and the metric ∥⋅∥ψ\|\cdot\|_{\psi} associated to ψ\psi by Proposition 5.16 agrees with ∥⋅∥ℒ\|\cdot\|_{{\mathcal{L}}}.

Proof.

The tensor product s⊗es^{\otimes e} defines a rational section of ℒ{\mathcal{L}}. Let Λ∈Π\Lambda\in\Pi and choose mΛ∈Mm_{\Lambda}\in M, lΛ∈ℤl_{\Lambda}\in\mathbb{Z} such that e​ψ|Λ=mΛ+lΛ|Λe\psi|_{\Lambda}=m_{\Lambda}+l_{\Lambda}|_{\Lambda}. Let u∈Λu\in\Lambda and p∈XΣanp\in X^{{\text{\rm an}}}_{\Sigma} with u=val⁡(p)u={\operatorname{val}}(p). Then red⁡(p)∈𝒳Λ{\operatorname{red}}(p)\in{\mathcal{X}}_{\Lambda}. But in 𝒳Λ{\mathcal{X}}_{\Lambda} the section χmΛ​ϖlΛ​s⊗e\chi^{m_{\Lambda}}\varpi^{l_{\Lambda}}s^{\otimes e} is regular and non-vanishing. Therefore, by Definition 2.17,

‖χmΛ​(p)​ϖlΛ​s⊗e​(p)‖ℒ=1.\|\chi^{m_{\Lambda}}(p)\varpi^{l_{\Lambda}}s^{\otimes e}(p)\|_{{\mathcal{L}}}=1.

Thus

ψ∥⋅∥ℒ(u)\displaystyle\psi_{\|\cdot\|_{{\mathcal{L}}}}(u) =1λK​log⁡(‖s⁡(p)‖ℒ)\displaystyle=\frac{1}{\lambda_{K}}\log(\|s(p)\|_{{\mathcal{L}}})
=1e​λK​log⁡(|χ−mΛ​(p)​ϖ−lΛ|)\displaystyle=\frac{1}{e\lambda_{K}}\log(|\chi^{-m_{\Lambda}}(p)\varpi^{-l_{\Lambda}}|)
=1e​(⟨mΛ,u⟩+lΛ)\displaystyle=\frac{1}{e}(\langle m_{\Lambda},u\rangle+l_{\Lambda})
=ψ⁡(u).\displaystyle=\psi(u).

Therefore ψ\psi agrees with the function associated to the metric ∥⋅∥ℒ\|\cdot\|_{{\mathcal{L}}}. Hence ψ−Ψ\psi-\Psi extends to a continuous function on NΣN_{\Sigma} and the metric ∥⋅∥ψ\|\cdot\|_{\psi} agrees with ∥⋅∥ℒ\|\cdot\|_{{\mathcal{L}}}. ∎

Example 5.42.

In the non-Archimedean case, the canonical metric of Proposition-Definition 5.20 is the toric algebraic metric induced by the canonical model of Definition 4.76.

Proposition 5.41 imposes a necessary condition for a rational piecewise affine function to determine a model of (XΣ,LΨ)(X_{\Sigma},L_{\Psi}).

Corollary 5.43.

Let Ψ\Psi be a virtual support function on Σ\Sigma and let ψ\psi be a rational piecewise affine function on NℝN_{\mathbb{R}}, with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi, such that there exists a complete SCR polyhedral complex Π\Pi with rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma and ψ\psi piecewise affine on Π\Pi. Then ψ−Ψ\psi-\Psi can be extended to a continuous function on NΣN_{\Sigma}.

Proof.

If there exists such a SCR polyhedral complex Π\Pi, then Π\Pi and ψ\psi determine a model of 𝒪⁡(DΨ)\mathcal{O}(D_{\Psi}) and hence a toric algebraic metric ∥⋅∥\|\cdot\|. By Proposition 5.41, ψ=ψ∥⋅∥\psi=\psi_{\|\cdot\|} and, by the classification of toric metrics in Proposition 5.16, the function ψ∥⋅∥−Ψ\psi_{\|\cdot\|}-\Psi extends to a continuous function on NΣN_{\Sigma}. ∎

Example 5.44.

Let N=ℤ2N=\mathbb{Z}^{2} and consider the fan Σ\Sigma generated by e0=(−1,−1)e_{0}=(-1,-1), e1=(1,0)e_{1}=(1,0) and e2=(0,1)e_{2}=(0,1). Then XΣ=ℙ2X_{\Sigma}=\mathbb{P}^{2}. The virtual support function Ψ=0\Psi=0 corresponds to the trivial line bundle 𝒪ℙ2\mathcal{O}_{\mathbb{P}^{2}}. Consider the function

ψ⁡(x,y)={0, if ​x≤0,x, if ​0≤x≤1,1, if ​1≤x.\psi(x,y)=\begin{cases}0,&\text{ if }x\leq 0,\\ x,&\text{ if }0\leq x\leq 1,\\ 1,&\text{ if }1\leq x.\\ \end{cases}

Then rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi, but ψ\psi does not extend to a continuous function on NΣN_{\Sigma} and therefore it does not determine a model of (XΣ,𝒪)(X_{\Sigma},\mathcal{O}). By contrast, let Σ′\Sigma^{\prime} be the fan obtained subdividing Σ\Sigma by adding the edge corresponding to e′=(0,−1)e^{\prime}=(0,-1). Then XΣ′X_{\Sigma^{\prime}} is isomorphic to a blow-up of ℙ2\mathbb{P}^{2} at one point. The function ψ\psi extends to a continuous function on NΣ′N_{\Sigma^{\prime}} and it corresponds to a toric model of (XΣ′,𝒪)(X_{\Sigma^{\prime}},\mathcal{O}).

Question 5.45.

Is the condition in Corollary 5.43 also sufficient? In other words, let NN, Σ\Sigma and Ψ\Psi be as before and let ψ\psi be a rational piecewise affine function on NℝN_{\mathbb{R}} such that ψ−Ψ\psi-\Psi can be extended to a continuous function on NΣN_{\Sigma}. Does it exists a complete SCR polyhedral complex Π\Pi with rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma and ψ\psi is piecewise affine on Π\Pi?

Remark 5.46.

By the proof of Theorem 4.97 and Corollary 5.43, when ψ\psi is concave, the conditions

  1. (1)

    |ψ−Ψ||\psi-\Psi| is bounded;

  2. (2)

    ψ−Ψ\psi-\Psi can be extended to a continuous function on NΣN_{\Sigma};

  3. (3)

    there exist a complete SCR polyhedral complex Π\Pi with rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma and ψ\psi piecewise affine on Π\Pi;

are equivalent. In particular, the answer to the above question is positive when ψ\psi is concave.

By Theorem 4.97, a rational piecewise affine concave function ψ\psi with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi determines an equivalence class of semipositive toric models of (XΣ,K,LΨ)(X_{\Sigma,K},L_{\Psi}). As before, every toric model in this class defines an algebraic metric on LΨanL_{\Psi}^{{\text{\rm an}}}. Since, by Proposition 2.18, equivalent models give rise to the same metric, this metric only depends on ψ\psi. Then Proposition 5.41 has the following direct consequence.

Corollary 5.47.

Let Σ\Sigma be a complete fan and let Ψ\Psi be a support function on Σ\Sigma. Let ψ\psi be a rational piecewise affine concave function on NℝN_{\mathbb{R}} with rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi and let ∥⋅∥\|\cdot\| be the metric defined by any model of (XΣ,LΨ)(X_{\Sigma},L_{\Psi}) in the equivalence class determined by ψ\psi. Then the equality ψ∥⋅∥=ψ\psi_{\|\cdot\|}=\psi holds. So the metric ∥⋅∥\|\cdot\| agrees with the metric ∥⋅∥ψ\|\cdot\|_{\psi} of Proposition 5.16. Moreover, the algebraic metric ∥⋅∥\|\cdot\| is semipositive.

Proof.

The equation ψ∥⋅∥=ψ\psi_{\|\cdot\|}=\psi is just Proposition 5.41 in the concave case. By the definition of semipositive algebraic metrics and Theorem 4.95 we obtain that ψ\psi concave implies ∥⋅∥\|\cdot\| semipositive. ∎

We have seen that rational piecewise affine functions give rise to toric algebraic metrics. We now study the converse. Let gg be a rational function on XΣX_{\Sigma}. Then we denote by ψg:Nℝ→ℝ\psi_{g}\colon N_{\mathbb{R}}\to\mathbb{R} the function ψg​(u)=1λK​log⁡|g⁡(θ0​(𝐞λK⁡(u)))|\psi_{g}(u)=\frac{1}{\lambda_{K}}\log|g(\theta_{0}({\operatorname{\mathbf{e}}}_{\lambda_{K}}(u)))|.

Lemma 5.48.

Let gg be a rational function on XΣX_{\Sigma}. Then the function ψg\psi_{g} is an H-lattice function (Definition 3.88). In particular it is a piecewise affine function.

Proof.

The function gg can be written as g=∑m∈Mαm​χm∑m∈Mβm​χmg=\frac{\sum_{m\in M}\alpha_{m}\chi^{m}}{\sum_{m\in M}\beta_{m}\chi^{m}}. Then

ψg​(u)\displaystyle\psi_{g}(u) =1λK​log⁡|g⁡(θ0​(𝐞λK⁡(u)))|\displaystyle=\frac{1}{\lambda_{K}}\log|g(\theta_{0}({\operatorname{\mathbf{e}}}_{\lambda_{K}}(u)))|
=1λK​log⁡|∑m∈Mαm​χm​(θ0​(𝐞λK⁡(u)))​|−1λK​log|​∑m∈Mβm​χm​(θ0​(𝐞λK⁡(u)))|\displaystyle=\frac{1}{\lambda_{K}}\log\Bigl|\sum_{m\in M}\alpha_{m}\chi^{m}(\theta_{0}({\operatorname{\mathbf{e}}}_{\lambda_{K}}(u)))\Bigr|-\frac{1}{\lambda_{K}}\log\Bigl|\sum_{m\in M}\beta_{m}\chi^{m}(\theta_{0}({\operatorname{\mathbf{e}}}_{\lambda_{K}}(u)))\Bigr|
=maxm∈M⁡(log⁡|αm|λK−⟨m,u⟩)−maxm∈M⁡(log⁡|βm|λK−⟨m,u⟩)\displaystyle=\max_{m\in M}\Bigl(\frac{\log|\alpha_{m}|}{\lambda_{K}}-\left<m,u\right>\Bigr)-\max_{m\in M}\Bigl(\frac{\log|\beta_{m}|}{\lambda_{K}}-\left<m,u\right>\Bigr)
=maxm∈M⁡(−ord⁡(αm)−⟨m,u⟩)−maxm∈M⁡(−ord⁡(βm)−⟨m,u⟩)\displaystyle=\max_{m\in M}(-{\operatorname{ord}}(\alpha_{m})-\left<m,u\right>)-\max_{m\in M}(-{\operatorname{ord}}(\beta_{m})-\left<m,u\right>)
=minm∈M⁡(⟨m,u⟩+ord⁡(βm))−minm∈M⁡(⟨m,u⟩+ord⁡(αm)).\displaystyle=\min_{m\in M}(\left<m,u\right>+{\operatorname{ord}}(\beta_{m}))-\min_{m\in M}(\left<m,u\right>+{\operatorname{ord}}(\alpha_{m})).

