ScalingStacks

8.2. Existence [01C2]

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8.2. Existence

As in [BBGZ09], the strategy is to first use a variational argument going back to Alexandrov [Ale38] in order to produce a solution φ∈ℰ1​(X,ω)\varphi\in\mathcal{E}^{1}(X,\omega).

Consider the functional Fμ:PSH(X,ω)→[−∞,+∞[F_{\mu}:\PSH(X,\omega)\to[-\infty,+\infty[ defined by

(8.3) Fμ​(φ):=Eω​(φ)−∫φ​μ.F_{\mu}(\varphi):=E_{\omega}(\varphi)-\int\varphi\mu.

We first claim that FμF_{\mu} is usc on PSH⁡(X,ω)\PSH(X,\omega). By Proposition 6.2, EωE_{\omega} is usc so that it is sufficient to prove φ↦∫φ​μ\varphi\mapsto\int\varphi\mu is continuous on PSH⁡(X,ω)\PSH(X,\omega). Pick a net φk→φ\varphi_{k}\to\varphi in PSH⁡(X,ω)\PSH(X,\omega), i.e. φk​(x)→φ​(x)\varphi_{k}(x)\to\varphi(x) for any x∈Xdivx\in X^{\mathrm{div}}. Since divisorial points are dense in Δ𝒳\Delta_{\mathcal{X}} by [JM10], and the family {φk|Δ𝒳}\{\varphi_{k}|_{\Delta_{\mathcal{X}}}\} is equicontinuous by Theorem 2.9, it follows that φk|Δ𝒳→φ|Δ𝒳\varphi_{k}|_{\Delta_{\mathcal{X}}}\to\varphi|_{\Delta_{\mathcal{X}}} uniformly. Whence ∫φk​μ→∫φ​μ\int\varphi_{k}\mu\to\int\varphi\mu since Δ𝒳\Delta_{\mathcal{X}} contains the support of μ\mu by assumption.

Now write PSH0⁡(X,ω):={φ∈PSH⁡(X,ω)∣supφ=0}\PSH_{0}(X,\omega):=\{\varphi\in\PSH(X,\omega)\mid\sup\varphi=0\}, and observe that Fμ​(φ+c)=Fμ​(φ)F_{\mu}(\varphi+c)=F_{\mu}(\varphi) for any constant cc by Proposition 6.2, so that supPSH⁡(X,ω)Fμ=supPSH0⁡(X,ω)Fμ\sup_{\PSH(X,\omega)}F_{\mu}=\sup_{\PSH_{0}(X,\omega)}F_{\mu}. Since FμF_{\mu} is usc, and PSH0⁡(X,ω)\PSH_{0}(X,\omega) is compact by Theorem 2.10, it actually attains its maximum. We can thus find φ∈PSH0⁡(X,ω)\varphi\in\PSH_{0}(X,\omega) such that

Fμ​(φ)=supPSH⁡(X,ω)Fμ.F_{\mu}(\varphi)=\sup_{\PSH(X,\omega)}F_{\mu}.

Clearly Eω​(φ)>−∞E_{\omega}(\varphi)>-\infty, so φ∈ℰ1​(X,ω)\varphi\in\mathcal{E}^{1}(X,\omega). Let us show that MA⁡(φ)=μ\MA(\varphi)=\mu. Pick any model function f≤0f\leq 0 on XX. For t∈𝐑t\in\mathbf{R}, consider the function

h⁡(t)=Eω∘Pω​(φ+t​f)−∫(φ+t​f)​μ.h(t)=E_{\omega}\circ P_{\omega}(\varphi+tf)-\int(\varphi+tf)\mu.

In view of Corollary 7.3, h⁡(t)h(t) is differentiable at t=0t=0 with derivative

h′​(0)=∫f​MA⁡(φ)−∫f​μ.h^{\prime}(0)=\int f\,\MA(\varphi)-\int f\,\mu.

But since Pω​(φ+t​f)≤φ+t​f≤0P_{\omega}(\varphi+tf)\leq\varphi+tf\leq 0, it follows that h⁡(t)≤Fμ∘Pω​(φ+t​f)≤Fμ​(φ)=h⁡(0)h(t)\leq F_{\mu}\circ P_{\omega}(\varphi+tf)\leq F_{\mu}(\varphi)=h(0) for all tt. Thus hh has a local maximum at t=0t=0, so h′​(0)=0h^{\prime}(0)=0, that is ∫f​μ=∫f​MA⁡(φ)\int f\mu=\int f\MA(\varphi). This implies MA⁡(φ)=μ\MA(\varphi)=\mu, as ff was an arbitrary model function.

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