ScalingStacks

6. Applications to regularity [05BJ]

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6. Applications to regularity

In this section we use the connection of the non-archimedean Monge-Ampère operator to the real one to transfer two known regularity results for the solutions of the real Monge-Ampère equation to the non-archimedean case. Again KK denotes a non-archimedean non-trivially valued field.

Definition 6.1.

Let Ω⊆ℝn\Omega\subseteq\mathbb{R}^{n} be an open subset and k∈ℕk\in\mathbb{N}. We write Ck​(Ω)C^{k}(\Omega) for the space of real valued, kk times continuously differentiable functions on Ω\Omega. Furthermore we denote by Ll​o​c1​(Ω)L_{loc}^{1}(\Omega) the space of locally integrable functions on Ω\Omega i.e. functions f:Ω→ℝf:\Omega\rightarrow\mathbb{R} such that the restriction of ff to any compact subset of Ω\Omega is integrable. Let f,g∈Ll​o​c1​(Ω)f,g\in L_{loc}^{1}(\Omega) and β∈ℕn\beta\in\mathbb{N}^{n}. We say that gg is the β\beta-th weak derivative of ff if for any test function φ∈C∞​(Ω)\varphi\in C^{\infty}(\Omega) with compact support we have

∫Ωf​Dβ​φ​𝑑𝒙=(−1)|β|​∫Ωg​φ​𝑑𝒙\int_{\Omega}fD^{\beta}\varphi\;\boldsymbol{dx}=(-1)^{|\beta|}\int_{\Omega}g\varphi\;\boldsymbol{dx}

where 𝒅​𝒙\boldsymbol{dx} denotes the Lebesgue measure on ℝn\mathbb{R}^{n}. We denote by Wl​o​ck,1​(Ω)W^{k,1}_{loc}(\Omega) the space of locally integrable functions on Ω\Omega whose weak derivatives exist up to order kk.

Proposition 6.2.

Let XX be an nn-dimensional proper variety over KK and L¯\overline{L} a line bundle with a fixed formal metric. Let μ\mu be a positive Borel measure on XanX^{\textup{an}} and φ\varphi a continuous function on XanX^{\textup{an}} such that the metric on L¯⊗𝒪¯φ\overline{L}\otimes\overline{\mathcal{O}}^{\varphi} is semipositive and solving the equation

c1​(L¯⊗𝒪¯φ)n=μ.c_{1}(\overline{L}\otimes\overline{\mathcal{O}}^{\varphi})^{n}=\mu.

Let τ\tau be an nn-dimensional open face of some skeleton Δ\Delta associated to a strongly nondegenerate strictly polystable formal model 𝔛\mathfrak{X} of XanX^{\textup{an}}. Suppose that 𝔛\mathfrak{X} is algebraic, L¯\overline{L} has a model on 𝔛\mathfrak{X} and λ⋅𝐝​𝐱≤μ≤Λ⋅𝐝​𝐱\lambda\cdot\boldsymbol{dx}\leq\mu\leq\Lambda\cdot\boldsymbol{dx} on τ\tau for some λ,Λ>0\lambda,\Lambda>0 where 𝐝​𝐱\boldsymbol{dx} denotes the Lebesgue measure on τ\tau. Assume that φ=φ∘p𝔛\varphi=\varphi\circ p_{\mathfrak{X}}. Then φ∈Wl​o​c2,1​(τ)\varphi\in W^{2,1}_{loc}(\tau).

Proof.

By Corollary B.4 φ\varphi is convex on every closed face of Δ\Delta. Note that the metric on L¯\overline{L} is trivial on p𝔛−1​(τ)p_{\mathfrak{X}}^{-1}(\tau). Hence we can apply Corollary 5.7 to get

μ=c1​(L¯⊗𝒪¯φ)n=deg⁡(S)⋅n!⋅MA⁡(φ)\mu=c_{1}(\overline{L}\otimes\overline{\mathcal{O}}^{\varphi})^{n}=\Deg(S)\cdot n!\cdot\MA(\varphi)

on τ\tau where SS is the stratum of 𝔛~\tilde{\mathfrak{X}} corresponding to τ\tau. Now the claim follows from the corresponding fact in the real case [Moo15, Theorem 1.2]. ∎

Remark 6.3.

The condition φ=φ∘p𝔛\varphi=\varphi\circ p_{\mathfrak{X}} is not automatic as shown by a counterexample of Burgos and Sombra, see [GJKM19, Appendix A].

Proposition 6.4.

Let XX be a smooth projective curve over KK and L¯\overline{L} a line bundle with a fixed formal metric. Let μ\mu be a positive Borel measure on XanX^{\textup{an}} and φ\varphi a continuous function on XanX^{\textup{an}} such that the metric on L¯⊗𝒪¯φ\overline{L}\otimes\overline{\mathcal{O}}^{\varphi} is semipositive and solving the equation

c1​(L¯⊗𝒪¯φ)=μ.c_{1}(\overline{L}\otimes\overline{\mathcal{O}}^{\varphi})=\mu.

If τ\tau is an open face of the skeleton Δ\Delta of a strictly semistable algebraic model 𝒳\mathscr{X} of XanX^{\textup{an}} on which L¯\overline{L} has an algebraic model, μ\mu is supported on Δ\Delta and μ=f⋅𝐝​𝐱\mu=f\cdot\boldsymbol{dx} on τ\tau for some positive function f∈Ck​(τ)f\in C^{k}(\tau) where 𝐝​𝐱\boldsymbol{dx} denotes the Lebesgue measure on τ\tau then φ∈Ck+2​(τ)\varphi\in C^{k+2}(\tau).

Proof.

By [GJKM19, Proposition 1.2] we have φ=φ∘p𝔛\varphi=\varphi\circ p_{\mathfrak{X}}. As in the previous result φ\varphi is convex on τ\tau and

μ=c1​(L¯⊗𝒪¯φ)=deg⁡(S)⋅MA⁡(φ)\mu=c_{1}(\overline{L}\otimes\overline{\mathcal{O}}^{\varphi})=\Deg(S)\cdot\MA(\varphi)

on τ\tau. But a solution to the archimedean Monge-Ampère problem is given by a second antiderivative of ff and the solution is unique up to addition of a linear function. Hence φ∈Ck+2​(τ)\varphi\in C^{k+2}(\tau) and deg⁡(S)⋅φ′′=f\Deg(S)\cdot\varphi^{\prime\prime}=f. ∎

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