Thus, it is the difference of two H-lattice concave functions. ∎

Theorem 5.49.

Let Σ\Sigma be a complete fan, Ψ\Psi a virtual support function on Σ\Sigma and (L,s)(L,s) the corresponding toric line bundle and section. Let ∥⋅∥\|\cdot\| be a toric algebraic metric on LanL^{{\text{\rm an}}}. Then the function ψ∥⋅∥\psi_{\|\cdot\|} is rational piecewise affine. If moreover ψ∥⋅∥\psi_{\|\cdot\|} is concave, the toric algebraic metric ∥⋅∥\|\cdot\| is semipositive and it comes from a toric model.

Proof.

Since the metric is algebraic, there exist a proper K∘K^{\circ}- scheme 𝒳\mathcal{X} and a line bundle ℒ\mathcal{L} on 𝒳\mathcal{X} such that the base change of (𝒳,ℒ)(\mathcal{X},\mathcal{L}) to KK is isomorphic to (XΣ,L⊗e)(X_{\Sigma},L^{\otimes e}). Let {𝒰i,si}\{{\mathcal{U}}_{i},s_{i}\} be a trivialization of ℒ\mathcal{L}. Let Ci=red−1⁡(𝒰i∩𝒳o)C_{i}={\operatorname{red}}^{-1}({\mathcal{U}}_{i}\cap\mathcal{X}_{o}). The subsets CiC_{i} form a finite closed cover of XΣanX_{\Sigma}^{{\text{\rm an}}}. On 𝒰i{\mathcal{U}}_{i} we can write sΨ⊗e=gi​sis_{\Psi}^{\otimes e}=g_{i}s_{i} for certain rational function gig_{i}. Therefore, on CiC_{i}, we have log⁡‖sΨ​(p)‖=log⁡|g⁡(p)|e\log\|s_{\Psi}(p)\|=\frac{\log|g(p)|}{e}. By Lemma 5.48, it follows that there is a finite closed cover of NℝN_{\mathbb{R}} and the restriction of ψ∥⋅∥\psi_{\|\cdot\|} to each of these closed subsets is rational piecewise affine. Therefore ψ∥⋅∥\psi_{\|\cdot\|} is rational piecewise affine. The second statement follows from the first and Corollary 5.47. ∎

The next point we study is how to turn a non-toric metric into a toric one. Since the image of θ0\theta_{0} consists of fixed points under the action of 𝕊an\mathbb{S}^{{\text{\rm an}}} (see Proposition-Definition 5.2), we may think of it as the analogue, in the non-Archimedean case, of a Haar measure of volume 11 on the compact torus 𝕊an\mathbb{S}^{{\text{\rm an}}}.

Let Ψ\Psi be a virtual support function on Σ\Sigma. Write L=𝒪⁡(DΨ)L=\mathcal{O}(D_{\Psi}) and s=sΨs=s_{\Psi}. Let ∥⋅∥\|\cdot\| be a metric on LanL^{{\text{\rm an}}}, non-necessarily toric. Then we define ψ∥⋅∥:Nℝ→ℝ\psi_{\|\cdot\|}\colon N_{\mathbb{R}}\to\mathbb{R} by

(5.50) ψ∥⋅∥(u)=1λKlog∥s(θ0(𝐞K(u)))∥.\psi_{\|\cdot\|}(u)=\frac{1}{\lambda_{K}}\log\|s(\theta_{0}({\operatorname{\mathbf{e}}}_{K}(u)))\|.

Note that, if ∥⋅∥\|\cdot\| is a toric metric, the definition of ψ∥⋅∥\psi_{\|\cdot\|} we have just given agrees with the one given in §5.2. This is clear because, if the metric is toric, then ‖s⁡(p)‖=‖s⁡(θ0​ρ0​(p))‖\|s(p)\|=\|s(\theta_{0}\rho_{0}(p))\|.

Proposition 5.51.

The assignment that, to a local section ss of LL gives the function defined as ∥s(θ0ρ0(p)∥\|s(\theta_{0}\rho_{0}(p)\| for p∈XΣanp\in X^{{\text{\rm an}}}_{\Sigma}, is a toric metric on LanL^{{\text{\rm an}}}, that we denote ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}}. Moreover, ψ∥⋅∥=ψ∥⋅∥𝕊\psi_{\|\cdot\|}=\psi_{\|\cdot\|_{\mathbb{S}}}.

Proof.

As in the proof of Proposition 5.16, we can verify that the function ψ∥⋅∥−Ψ\psi_{\|\cdot\|}-\Psi can be extended to a continuous function on NΣN_{\Sigma}. Using that θ0\theta_{0} is a section of ρ0\rho_{0} and the image of θ0\theta_{0} consists of points which are fixed under the action of 𝕊an\mathbb{S}^{{\text{\rm an}}}, we also verify that ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} is the toric metric associated to ψ∥⋅∥\psi_{\|\cdot\|} by the same proposition. ∎

The relationship between toric algebraic metrics and rational piecewise functions of Theorem 5.49 can be extended to the case when the metric is non-toric.

Proposition 5.52.

Let ∥⋅∥\|\cdot\| be an algebraic metric. Then the function ψ∥⋅∥\psi_{\|\cdot\|} is rational piecewise affine.

Proof.

Just observe that in the proof of Theorem 5.49 one does not use the fact that the metric is toric. ∎

We now study the effect of taking a field extension. Let K⊂HK\subset H be a finite extension of fields that are complete with respect to an absolute value associated to a nontrivial discrete valuation. We assume that the absolute value of HH is an extension of the absolute value of KK. Let H∘{H}^{\circ} be the valuation ring of HH, H∘⁣∘{H}^{\circ\circ} the maximal ideal, ϖ′\varpi^{\prime} a generator of the maximal ideal, λH=log⁡(|ϖ′|−1)\lambda_{H}=\log(|\varpi^{\prime}|^{-1}). Let eH/Ke_{H/K} be the ramification degree of the extension. Hence λK=eH/K​λH\lambda_{K}=e_{H/K}\lambda_{H}.

Proposition 5.53.

Let Σ\Sigma be a complete fan in NℝN_{\mathbb{R}} and let Π\Pi be a complete SCR polyhedral complex in NℝN_{\mathbb{R}} with Σ=rec⁡(Π)\Sigma=\operatorname{rec}(\Pi).

  1. (1)

    Let XΣ,KX_{\Sigma,K} and XΣ,HX_{\Sigma,H} denote the toric varieties defined by Σ\Sigma over KK and HH respectively. Then

    XΣ,H=Spec⁡(H)×XΣ,K.X_{\Sigma,H}=\operatorname{Spec}(H)\times X_{\Sigma,K}.

    Moreover there is a commutative diagram

    XΣ,Han\textstyle{X_{\Sigma,H}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ρΣ,H\scriptstyle{\rho_{\Sigma,H}}XΣ,Kan\textstyle{X^{{\text{\rm an}}}_{\Sigma,K}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ρΣ,K\scriptstyle{\rho_{\Sigma,K}}XΣ​(ℝ≥0),\textstyle{X_{\Sigma}(\mathbb{R}_{\geq 0}),}

    where the horizontal map is induced by the restriction of seminorms.

  2. (2)

    Let Π′\Pi^{\prime} be the polyhedral complex in NℝN_{\mathbb{R}} obtained from Π\Pi by applying a homothety of ratio eH/Ke_{H/K}. Then

    𝒳Π′,H∘=Nor⁡(Spec⁡(H∘)×𝒳Π,K∘),{\mathcal{X}}_{\Pi^{\prime},{H}^{\circ}}=\operatorname{Nor}(\operatorname{Spec}(H^{\circ})\times{\mathcal{X}}_{\Pi,K^{\circ}}),

    where Nor\operatorname{Nor} denotes the normalization of a scheme.

  3. (3)

    Let ψ\psi be a rational piecewise linear function on Π\Pi and denote Ψ=rec⁡(ψ)\Psi=\operatorname{rec}(\psi). Let L=𝒪⁡(DΨ)L=\mathcal{O}(D_{\Psi}) be the line bundle on XΣ,KX_{\Sigma,K} determined by Ψ\Psi and let ∥⋅∥\|\cdot\| be the metric on LanL^{{\text{\rm an}}} determined by ψ\psi. Let L′L^{\prime} be the line bundle obtained by base change and ∥⋅∥′\|\cdot\|^{\prime} the metric obtained by inverse image. Then

    ψ∥⋅∥′(u)=(ψeH/K)(u)=eH/Kψ(eH/K−1u).\psi_{\|\cdot\|^{\prime}}(u)=(\psi e_{H/K})(u)=e_{H/K}\psi(e_{H/K}^{-1}u).
  4. (4)

    There is a commutative diagram

    XΣ,Han\textstyle{X_{\Sigma,H}^{{\text{\rm an}}}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}XΣ,Kan\textstyle{X^{{\text{\rm an}}}_{\Sigma,K}}XΣ​(ℝ≥0).\textstyle{X_{\Sigma}(\mathbb{R}_{\geq 0})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces.}θΣ,H\scriptstyle{\theta_{\Sigma,H}}θΣ,K\scriptstyle{\theta_{\Sigma,K}}
Proof.

The statement (1) can be checked locally. Let σ\sigma be a cone of Σ\Sigma. Then

Xσ,H=Spec⁡(H⁡[Mσ])=Spec⁡(K⁡[Mσ]​⊗𝐾​H)=Spec⁡(H)​×𝐾​Xσ,K.X_{\sigma,H}=\operatorname{Spec}(H[M_{\sigma}])=\operatorname{Spec}(K[M_{\sigma}]\underset{K}{\otimes}H)=\operatorname{Spec}(H)\underset{K}{\times}X_{\sigma,K}.

This proves the first assertion. The commutativity of the diagram follows from the fact that the map XΣ,Han→XΣ,KanX_{\Sigma,H}^{{\text{\rm an}}}\to X^{{\text{\rm an}}}_{\Sigma,K} is given by the restriction of seminorms.

The statement (2) can also be checked locally. Let Λ\Lambda be a polyhedron of Π\Pi. Let Λ′=eK′/K​Λ\Lambda^{\prime}=e_{K^{\prime}/K}\Lambda. Then it is clear that

K∘​[𝒳Λ]​⊗K∘​H∘⊂H∘​[𝒳Λ′].K^{\circ}[{\mathcal{X}}_{\Lambda}]\underset{K^{\circ}}{\otimes}H^{\circ}\subset H^{\circ}[{\mathcal{X}}_{\Lambda^{\prime}}].

Since the right-hand side ring is integrally closed, the integral closure of the left side ring is contained in the right side ring. Therefore we need to prove that H⁡[M~Λ′]H[{\widetilde{M}}_{\Lambda^{\prime}}] is integral over the left side ring. Let (a,l)∈M~Λ′(a,l)\in{\widetilde{M}}_{\Lambda^{\prime}}. Thus (eH/K​a,l)∈M~Λ(e_{H/K}a,l)\in{\widetilde{M}}_{\Lambda}. Then the monomial χaϖ′∈lH∘[𝒳Λ′]\chi^{a}\varpi^{\prime}{}^{l}\in H^{\circ}[{\mathcal{X}}_{\Lambda^{\prime}}] satisfies

(χaϖ′)leH/K=(χeH/K​aϖl)∈K∘[𝒳Λ]⊗K∘H∘.(\chi^{a}\varpi^{\prime}{}^{l})^{e_{H/K}}=(\chi^{e_{H/K}a}\varpi^{l})\in K^{\circ}[{\mathcal{X}}_{\Lambda}]\underset{K^{\circ}}{\otimes}H^{\circ}.

Hence χaϖ′l\chi^{a}\varpi^{\prime}{}^{l} is integral over K∘​[𝒳Λ]​⊗K∘​H∘.K^{\circ}[{\mathcal{X}}_{\Lambda}]\underset{K^{\circ}}{\otimes}H^{\circ}. Since these monomials generate H∘​[𝒳Λ′]H^{\circ}[{\mathcal{X}}_{\Lambda^{\prime}}], we obtain the result.

To prove (3), let p′∈X0,Hanp^{\prime}\in X^{{\text{\rm an}}}_{0,H} and let p∈X0,Kanp\in X^{{\text{\rm an}}}_{0,K} be the corresponding point. Then valK⁡(p)=valH⁡(p′)eH/K{\operatorname{val}}_{K}(p)=\frac{{\operatorname{val}}_{H}(p^{\prime})}{e_{H/K}}. Therefore, if we write u=valK⁡(p)u={\operatorname{val}}_{K}(p) and u′=valH⁡(p′)eH/Ku^{\prime}=\frac{{\operatorname{val}}_{H}(p^{\prime})}{e_{H/K}}, we have

ψ∥⋅∥′(u′)=1λHlog∥s(p′)∥′=eH/KλKlog∥s(p)∥=eH/Kψ(u)=eH/Kψ(u′/eH/K).\psi_{\|\cdot\|^{\prime}}(u^{\prime})=\frac{1}{\lambda_{H}}\log\|s(p^{\prime})\|^{\prime}=\frac{e_{H/K}}{\lambda_{K}}\log\|s(p)\|=e_{H/K}\psi(u)=e_{H/K}\psi(u^{\prime}/e_{H/K}).

Finally, statement (4) follows directly from the definition of θΣ\theta_{\Sigma} because the horizontal arrow is given by the restriction of seminorms. ∎

5.5. The one-dimensional case

We now study in detail the one-dimensional case. Besides being a concrete example of the relationship between functions, models, metrics, and measures, it is also a crucial step in the proof that a toric metric is semipositive if and only if the corresponding function is concave. Of this equivalence, up to now we have proved only one implication and the reverse implication will be proved in the next section.

The only complete one-dimensional toric variety over a field is the projective line. Since, by Proposition 5.53 and Proposition 2.35 we know the effect of taking finite extensions of the field KK, we can use the following result to reduce any model of ℙ1\mathbb{P}^{1} to a simpler form.

Definition 5.54.

Let KK be a field complete with respect to an absolute value associated to a nontrivial discrete valuation. Let K∘K^{\circ} be the ring of integers. Let XX be a proper curve over KK. A semi-stable model of XX is a flat proper regular scheme 𝒳{\mathcal{X}} of finite type over Spec⁡(K∘)\operatorname{Spec}(K^{\circ}) with an isomorphism X→𝒳ηX\to{\mathcal{X}}_{\eta}, such that the special fibre 𝒳o{\mathcal{X}}_{o} is a reduced normal crossing divisor.

Proposition 5.55.

Let KK be a field complete with respect to an absolute value associated to a nontrivial discrete valuation. Let K∘K^{\circ} be the ring of integers. Let 𝒳{\mathcal{X}} be a proper model over K∘K^{\circ} of ℙK1\mathbb{P}^{1}_{K}. Then there exists a finite extension HH of KK with ring of integers H∘{H}^{\circ}, a semi-stable model 𝒳′{\mathcal{X}}^{\prime} of ℙH1\mathbb{P}^{1}_{H}, and a proper morphism of models 𝒳′→𝒳×Spec⁡(H∘)\mathcal{X}^{\prime}\to\mathcal{X}\times\operatorname{Spec}({H}^{\circ}).

Proof.

This follows, for instance, from [Liu06, Corollary 2.8]. ∎

Consider the toric variety XΣ≃ℙ1X_{\Sigma}\simeq\mathbb{P}^{1}. We can choose an isomorphism N≃ℤN\simeq\mathbb{Z} and Nℝ≃ℝN_{\mathbb{R}}\simeq\mathbb{R}. Then Σ={ℝ−,{0},ℝ+}\Sigma=\{\mathbb{R}_{-},\{0\},\mathbb{R}_{+}\}. Let 00 denote the invariant point of ℙK1\mathbb{P}^{1}_{K} corresponding to the cone ℝ+\mathbb{R}_{+} and ∞\infty the invariant point corresponding to the cone ℝ−\mathbb{R}_{-}. Let tt denote the absolute coordinate of ℙ1\mathbb{P}^{1} given by the monomial χ1\chi^{1}.

Let 𝒳\mathcal{X} be a semi-stable model of ℙK1\mathbb{P}^{1}_{K}. By extending scalars if necessary, we may suppose that all the components of the special fibre are defined over k=K∘/K∘⁣∘k=K^{\circ}/K^{\circ\circ} and contain a rational point. Since the special fibre 𝒳o\mathcal{X}_{o} is connected and of genus zero, we deduce that the special fibre is a tree of rational curves, each isomorphic to ℙk1\mathbb{P}^{1}_{k}. Let D0D_{0} and D∞D_{\infty} denote the horizontal divisors corresponding to the point 00 and ∞\infty of ℙK1\mathbb{P}^{1}_{K}. Then, there is a chain of rational curves that links the divisor D0D_{0} with D∞D_{\infty} that is contained in the special fibre. We will denote the irreducible components of the special fibre that form this chain by E0,…,EkE_{0},\dots,E_{k}, in such a way that the component E0E_{0} meets D0D_{0}, the component EkE_{k} meets D∞D_{\infty} and, for 0<i<k0<i<k, the component EiE_{i} meets only Ei−1E_{i-1} and Ei+1E_{i+1}. The other components of 𝒳o\mathcal{X}_{o} will be grouped in branches, each branch has its root in one of the components EiE_{i}. We will denote by Fi,jF_{i,j}, j∈Θij\in\Theta_{i} the components that belong to a branch with root in EiE_{i}. We are not giving any particular order to the sets Θi\Theta_{i}.

We denote by E⋅FE\cdot F the intersection product of two 11-cycles of 𝒳{\mathcal{X}}. Since the special fibre is reduced, we have

div⁡(ϖ)=∑i=0k(Ei+∑j∈ΘiFi,j).\operatorname{div}(\varpi)=\sum_{i=0}^{k}\left(E_{i}+\sum_{j\in\Theta_{i}}F_{i,j}\right).

Again by the assumption of semi-stability, the intersection product of two different components of 𝒳o\mathcal{X}_{o} is either 11, if they meet, or zero, if they do not meet. Since the intersection product of div⁡(ϖ)\operatorname{div}(\varpi) with any component of 𝒳o\mathcal{X}_{o} is zero, we deduce that, if EE is any component of 𝒳o\mathcal{X}_{o}, the self-intersection product E⋅EE\cdot E is equal to minus the number of components that meet EE. In particular, all components Fi,jF_{i,j} that are terminal, are (−1)(-1)-curves. By Castelnuovo Criterion, we can successively blow-down all the components Fi,jF_{i,j} to obtain a new semi-stable model of ℙK1\mathbb{P}^{1}_{K} whose special fibre consist of a chain of rational curves. For reasons that will become apparent later we denote this model as 𝒳𝕊{\mathcal{X}}_{\mathbb{S}}.

Lemma 5.56.

If we view tt as a rational function on 𝒳\mathcal{X}, then there is an integer aa such that

div⁡(t)=D0−D∞+∑i=0k(a−i)​(Ei+∑j∈ΘiFi,j).\operatorname{div}(t)=D_{0}-D_{\infty}+\sum_{i=0}^{k}(a-i)\left(E_{i}+\sum_{j\in\Theta_{i}}F_{i,j}\right).
Proof.

It is clear that

div⁡(t)=D0−D∞+∑i=0kai​Ei+∑j∈Θiai,j​Fi,j\operatorname{div}(t)=D_{0}-D_{\infty}+\sum_{i=0}^{k}a_{i}E_{i}+\sum_{j\in\Theta_{i}}a_{i,j}F_{i,j}

for certain coefficients aia_{i} and ai,ja_{i,j} that we want to determine as much as possible.

If a component EE of 𝒳0\mathcal{X}_{0}, with coefficient aa, does not meet D0D_{0} nor D∞D_{\infty}, but meets r≥1r\geq 1 other components, and the coefficients of r−1r-1 of these components are equal to aa, while the coefficient of the remaining component is bb, we obtain that

0=div⁡(t)⋅E=a​E⋅E+a⁡(r−1)+b=−r​a+a⁡(r−1)+b=b−a0=\operatorname{div}(t)\cdot E=aE\cdot E+a(r-1)+b=-ra+a(r-1)+b=b-a

Thus b=ab=a. Starting with the components Fi,jF_{i,j} that are terminal, we deduce that, for all ii and j∈Θij\in\Theta_{i}, ai=ai,ja_{i}=a_{i,j}. Therefore,

div⁡(t)=D0−D∞+∑i=0kai​(Ei+∑j∈ΘiFi,j).\operatorname{div}(t)=D_{0}-D_{\infty}+\sum_{i=0}^{k}a_{i}\left(E_{i}+\sum_{j\in\Theta_{i}}F_{i,j}\right).

In particular, the lemma is proved for k=0k=0. Assume now that k>0k>0.

It only remains to show that ai=a0−ia_{i}=a_{0}-i, that we prove by induction. For i=1i=1, we compute

0=div⁡(t)⋅E0=D0⋅E0+a0​E0⋅E0+a0​∑j∈Θ0F0,j⋅E0+a1​E1⋅E0=1−a0+a1.0=\operatorname{div}(t)\cdot E_{0}=D_{0}\cdot E_{0}+a_{0}E_{0}\cdot E_{0}+a_{0}\sum_{j\in\Theta_{0}}F_{0,j}\cdot E_{0}+a_{1}E_{1}\cdot E_{0}=1-a_{0}+a_{1}.

Thus a1=a0−1a_{1}=a_{0}-1. For 1<i≤k1<i\leq k, by induction hypothesis, ai−1=ai−2−1a_{i-1}=a_{i-2}-1. Then

0=div⁡(t)⋅Ei−1=ai−2−2​ai−1+ai=1−ai−1+ai.0=\operatorname{div}(t)\cdot E_{i-1}=a_{i-2}-2a_{i-1}+a_{i}=1-a_{i-1}+a_{i}.

Thus ai=ai−1−1=a0−ia_{i}=a_{i-1}-1=a_{0}-i, proving the lemma. ∎

The determination of div⁡(t)\operatorname{div}(t) allows us to give a partial description of the map red:XΣan→𝒳o{\operatorname{red}}\colon X_{\Sigma}^{{\text{\rm an}}}\to\mathcal{X}_{o}. For us, the most interesting points of 𝒳o\mathcal{X}_{o} are the points q0:=D0∩E0q_{0}:=D_{0}\cap E_{0}, qi:=Ei−1∩Eiq_{i}:=E_{i-1}\cap E_{i}, i=1,…,ki=1,\dots,k, qk+1:=Ek∩D∞q_{k+1}:=E_{k}\cap D_{\infty} and the generic points of the components EiE_{i} that we denote ηi\eta_{i}, i=0,…,ki=0,\dots,k.

Lemma 5.57.

Let p∈XΣanp\in X_{\Sigma}^{{\text{\rm an}}}. Then

red⁡(p)={q0, if ​|t⁡(p)|<|ϖ|aqi,i=1​…,k, if ​|ϖ|a−i+1<|t⁡(p)|<|ϖ|a−iqk+1, if ​|ϖ|a−k<|t⁡(p)|ηi,i=0​…,k, if ​|t⁡(p)|=|ϖ|a−i​ and ​p∈im⁡(θΣ).{\operatorname{red}}(p)=\begin{cases}q_{0},&\text{ if }|t(p)|<|\varpi|^{a}\\ q_{i},\ i=1\dots,k,&\text{ if }|\varpi|^{a-i+1}<|t(p)|<|\varpi|^{a-i}\\ q_{k+1},&\text{ if }|\varpi|^{a-k}<|t(p)|\\ \eta_{i},\ i=0\dots,k,&\text{ if }|t(p)|=|\varpi|^{a-i}\text{ and }p\in\operatorname{im}(\theta_{\Sigma}).\end{cases}
Proof.

Let 1≤i≤k1\leq i\leq k. The rational function x:=t​ϖ−a+ix:=t\varpi^{-a+i} has a zero of order one along the component Ei−1E_{i-1} and the support of its divisor does not contain the component EiE_{i}. On the other hand, the rational function y:=t−1​ϖa−i+1y:=t^{-1}\varpi^{a-i+1} has a zero of order one along the component EiE_{i} and the support of its divisor does not contain the component Ei−1E_{i-1}. Thus {x,y}\{x,y\} is a system of parameters in a neighbourhood of qiq_{i}. We denote

A=K∘​[t​ϖ−a+i,t−1​ϖa−i+1]≃K∘​[x,y]/(x​y−ϖ).A=K^{\circ}[t\varpi^{-a+i},t^{-1}\varpi^{a-i+1}]\simeq K^{\circ}[x,y]/(xy-\varpi).

The local ring at the point qiq_{i} is A(x,y)A_{(x,y)}. Let pp be a point such that |ϖ|a−i+1<|t⁡(p)|<|ϖ|a−i|\varpi|^{a-i+1}<|t(p)|<|\varpi|^{a-i}. Therefore, for f∈Af\in A we have |f⁡(p)|≤1|f(p)|\leq 1. Moreover, if f∈(x,y)f\in(x,y), then |f⁡(p)|<1|f(p)|<1. Since the ideal (x,y)(x,y) is maximal, we deduce that, for f∈Af\in A, the condition |f⁡(p)|<1|f(p)|<1 is equivalent to the condition f∈(x,y)f\in(x,y). This implies that red⁡(p)=qi{\operatorname{red}}(p)=q_{i}. A similar argument works for q0q_{0} and qk+1q_{k+1}.

Assume now that p∈im⁡(θΣ)p\in\operatorname{im}(\theta_{\Sigma}) and that |t⁡(p)|=|ϖ|a−i|t(p)|=|\varpi|^{a-i}. If i≠0i\not=0 we consider again the ring AA, but in this case |x⁡(p)|=|t⁡(p)​ϖ−a+i|=1|x(p)|=|t(p)\varpi^{-a+i}|=1. Let I={f∈A∣|f⁡(p)|<1}I=\{f\in A\mid|f(p)|<1\}. It is clear that (y,ϖ)⊂I(y,\varpi)\subset I. For f=∑m∈ℤβm​tm∈Af=\sum_{m\in\mathbb{Z}}\beta_{m}t^{m}\in A, since p∈im⁡(θΣ)p\in\operatorname{im}(\theta_{\Sigma}), we have

|f⁡(p)|=supm(|βm|​|t⁡(p)|m).|f(p)|=\sup_{m}(|\beta_{m}||t(p)|^{m}).

This implies that I⊂(y,ϖ)I\subset(y,\varpi). Hence II is the ideal that defines the component EiE_{i} and this is equivalent to red⁡(p)=ηi{\operatorname{red}}(p)=\eta_{i}. The case i=0i=0 is analogous. ∎

The image by red{\operatorname{red}} of the remaining points of XΣanX_{\Sigma}^{{\text{\rm an}}} is not characterized only by the value of |t⁡(p)||t(p)|. Using a proof similar to that of the lemma, one can show that, if |t⁡(p)|=|ϖ|a−i|t(p)|=|\varpi|^{a-i} then red⁡(p){\operatorname{red}}(p) belongs either to EiE_{i} or to any of the components Fi,jF_{i,j}, j∈Θij\in\Theta_{i}.

We denote by ξi\xi_{i} (resp. ξi,j\xi_{i,j}) the point of XΣanX_{\Sigma}^{{\text{\rm an}}} corresponding to the component EiE_{i} (resp. Fi,jF_{i,j}). That is, red⁡(ξi)=ηi{\operatorname{red}}(\xi_{i})=\eta_{i} and red⁡(ξi,j)=ηi,j{\operatorname{red}}(\xi_{i,j})=\eta_{i,j}, where ηi,j\eta_{i,j} is the generic point of Fi,jF_{i,j} (see (2.15) and (2.14)).

Lemma 5.58.

Let 0≤i≤k0\leq i\leq k. Then, for every j∈Θij\in\Theta_{i},

valK⁡(ξi)=valK⁡(ξi,j)=a−i,{\operatorname{val}}_{K}(\xi_{i})={\operatorname{val}}_{K}(\xi_{i,j})=a-i,

where aa is the integer of Lemma 5.56.

Proof.

We consider the rational function ϖ−a+i​t\varpi^{-a+i}t. Since the support of div⁡(ϖ−a+i​t)\operatorname{div}(\varpi^{-a+i}t) does not contain the component EiE_{i} nor any of the components Fi,jF_{i,j}, we have that

|ϖ−a+i​t​(ξi)|=|ϖ−a+i​t​(ξi,j)|=1.|\varpi^{-a+i}t(\xi_{i})|=|\varpi^{-a+i}t(\xi_{i,j})|=1.

Since t=χ1t=\chi^{1}, we deduce, using equation (5.4), that

valK⁡(ξi)=−log⁡|χ1​(xi)|λK=−log⁡|ϖa−i|−log⁡|ϖ|=a−i.{\operatorname{val}}_{K}(\xi_{i})=\frac{-\log|\chi^{1}(x_{i})|}{\lambda_{K}}=\frac{-\log|\varpi^{a-i}|}{-\log|\varpi|}=a-i.

∎

Let now Ψ\Psi be a virtual support function on Σ\Sigma. It can be written as

Ψ⁡(u)={m∞​u, if ​u≤0,m0​u, if ​u≥0.\Psi(u)=\begin{cases}m_{\infty}u,&\text{ if }u\leq 0,\\ m_{0}u,&\text{ if }u\geq 0.\end{cases}

for some m0,m∞∈ℤm_{0},m_{\infty}\in\mathbb{Z}. Then, L=𝒪⁡(DΨ)≃𝒪⁡(m∞−m0)L=\mathcal{O}(D_{\Psi})\simeq\mathcal{O}(m_{\infty}-m_{0}), and div⁡(sΨ)=−m0​[0]+m∞​[∞]\operatorname{div}(s_{\Psi})=-m_{0}[0]+m_{\infty}[\infty]. Let ℒ\mathcal{L} be a model over 𝒳\mathcal{X} of L⊗eL^{\otimes e}. If we consider sΨ⊗es_{\Psi}^{\otimes e} as a rational section of ℒ\mathcal{L}, then

(5.59) div⁡(sΨ⊗e)=−e​m0​D0+e​m∞​D∞+∑i=0k(αi​Ei+∑j∈Θiαi,j​Fi,j)\operatorname{div}(s_{\Psi}^{\otimes e})=-em_{0}D_{0}+em_{\infty}D_{\infty}+\sum_{i=0}^{k}\left(\alpha_{i}E_{i}+\sum_{j\in\Theta_{i}}\alpha_{i,j}F_{i,j}\right)

for certain coefficients αi\alpha_{i} and αi,j\alpha_{i,j}. Let ∥⋅∥\|\cdot\| be the metric on LanL^{{\text{\rm an}}} determined by this model.

Lemma 5.60.

The function ψ∥⋅∥\psi_{\|\cdot\|} is given by

ψ∥⋅∥(u)={m0​u−m0​a−α0e, if ​u≥a,(αi+1−αi)​u−(αi+1−αi)​(a−i)−αie, if ​a−i≥u≥a−i−1,m∞​u−m∞​(a−k)−αke, if ​a−k≥u.\psi_{\|\cdot\|}(u)=\begin{cases}m_{0}u-m_{0}a-\frac{\alpha_{0}}{e},&\text{ if }u\geq a,\\ \frac{(\alpha_{i+1}-\alpha_{i})u-(\alpha_{i+1}-\alpha_{i})(a-i)-\alpha_{i}}{e},&\text{ if }a-i\geq u\geq a-i-1,\\ m_{\infty}u-m_{\infty}(a-k)-\frac{\alpha_{k}}{e},&\text{ if }a-k\geq u.\end{cases}

In other words, if Π\Pi is the polyhedral complex in NℝN_{\mathbb{R}} given by the intervals

(−∞,a−k],[a−i,a−i+1],i=1,…,k,[a,∞),(-\infty,a-k],\quad[a-i,a-i+1],\ i=1,\dots,k,\quad[a,\infty),

then ψ∥⋅∥\psi_{\|\cdot\|} is the rational piecewise affine function on Π\Pi characterized by the conditions

  1. (1)

    rec(ψ∥⋅∥)=Ψ\operatorname{rec}(\psi_{\|\cdot\|})=\Psi,

  2. (2)

    the value of ψ∥⋅∥\psi_{\|\cdot\|} at the point a−ia-i is −αi/e-\alpha_{i}/e.

Proof.

Let p∈im⁡θΣp\in\operatorname{im}\theta_{\Sigma} be such that valK⁡(p)>a{\operatorname{val}}_{K}(p)>a, hence |t⁡(p)|<|ϖ|a|t(p)|<|\varpi|^{a}. By Lemma 5.57, this implies that red⁡(p)=q0{\operatorname{red}}(p)=q_{0}. In a neighbourhood of q0q_{0}, the divisor of the rational section sΨ⊗e​te​m0​ϖ−α0−e​m0​as_{\Psi}^{\otimes e}t^{em_{0}}\varpi^{-\alpha_{0}-em_{0}a} is zero, and so

‖sΨ⊗e​(p)​te​m0​(p)​ϖ−α0−e​m0​a‖=1.\|s_{\Psi}^{\otimes e}(p)t^{em_{0}}(p)\varpi^{-\alpha_{0}-em_{0}a}\|=1.

Set u=val⁡(p)u={\operatorname{val}}(p). Then,

ψ∥⋅∥(u)\displaystyle\psi_{\|\cdot\|}(u) =log⁡‖sΨ⊗e​(p)‖e​λK\displaystyle=\frac{\log\|s_{\Psi}^{\otimes e}(p)\|}{e\lambda_{K}}
=−e​m0​log⁡|t⁡(p)​|+(α0+e​m0​a)​log|​ϖ|−e​log⁡|ϖ|\displaystyle=\frac{-em_{0}\log|t(p)|+(\alpha_{0}+em_{0}a)\log|\varpi|}{-e\log|\varpi|}
=m0​(u−a)−α0e.\displaystyle=m_{0}(u-a)-\frac{\alpha_{0}}{e}.

The other cases are proved in a similar way. ∎

Since rec⁡(Π)=Σ\operatorname{rec}(\Pi)=\Sigma, this polyhedral complex defines a toric model 𝒳Π\mathcal{X}_{\Pi} of XΣX_{\Sigma}.

Proposition 5.61.

The identity map of XΣX_{\Sigma} extend to an isomorphism of models 𝒳𝕊→𝒳Π\mathcal{X}_{\mathbb{S}}\to\mathcal{X}_{\Pi}.

Proof.

The special fibre of 𝒳Π\mathcal{X}_{\Pi} is a chain of rational curves EiE_{i}, i=0,…,ki=0,\dots,k, corresponding to the points a−ia-i. The monomial χ1\chi^{1} is a section of the trivial line bundle and corresponds to the function ψ⁡(u)=−u\psi(u)=-u. Using Proposition 4.84 we obtain that

div⁡(χ1)=D0−D∞+∑i=0k(a−i)​Ei,\operatorname{div}(\chi^{1})=D_{0}-D_{\infty}+\sum_{i=0}^{k}(a-i)E_{i},

where D0D_{0} and D∞D_{\infty} are again the horizontal divisors determined by the points 00 and ∞\infty.

Since the vertices of the polyhedral complex Π\Pi are integral, by equation (4.87), we deduce that div⁡(ϖ)\operatorname{div}(\varpi) is reduced.

Then the result follows from [Lic68, Corollary 1.13] using an explicit description of the local rings at the points of the special fibre as in the proof of Lemma 5.57. ∎

From Proposition 5.61 we obtain a proper morphism π:𝒳→𝒳Π\pi\colon\mathcal{X}\to\mathcal{X}_{\Pi}. On 𝒳\mathcal{X} we had a line bundle ℒ\mathcal{L} and sΨ⊗es_{\Psi}^{\otimes e} was considered as a rational section of this line bundle. Let D=div⁡(sΨ⊗e)D=\operatorname{div}(s_{\Psi}^{\otimes e}) be the divisor given by equation (5.59). We denote

(5.62) D𝕊=π∗​D=−e​m0​D0+e​m∞​D∞+∑i=0kαi​Ei.D_{\mathbb{S}}=\pi_{\ast}D=-em_{0}D_{0}+em_{\infty}D_{\infty}+\sum_{i=0}^{k}\alpha_{i}E_{i}.

By Proposition 4.84 and Lemma 5.60 we see that D𝕊=De​ψhD_{\mathbb{S}}=D_{e\psi_{h}}. Thus 𝒪⁡(D𝕊)\mathcal{O}(D_{\mathbb{S}}) is a toric model of L⊗eL^{\otimes e}. Recall that ∥⋅∥\|\cdot\| denoted the metric associated to the model 𝒪⁡(D)\mathcal{O}(D). Let ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} be the toric metric obtained from ∥⋅∥\|\cdot\| as in Proposition 5.51. By this proposition and equation (5.62), the metric ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} agrees with the metric defined by the model 𝒪⁡(D𝕊)\mathcal{O}(D_{\mathbb{S}}). Thus, we have identified a toric model that corresponds to the metric ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}}. This allows us to compute directly the associated measure.

Proposition 5.63.

Let XΣ≃ℙK1X_{\Sigma}\simeq\mathbb{P}^{1}_{K} be a one-dimensional toric variety over KK. Let L≃𝒪⁡(DΨ)L\simeq\mathcal{O}(D_{\Psi}) be a toric line bundle and let ∥⋅∥\|\cdot\| be an algebraic metric defined by a semi-stable model and let ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} be the associated toric metric. Then

c1(L,∥⋅∥𝕊)∧δXΣ=(θΣ)∗(ρΣ)∗(c1(L,∥⋅∥)∧δXΣ).c_{1}(L,\|\cdot\|_{\mathbb{S}})\land\delta_{X_{\Sigma}}=(\theta_{\Sigma})_{\ast}(\rho_{\Sigma})_{\ast}\left(c_{1}(L,\|\cdot\|)\land\delta_{X_{\Sigma}}\right).
Proof.

Since the special fibre is reduced, by equation (2.29)

c1(L,∥⋅∥)∧δXΣ=1e∑i=0k(degℒEiδξi+∑j∈ΘidegℒFi,jδξi,j).c_{1}(L,\|\cdot\|)\land\delta_{X_{\Sigma}}=\frac{1}{e}\sum_{i=0}^{k}\left(\deg_{\mathcal{L}}E_{i}\delta_{\xi_{i}}+\sum_{j\in\Theta_{i}}\deg_{\mathcal{L}}F_{i,j}\delta_{\xi_{i,j}}\right).

Denote this measure temporarily by μ\mu. Then

(θΣ)∗​(ρΣ)∗​μ\displaystyle(\theta_{\Sigma})_{\ast}(\rho_{\Sigma})_{\ast}\mu =1e​∑i=0k(degℒ⁡Ei+∑j∈Θidegℒ⁡Fi,j)​δξi\displaystyle=\frac{1}{e}\sum_{i=0}^{k}\left(\deg_{\mathcal{L}}E_{i}+\sum_{j\in\Theta_{i}}\deg_{\mathcal{L}}F_{i,j}\right)\delta_{\xi_{i}}
=1e​∑i=0k(D⋅Ei+∑j∈ΘiD⋅Fi,j)​δξi\displaystyle=\frac{1}{e}\sum_{i=0}^{k}\left(D\cdot E_{i}+\sum_{j\in\Theta_{i}}D\cdot F_{i,j}\right)\delta_{\xi_{i}}
=1e​∑i=0k∑l=0k(αl​El+∑s∈Θlαl,s​Fl,s)⋅(Ei+∑j∈ΘiFi,j)​δξi\displaystyle=\frac{1}{e}\sum_{i=0}^{k}\sum_{l=0}^{k}\left(\alpha_{l}E_{l}+\sum_{s\in\Theta_{l}}\alpha_{l,s}F_{l,s}\right)\cdot\left(E_{i}+\sum_{j\in\Theta_{i}}F_{i,j}\right)\delta_{\xi_{i}}
=1e​∑i=0k(αi−1​Ei−1+αi​Ei+αi+1​Ei+1)⋅(Ei+∑j∈ΘiFi,j)​δξi\displaystyle=\frac{1}{e}\sum_{i=0}^{k}\left(\alpha_{i-1}E_{i-1}+\alpha_{i}E_{i}+\alpha_{i+1}E_{i+1}\right)\cdot\left(E_{i}+\sum_{j\in\Theta_{i}}F_{i,j}\right)\delta_{\xi_{i}}
=1e​∑i=0k(αi−1−2​αi+αi+1)​δξi.\displaystyle=\frac{1}{e}\sum_{i=0}^{k}(\alpha_{i-1}-2\alpha_{i}+\alpha_{i+1})\delta_{\xi_{i}}.

In the previous computation, we have used that, since El⋅div⁡(ϖ)=Fl,s⋅div⁡(ϖ)=0E_{l}\cdot\operatorname{div}(\varpi)=F_{l,s}\cdot\operatorname{div}(\varpi)=0, then

Fl,s⋅(Ei+∑j∈ΘiFi,j)\displaystyle F_{l,s}\cdot(E_{i}+\sum_{j\in\Theta_{i}}F_{i,j}) =0, for all i,j,l,s,\displaystyle=0,\text{ for all }i,j,l,s,
El⋅(Ei+∑j∈ΘiFi,j)\displaystyle E_{l}\cdot(E_{i}+\sum_{j\in\Theta_{i}}F_{i,j}) ={0, if ​l≠i−1,i,i+1,1, if ​l=i−1,i+1,−2, if ​l=i.\displaystyle=\begin{cases}0,&\text{ if }l\not=i-1,i,i+1,\\ 1,&\text{ if }l=i-1,i+1,\\ -2,&\text{ if }l=i.\end{cases}

An analogous computation shows that

(5.64) c1(L,∥⋅∥𝕊)∧δXΣ=1e∑i=0k(αi−1−2αi+αi+1)δξi.c_{1}(L,\|\cdot\|_{\mathbb{S}})\land\delta_{X_{\Sigma}}=\frac{1}{e}\sum_{i=0}^{k}(\alpha_{i-1}-2\alpha_{i}+\alpha_{i+1})\delta_{\xi_{i}}.

∎

Using Proposition 5.55 we can extend the above result to the case when the model is not semi-stable.

Corollary 5.65.

Let XΣ≃ℙK1X_{\Sigma}\simeq\mathbb{P}^{1}_{K} be a one-dimensional toric variety over KK. Let L≃𝒪⁡(DΨ)L\simeq\mathcal{O}(D_{\Psi}) be a toric line bundle, ∥⋅∥\|\cdot\| an algebraic metric, and ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} the associated toric metric. Then

c1(L,∥⋅∥𝕊)∧δXΣ=(θΣ)∗(ρΣ)∗(c1(L,∥⋅∥)∧δXΣ).c_{1}(L,\|\cdot\|_{\mathbb{S}})\land\delta_{X_{\Sigma}}=(\theta_{\Sigma})_{\ast}(\rho_{\Sigma})_{\ast}\left(c_{1}(L,\|\cdot\|)\land\delta_{X_{\Sigma}}\right).
Proof.

Let (𝒳,ℒ)(\mathcal{X},\mathcal{L}) be a model of (XΣ,L⊗e)(X_{\Sigma},L^{\otimes e}) that realizes the algebraic metric ∥⋅∥\|\cdot\|. For short, denote μ=c1(L,∥⋅∥)∧δXΣ\mu=c_{1}(L,\|\cdot\|)\land\delta_{X_{\Sigma}} and μ𝕊=c1(L,∥⋅∥𝕊)∧δXΣ\mu_{\mathbb{S}}=c_{1}(L,\|\cdot\|_{\mathbb{S}})\land\delta_{X_{\Sigma}}. By Proposition 5.55 there is a non-Archimedean field HH over KK and a semi-stable model 𝒳′{\mathcal{X}}^{\prime} of XΣ,HX_{\Sigma,H}. We may further assume that all the components of the special fibre of 𝒳′{\mathcal{X}}^{\prime} are defined over H∘/H∘⁣∘H^{\circ}/H^{\circ\circ}. Let (L′,∥⋅∥′)(L^{\prime},\|\cdot\|^{\prime}) be the metrized line bundle obtained by base change to HH. Then (∥⋅∥′)𝕊(\|\cdot\|^{\prime})_{\mathbb{S}} is obtained from ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} by base change. We denote by π:XΣ,Han→XΣ,Kan\pi\colon X^{{\text{\rm an}}}_{\Sigma,H}\to X^{{\text{\rm an}}}_{\Sigma,K} the map of analytic spaces. Be will denote by μ′\mu^{\prime}, μ𝕊′\mu^{\prime}_{\mathbb{S}}, θΣ′\theta_{\Sigma}^{\prime} and ρΣ′\rho_{\Sigma}^{\prime} the corresponding objects for XΣ,HX_{\Sigma,H}. Then, by Proposition 2.35 and Proposition 5.53,

μ𝕊=π∗​μ𝕊′=π∗​(θΣ′)∗​(ρΣ′)∗​μ′=(θΣ)∗​(ρΣ)∗​π∗​μ′=(θΣ)∗​(ρΣ)∗​μ.\mu_{\mathbb{S}}=\pi_{\ast}\mu^{\prime}_{\mathbb{S}}=\pi_{\ast}(\theta^{\prime}_{\Sigma})_{\ast}(\rho^{\prime}_{\Sigma})_{\ast}\mu^{\prime}=(\theta_{\Sigma})_{\ast}(\rho_{\Sigma})_{\ast}\pi_{\ast}\mu^{\prime}=(\theta_{\Sigma})_{\ast}(\rho_{\Sigma})_{\ast}\mu.

∎

We can now relate semipositivity of the metric with concavity of the associated function on the one-dimensional case.

Corollary 5.66.

Let XΣ≃ℙK1X_{\Sigma}\simeq\mathbb{P}^{1}_{K} be a one-dimensional toric variety over KK. Let (L,s)(L,s) be a toric line bundle with a toric section and let ∥⋅∥\|\cdot\| be a semipositive algebraic metric. Then ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} is a semipositive toric algebraic metric and ψ∥⋅∥\psi_{\|\cdot\|} is concave.

Proof.

Since ∥⋅∥\|\cdot\| is semipositive, c1(L,∥⋅∥)∧δXΣc_{1}(L,\|\cdot\|)\land\delta_{X_{\Sigma}} is a positive measure. By Corollary 5.65, c1(L,∥⋅∥𝕊)∧δXΣc_{1}(L,\|\cdot\|_{\mathbb{S}})\land\delta_{X_{\Sigma}} is a positive measure. Hence ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} is a semipositive toric metric. By equation (5.64) and Lemma 5.60, the positivity of c1(L,∥⋅∥𝕊)∧δXΣc_{1}(L,\|\cdot\|_{\mathbb{S}})\land\delta_{X_{\Sigma}} implies that the function ψ∥⋅∥=ψ∥⋅∥𝕊\psi_{\|\cdot\|}=\psi_{\|\cdot\|_{\mathbb{S}}} is concave. ∎

5.6. Algebraic metrics and their associated measures

We come back to the case of general dimension. Let Σ\Sigma be a complete fan, Ψ\Psi a support function on Σ\Sigma and (L,s)=(LΨ,sΨ)(L,s)=(L_{\Psi},s_{\Psi}). Since Ψ\Psi is a support function, the line bundle LL is generated by global sections.

Proposition 5.67.

Let ∥⋅∥\|\cdot\| be a semipositive algebraic metric on LanL^{{\text{\rm an}}}. Then the function ψ∥⋅∥\psi_{\|\cdot\|} is concave.

Proof.

Assume that ∥⋅∥\|\cdot\| is semipositive. Let u0u_{0} be a point of NℚN_{\mathbb{Q}} and let v0∈Nv_{0}\in N be primitive. Since the condition of being concave is closed, if we prove that, for all choices of u0∈Nℚu_{0}\in N_{\mathbb{Q}} and v0∈Nv_{0}\in N, the restriction of ψ∥⋅∥\psi_{\|\cdot\|} to the line u0+ℝ​v0u_{0}+\mathbb{R}v_{0} is concave, we will deduce that the function ψ∥⋅∥\psi_{\|\cdot\|} is concave. Let e∈ℕ×e\in\mathbb{N}^{\times} such that e​u0∈Neu_{0}\in N. Then H=K⁡(ϖ1/e)H=K(\varpi^{1/e}) is a finite extension of KK and there is a unique extension of the absolute value of KK to HH. We will denote with ′ the objects obtained by base change to HH. Let p∈X0,H​(H)p\in X_{0,H}(H) such that valH⁡(p)=e​u0{\operatorname{val}}_{H}(p)=eu_{0}. We consider the affine map A:ℤ→NA\colon\mathbb{Z}\to N given by l↦v0​l+e​u0l\mapsto v_{0}l+eu_{0}, and let HH be the linear part of AA. We consider the equivariant morphism φ=φp,H:ℙH1→XΣ,H\varphi=\varphi_{p,H}\colon\mathbb{P}^{1}_{H}\to X_{\Sigma,H} of Theorem 4.9. The metric ∥⋅∥\|\cdot\| induces an algebraic semipositive metric φ∗∥⋅∥′\varphi^{\ast}\|\cdot\|^{\prime} on the restriction of L′L^{\prime} (the line bundle obtained from LL by base change to HH) to ℙH1\mathbb{P}^{1}_{H}. By propositions 5.24 and 5.53(3) we obtain that

ψφ∗∥⋅∥(u)=eψ∥⋅∥(u0+e−1uv0).\psi_{\varphi^{\ast}\|\cdot\|}(u)=e\psi_{\|\cdot\|}(u_{0}+e^{-1}uv_{0}).

By Corollary 5.66 the left-hand side function is concave. Thus the restriction of ψ∥⋅∥\psi_{\|\cdot\|} to u0+ℝ​v0u_{0}+\mathbb{R}v_{0} is concave. We conclude that ψ=ψ∥⋅∥\psi=\psi_{\|\cdot\|} is concave. ∎

Corollary 5.68.

Let ∥⋅∥\|\cdot\| be a semipositive algebraic metric on LanL^{{\text{\rm an}}}. Then the toric metric ∥⋅∥𝕊\|\cdot\|_{\mathbb{S}} is a semipositive toric algebraic metric.

Proof.

By Proposition 5.67, the function ψ∥⋅∥\psi_{\|\cdot\|} is concave. By Proposition 5.52 it is also rational piecewise affine. By Corollary 5.47, the metric ∥⋅∥𝕊=∥⋅∥ψ\|\cdot\|_{\mathbb{S}}=\|\cdot\|_{\psi} is toric algebraic and semipositive. ∎

Putting together Proposition 5.67 and Theorem 5.49, we see that the relationship between semipositivity of the metric and concavity of the associated function given in the Archimedean case by Proposition 5.29 carries over to the non-Archimedean case.

Corollary 5.69.

Let ∥⋅∥\|\cdot\| be a toric algebraic metric and ψ∥⋅∥\psi_{\|\cdot\|} the associated function. Then the metric is semipositive if and only if the function ψ∥⋅∥\psi_{\|\cdot\|} is concave.

We can now characterize the Chambert-Loir measure associated to a toric semipositive algebraic metric.

Theorem 5.70.

Let ∥⋅∥\|\cdot\| be a toric semipositive algebraic metric on LanL^{{\text{\rm an}}} and let ψ=ψ∥⋅∥\psi=\psi_{\|\cdot\|} be the associated function on NℝN_{\mathbb{R}}. Let c1​(L¯)n∧δXΣc_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}} be the associated measure. Then

(5.71) (valK)∗​(c1​(L¯)n∧δXΣ)=n!​ℳ¯M​(ψ),({\operatorname{val}}_{K})_{\ast}(c_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}})=n!{\overline{\mathcal{M}}}_{M}(\psi),

where ℳ¯​(ψ){\overline{\mathcal{M}}}(\psi) is the measure of Definition 5.32. Moreover,

(5.72) c1​(L¯)n∧δXΣ=(θΣ)∗​(𝐞K)∗​n!​ℳ¯M​(ψ).c_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}}=(\theta_{\Sigma})_{\ast}({\operatorname{\mathbf{e}}}_{K})_{\ast}n!{\overline{\mathcal{M}}}_{M}(\psi).
Proof.

Since the metric is semipositive and toric, by Proposition 5.67 the function ψ\psi is concave. Since, moreover it is algebraic, by Theorem 5.49 it is defined by a toric model (𝒳Π,Dψ,e)({\mathcal{X}}_{\Pi},D_{\psi},e) of (XΣ,DΨ)(X_{\Sigma},D_{\Psi}) in the equivalence class determined by ψ\psi. As in Remark 4.66, the irreducible components of 𝒳Π,o{\mathcal{X}}_{\Pi,o} are in bijection with the vertices of Π\Pi. For each vertex v∈Π0v\in\Pi^{0}, let ξv\xi_{v} be the point of XΣanX_{\Sigma}^{{\text{\rm an}}} corresponding to the generic point of V⁡(v)V(v) defined by equation (2.15). Then, by equation (2.29),

c1​(L¯)n∧δXΣ=1en​∑v∈Π0νv​degDψ⁡V⁡(v)​δξv.c_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}}=\frac{1}{e^{n}}\sum_{v\in\Pi^{0}}\nu_{v}\deg_{D_{\psi}}V(v)\delta_{\xi_{v}}.

Thus, by Corollary 5.40,

(valK)∗​(c1​(L¯)n∧δXΣ)=1en​∑v∈Π0νv​degDψ⁡V⁡(v)​δv.({\operatorname{val}}_{K})_{\ast}(c_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}})=\frac{1}{e^{n}}\sum_{v\in\Pi^{0}}\nu_{v}\deg_{D_{\psi}}V(v)\delta_{v}.

But, using Proposition 3.95 and Proposition 4.105, the Monge-Ampère measure is given by

ℳM​(ψ)\displaystyle\mathcal{M}_{M}(\psi) =1en​ℳM​(e​ψ)\displaystyle=\frac{1}{e^{n}}\mathcal{M}_{M}(e\psi)
=1en​∑v∈Π0volM⁡(v∗)​δv\displaystyle=\frac{1}{e^{n}}\sum_{v\in\Pi^{0}}\operatorname{vol}_{M}(v^{\ast})\delta_{v}
=1n!​en​∑v∈Π0νv​degDψ⁡V⁡(v)​δv.\displaystyle=\frac{1}{n!e^{n}}\sum_{v\in\Pi^{0}}\nu_{v}\deg_{D_{\psi}}V(v)\delta_{v}.

Since ℳM​(ψ)\mathcal{M}_{M}(\psi) is a finite sum of Dirac deltas, we obtain that

ℳ¯M​(ψ)=1n!​en​∑v∈Π0νv​degDψ⁡V⁡(v)​δv.{\overline{\mathcal{M}}}_{M}(\psi)=\frac{1}{n!e^{n}}\sum_{v\in\Pi^{0}}\nu_{v}\deg_{D_{\psi}}V(v)\delta_{v}.

Hence we have proved (5.71). To prove equation (5.72) we just observe that xv=(θ0∘𝐞K)​(v)x_{v}=(\theta_{0}\circ{\operatorname{\mathbf{e}}}_{K})(v). ∎

5.7. Approachable and integrable metrics

We are now in position to characterize the approachable metrics. In this section KK is either ℝ\mathbb{R}, ℂ\mathbb{C} or a complete field with respect to an absolute value associated to a nontrivial discrete valuation. We fix a complete fan Σ\Sigma of NℝN_{\mathbb{R}}, so that XΣX_{\Sigma} is proper. Let Ψ\Psi be a support function on Σ\Sigma, ΔΨ\Delta_{\Psi} the corresponding polytope, and (LΨ,sΨ)(L_{\Psi},s_{\Psi}) the corresponding toric line bundle and section. For short, write X=XΣX=X_{\Sigma}, L=LΨL=L_{\Psi} and s=sΨs=s_{\Psi}.

Theorem 5.73.

Assume the previous hypothesis.

  1. (1)

    The assignment ∥⋅∥↦ψ∥⋅∥\|\cdot\|\mapsto\psi_{\|\cdot\|} is a bijection between the space of approachable toric metrics on LanL^{{\text{\rm an}}} and the space of continuous concave functions ψ\psi on NℝN_{\mathbb{R}} such that |ψ−Ψ||\psi-\Psi| is bounded.

  2. (2)

    The assignment ∥⋅∥↦ψ∥⋅∥∨\|\cdot\|\mapsto\psi_{\|\cdot\|}^{\vee} is a bijection between the space of approachable toric metrics on LanL^{{\text{\rm an}}} and the space of continuous concave functions on ΔΨ\Delta_{\Psi}.

Proof.

By Proposition 3.77(2) and Proposition 3.80, the statements (1) and (2) are equivalent.

Let ∥⋅∥\|\cdot\| be an approachable toric metric. By Corollary 5.17 the function |ψ∥⋅∥−Ψ||\psi_{\|\cdot\|}-\Psi| is bounded. By approachability there is a sequence ∥⋅∥l\|\cdot\|_{l} of smooth (resp. algebraic) semipositive metrics that converges to ∥⋅∥\|\cdot\|. Since ∥⋅∥\|\cdot\| is toric, ∥⋅∥𝕊=∥⋅∥\|\cdot\|_{\mathbb{S}}=\|\cdot\|. Hence, the sequence of toric metrics (∥⋅∥l)𝕊(\|\cdot\|_{l})_{\mathbb{S}} also converges to ∥⋅∥\|\cdot\|. We denote ψl=ψ(∥⋅∥l)𝕊\psi_{l}=\psi_{(\|\cdot\|_{l})_{\mathbb{S}}}. By Proposition 5.38 and Proposition 5.67 the functions ψl\psi_{l} are concave. Since the sequence (ψl)l(\psi_{l})_{l} converge uniformly to ψ∥⋅∥\psi_{\|\cdot\|}, the latter is concave.

Let now ψ\psi be a concave function on NℝN_{\mathbb{R}} such that |Ψ−ψ||\Psi-\psi| is bounded. Then ψ\psi determines a metric ∥⋅∥\|\cdot\| on the restriction of LanL^{{\text{\rm an}}} to X0anX_{0}^{{\text{\rm an}}}. Since stab⁡(ψ)=stab⁡(Ψ)=ΔΨ\operatorname{stab}(\psi)=\operatorname{stab}(\Psi)=\Delta_{\Psi}, by Proposition 3.81 there is a sequence of rational piecewise affine concave functions ψl\psi_{l} that converge uniformly to ψ\psi and with rec⁡(ψl)=Ψ\operatorname{rec}(\psi_{l})=\Psi. By Remark 5.46, the functions Ψ−ψl\Psi-\psi_{l} can be extended to continuous functions on NΣN_{\Sigma}. Therefore, Ψ−ψ\Psi-\psi can be extended to a continuous function on NΣN_{\Sigma}. Consequently the metric ∥⋅∥\|\cdot\| can be extended to XanX^{{\text{\rm an}}}. Let ∥⋅∥l\|\cdot\|_{l} be the metric associated to ψl\psi_{l}. Then the sequence of metrics ∥⋅∥l\|\cdot\|_{l} converges to ∥⋅∥\|\cdot\|. By Corollary 5.28, the metrics ∥⋅∥l\|\cdot\|_{l} are approachable. We deduce that ∥⋅∥\|\cdot\| is approachable. ∎

Remark 5.74.

For the case K=ℂK=\mathbb{C}, statement (2) in the above result is related to the Guillemin-Abreu classification of Kähler structures on symplectic toric varieties as explained in [Abr03]. By definition, a symplectic toric variety is a compact symplectic manifold of dimension 2​n2n together with a Hamiltonian action of the compact torus 𝕊an≃(S1)n\mathbb{S}^{{\text{\rm an}}}\simeq(S^{1})^{n}. These spaces are classified by Delzant polytopes of MℝM_{\mathbb{R}}, see for instance [Gui95]. For a given Delzant polytope Δ⊂Mℝ\Delta\subset M_{\mathbb{R}}, the possible (S1)n(S^{1})^{n}-invariant Kähler forms on the symplectic toric variety corresponding to Δ\Delta are classified by smooth convex functions on Δ∘\Delta^{\circ} satisfying some conditions near the border of Δ\Delta. Several differential geometric invariants of a Kähler toric variety can be translated and studied in terms of this convex function, also called the ‘‘symplectic potential’’.

For a smooth positive toric metric ∥⋅∥\|\cdot\| on LΨΔ​(ℂ)L_{\Psi_{\Delta}}(\mathbb{C}), the Chern form defines a Kähler structure on the complex toric variety XΣΔ​(ℂ)X_{\Sigma_{\Delta}}(\mathbb{C}). It turns out that the corresponding symplectic potential coincides with minus the function ψ∨∥⋅∥\psi^{\vee}_{\|\cdot\|}. It would be most interesting to explore further this connection.

We now study the compatibility of the restriction of approachable toric metrics to toric orbits and its inverse image by equivariant maps with direct and inverse image of concave functions. This is an extension of propositions 4.99 and 4.108. We start with the case of orbits, and we state a variant of Proposition 5.22 for approachable metrics.

Proposition 5.75.

Let ∥⋅∥\|\cdot\| be an approachable toric metric on LanL^{{\text{\rm an}}}, and denote L¯=(L,∥⋅∥){\overline{L}}=(L,\|\cdot\|) and ψ=ψL¯,s\psi=\psi_{{\overline{L}},s} the associated concave function on NℝN_{\mathbb{R}}. 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, πσ∨:M​(σ)ℝ→Mℝ\pi^{\vee}_{\sigma}\colon M(\sigma)_{\mathbb{R}}\to M_{\mathbb{R}} the dual inclusion and ι:V⁡(σ)→X\iota\colon V(\sigma)\to X the closed immersion. Set s′=χmσ​ss^{\prime}=\chi^{m_{\sigma}}s. Then

(5.76) ψι∗​L¯,ι∗​s′=(πσ)∗​(ψ−mσ).\psi_{\iota^{\ast}{\overline{L}},\iota^{\ast}s^{\prime}}=(\pi_{\sigma})_{\ast}(\psi-m_{\sigma}).

Dually, we have that

(5.77) ψι∗​L¯,ι∗​s′∨=(πσ∨+mσ)∗​ψ∨.\psi_{\iota^{\ast}{\overline{L}},\iota^{\ast}s^{\prime}}^{\vee}=(\pi^{\vee}_{\sigma}+m_{\sigma})^{\ast}\psi^{\vee}.

In other words, the Legendre-Fenchel dual of ψι∗​L¯,ι∗​s′\psi_{\iota^{\ast}{\overline{L}},\iota^{\ast}s^{\prime}} is the restriction of ψ∨\psi^{\vee} to the face FσF_{\sigma} translated by −mσ-m_{\sigma}.

Proof.

As in the proof of Proposition 4.99, it is enough to prove equation (5.76). By replacing ψ\psi by ψ−mσ\psi-m_{\sigma}, we can assume without loss of generality that mσ=0m_{\sigma}=0. By the continuity of the metric, the function ψ\psi can be extended to a continuous function ψ¯σ{\overline{\psi}}_{\sigma} on NσN_{\sigma}. Fix u0∈N​(σ)ℝu_{0}\in N(\sigma)_{\mathbb{R}}, write s=ψ¯σ​(u0)s={\overline{\psi}}_{\sigma}(u_{0}) and let u∈Nℝu\in N_{\mathbb{R}} such that πσ​(u)=u0\pi_{\sigma}(u)=u_{0}. By definition

(πσ)∗​(ψ)​(u0)=supp∈ℝ​σψ⁡(u+p).(\pi_{\sigma})_{\ast}(\psi)(u_{0})=\sup_{p\in\mathbb{R}\sigma}\psi(u+p).

It is clear that supp∈ℝ​σψ⁡(u+p)≥s\sup_{p\in\mathbb{R}\sigma}\psi(u+p)\geq s. Suppose that supp∈ℝ​σψ⁡(u+p)>s\sup_{p\in\mathbb{R}\sigma}\psi(u+p)>s. Let q∈ℝ​σq\in\mathbb{R}\sigma such that ψ⁡(u+q)>s\psi(u+q)>s and let ε=(ψ⁡(u+q)−s)/2\varepsilon=(\psi(u+q)-s)/2. By the definition of the topology of NσN_{\sigma}, there exists a p∈ℝ​σp\in\mathbb{R}\sigma such that

(5.78) s−ε<ψ⁡(u+p+σ)<s+ε.s-\varepsilon<\psi(u+p+\sigma)<s+\varepsilon.

Since σ\sigma is a cone of maximal dimension in ℝ​σ\mathbb{R}\sigma, there exists a point r∈(q+σ)∩(p+σ)r\in(q+\sigma)\cap(p+\sigma). By the right inequality of equation (5.78) ψ⁡(u+r)<ψ⁡(u+q)\psi(u+r)<\psi(u+q). By concavity of ψ\psi this implies that

(5.79) limλ→∞ψ⁡(u+r+λ⁡(r−q))=−∞.\lim_{\lambda\to\infty}\psi(u+r+\lambda(r-q))=-\infty.

Since, by construction u+r+ℝ≥0​(r−q)u+r+\mathbb{R}_{\geq 0}(r-q) is contained in u+p+σu+p+\sigma, equation (5.79) contradicts the left inequality of equation (5.78). Hence supp∈ℝ​σψ⁡(u+p)=s\sup_{p\in\mathbb{R}\sigma}\psi(u+p)=s, which proves equation (5.76). ∎

We now interpret the inverse image of an approachable toric metric by an equivariant map whose image intersects the principal open subset in terms of direct and inverse images of concave functions.

Proposition 5.80.

Let N1N_{1} and N2N_{2} be lattices and Σi\Sigma_{i} a complete fan in Ni,ℝN_{i,\mathbb{R}}, i=1,2i=1,2. Let H:N1→N2H\colon N_{1}\to N_{2} be a linear map such that, for each σ1∈Σ1\sigma_{1}\in\Sigma_{1}, there exists σ2∈Σ2\sigma_{2}\in\Sigma_{2} with H⁡(σ1)⊂σ2H(\sigma_{1})\subset\sigma_{2}. Let p∈XΣ2,0​(K)p\in X_{\Sigma_{2},0}(K) and write A:N1,ℝ→N2,ℝA\colon N_{1,\mathbb{R}}\to N_{2,\mathbb{R}} for the affine map A=H+val⁡(p)A=H+{\operatorname{val}}(p). Let ∥⋅∥\|\cdot\| be an approachable toric metric on 𝒪​(DΨ2)an{\mathcal{O}}(D_{\Psi_{2}})^{{\text{\rm an}}}. Then

ψφp.H∗∥⋅∥=A∗ψ∥⋅∥.\psi_{\varphi_{p.H}^{\ast}\|\cdot\|}=A^{*}\psi_{\|\cdot\|}.

Moreover, the Legendre-Fenchel dual of this function is given by

ψφp.H∗∥⋅∥∨=(H∨)∗(ψ∥⋅∥∨−val(p)).\psi_{\varphi_{p.H}^{\ast}\|\cdot\|}^{\vee}=(H^{\vee})_{*}\big(\psi^{\vee}_{\|\cdot\|}-{\operatorname{val}}(p)\big).
Proof.

The first statement is a direct consequence of Proposition 5.24 while the second one follows from Proposition 3.78(1). ∎

We next characterize the measures associated to an approachable metric.

Theorem 5.81.

Let Σ\Sigma be a complete fan of NℝN_{\mathbb{R}}, let Ψ\Psi be a support function on Σ\Sigma and let L=𝒪⁡(DΨ)L=\mathcal{O}(D_{\Psi}). Let ∥⋅∥\|\cdot\| be an approachable metric on LanL^{{\text{\rm an}}} and let ψ=ψ∥⋅∥\psi=\psi_{\|\cdot\|} be the corresponding concave function. Then

(5.82) (valK)∗​(c1​(L¯)n∧δXΣ)=n!​ℳ¯M​(ψ).({\operatorname{val}}_{K})_{\ast}(c_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}})=n!{\overline{\mathcal{M}}}_{M}(\psi).

Moreover, the measure c1​(L¯)n∧δXΣc_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}} is characterized, in the Archimedean case, by equation (5.82) and the fact of being toric, while in the non-Archimedean case it is given by

c1​(L¯)n∧δXΣ=(θΣ)∗​(𝐞K)∗​n!​ℳ¯M​(ψ).c_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}}=(\theta_{\Sigma})_{\ast}({\operatorname{\mathbf{e}}}_{K})_{\ast}n!{\overline{\mathcal{M}}}_{M}(\psi).
Proof.

For short, denote μ=(valK)∗​(c1​(L¯)n∧δXΣ)\mu=({\operatorname{val}}_{K})_{\ast}(c_{1}(\overline{L})^{n}\land\delta_{X_{\Sigma}}). Let ∥⋅∥l\|\cdot\|_{l} be a sequence of semipositive smooth (respectively algebraic) metrics converging to ∥⋅∥\|\cdot\|. By Proposition 2.33, the measures c1(L,∥⋅∥l)n∧δXΣc_{1}(L,\|\cdot\|_{l})^{n}\land\delta_{X_{\Sigma}} converge to c1​(L¯)n∧δXΣc_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}}. Therefore, the measures (valK)∗(c1(L,∥⋅∥l)n∧δXΣ)({\operatorname{val}}_{K})_{\ast}(c_{1}(L,\|\cdot\|_{l})^{n}\land\delta_{X_{\Sigma}}) converge to the measure μ\mu on NΣN_{\Sigma}. Proposition 2.37 implies that the measure of XΣan∖X0anX_{\Sigma}^{{\text{\rm an}}}\setminus X_{0}^{{\text{\rm an}}} with respect to c1​(L¯)n∧δXΣc_{1}({\overline{L}})^{n}\land\delta_{X_{\Sigma}} is zero. Therefore NΣ∖NℝN_{\Sigma}\setminus N_{\mathbb{R}} has μ\mu-measure zero. Denote ψl=ψ(∥⋅∥l)𝕊\psi_{l}=\psi_{(\|\cdot\|_{l})_{\mathbb{S}}}. By Proposition 3.108, the measures ℳM​(ψl)\mathcal{M}_{M}(\psi_{l}) converge to the measure ℳM​(ψ)\mathcal{M}_{M}(\psi). Thus μ|Nℝ=n!​ℳM​(ψ)\mu|_{N_{\mathbb{R}}}=n!\mathcal{M}_{M}(\psi). If we add to this that the measure of NΣ∖NℝN_{\Sigma}\setminus N_{\mathbb{R}} is zero, we deduce equation (5.82). The last statement of the theorem is clear from Theorem 5.33 and Theorem 5.70. ∎

We end this section by characterizing integrable metrics.

Corollary 5.83.

Let Σ\Sigma be a complete fan. Then the map ∥⋅∥↦ψ∥⋅∥\|\cdot\|\mapsto\psi_{\|\cdot\|} is a bijection between the space of integrable toric metrics on 𝒪​(DΨ)an\mathcal{O}(D_{\Psi})^{{\text{\rm an}}} and the space of functions ψ∈𝒟¯​(Nℝ)\psi\in{\overline{\mathscr{D}}}(N_{\mathbb{R}}) such that rec⁡(ψ)=Ψ\operatorname{rec}(\psi)=\Psi, were 𝒟¯​(Nℝ){\overline{\mathscr{D}}}(N_{\mathbb{R}}) is the space of functions of Definition 3.82.

5.8. Adelic toric metrics

We now turn to the global case. Let (𝕂,M𝕂)(\mathbb{K},M_{\mathbb{K}}) be an adelic field (Definition 2.47). We fix a complete fan Σ\Sigma in NℝN_{\mathbb{R}} and a virtual support function Ψ\Psi on Σ\Sigma. Let (L,s)(L,s) be the associated toric line bundle and section. If XX is a variety over 𝕂\mathbb{K} and v∈M𝕂v\in M_{\mathbb{K}} we will denote by Xan,vX^{{\text{\rm an}},v} its analytification with respect to vv. Analogously 𝕊an,v\mathbb{S}^{{\text{\rm an}},v} will denote the compact subtorus of 𝕋an,v\mathbb{T}^{{\text{\rm an}},v}.

Definition 5.84.

A toric metric on LL is a family (∥⋅∥v)v∈M𝕂(\|\cdot\|_{v})_{v\in M_{\mathbb{K}}}, where ∥⋅∥v\|\cdot\|_{v} is a toric metrics on LvanL_{v}^{{\text{\rm an}}}. A toric metric is called adelic if ψ∥⋅∥v=Ψ\psi_{\|\cdot\|_{v}}=\Psi for all but finitely many vv.

Theorem 5.85.

Let (𝕂,M𝕂)(\mathbb{K},M_{\mathbb{K}}) be a global field. A toric metric on LL is quasi-algebraic (Definition 2.52) if and only if it is an adelic toric metric.

Proof.

Let (∥⋅∥v)v∈M𝕂(\|\cdot\|_{v})_{v\in M_{\mathbb{K}}} be a metric on LL and write L¯=(L,(∥⋅∥v)v∈M𝕂){\overline{L}}=(L,(\|\cdot\|_{v})_{v\in M_{\mathbb{K}}}). Suppose first that L¯{\overline{L}} is toric and quasi-algebraic. Let S⊂M𝕂S\subset M_{\mathbb{K}} be a finite set containing the Archimedean places, 𝕂S∘\mathbb{K}^{\circ}_{S} as in Definition 2.51, e≥1e\geq 1 an integer and (𝒳,ℒ)({\mathcal{X}},{\mathcal{L}}) a proper model over 𝕂S∘\mathbb{K}^{\circ}_{S} of (XΣ,L⊗e)(X_{\Sigma},L^{\otimes e}) so that ∥⋅∥v\|\cdot\|_{v} is induced by the localization ℒv{\mathcal{L}}_{v} for all v∉Sv\notin S. Over 𝕂\mathbb{K}, there is an isomorphism from (𝒳,ℒ)({\mathcal{X}},{\mathcal{L}}) to the canonical model (𝒳Σ,ℒe​Ψ)({\mathcal{X}}_{\Sigma},{\mathcal{L}}_{e\Psi}). Since 𝕂S∘\mathbb{K}^{\circ}_{S} is Noetherian, this isomorphism and its inverse are defined over 𝕂S′∘\mathbb{K}^{\circ}_{S^{\prime}} for certain finite subset S′S^{\prime} containing SS. Thus, enlarging the finite set SS if necessary, we can suppose without loss of generality that (𝒳,ℒ)({\mathcal{X}},{\mathcal{L}}) agrees with the canonical model (𝒳Σ,ℒe​Ψ)({\mathcal{X}}_{\Sigma},{\mathcal{L}}_{e\Psi}). Hence, ∥⋅∥v=∥⋅∥v,e​Ψ1/e=∥⋅∥v,Ψ\|\cdot\|_{v}=\|\cdot\|_{v,e\Psi}^{1/e}=\|\cdot\|_{v,\Psi} for all places v∉Sv\notin S. In consequence, it is an adelic toric metric.

Conversely, suppose that L¯{\overline{L}} is a toric adelic metrized line bundle. Let SS be the union of the set of Archimedean places and {v∈M𝕂|ψv≠Ψ}\{v\in M_{\mathbb{K}}|\psi_{v}\neq\Psi\}. By definition, this is a finite set. Let (𝒳Σ,ℒΨ)({\mathcal{X}}_{\Sigma},{\mathcal{L}}_{\Psi}) be the canonical model over 𝕂S∘\mathbb{K}^{\circ}_{S} of (XΣ,L)(X_{\Sigma},L). Then ∥⋅∥v\|\cdot\|_{v} is the metric induced by this model, for all v∉Sv\notin S. Hence L¯{\overline{L}} is quasi-algebraic. ∎

Corollary 5.86.

Let LL be as before.

  1. (1)

    There is a bijection between the set of approachable adelic toric metric on LL and the set of families of continuous concave functions {ψv}v\{\psi_{v}\}_{v} on NℝN_{\mathbb{R}} such that |ψv−Ψ||\psi_{v}-\Psi| is bounded and ψv=Ψ\psi_{v}=\Psi for all but finitely many vv.

  2. (2)

    There is a bijection between the set of approachable adelic toric metric on LL and the set of families of continuous concave functions {ψv∨}v\{\psi^{\vee}_{v}\}_{v} on ΔΨ\Delta_{\Psi} such that ψv∨=0\psi^{\vee}_{v}=0 for all but finitely many vv.

Proof.

This follows from Theorem 5.85 and Theorem 5.73. ∎

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