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16.4 Properties of the $P$-envelope666167293D79

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Let $\theta ,\theta _1,\theta _2$ be smooth closed real $(1,1)$-forms on $X$.

Proposition 16.4.1.055CAE14F80F Let $\pi \colon Y\rightarrow X$ be a proper bimeromorphic morphism from a Kähler manifold $Y$ to $X$. Then for any $\varphi \in \mathrm{PSH}(X,\theta )$, we have

\[ P_{\pi ^*\theta }[\pi ^*\varphi ]=\pi ^*P_{\theta }[\varphi ]. \]

In particular, a potential $\varphi \in \mathrm{PSH}(X,\theta )_{>0}$ is model if and only if $\pi ^*\varphi \in \mathrm{PSH}(Y,\pi ^*\theta )_{>0}$ is model.

Proof. By proposition 5.17.8, every $\chi \in \mathrm{PSH}(Y,\pi ^*\theta )$ is of the form $\chi =\pi ^*\psi $ for a unique $\psi \in \mathrm{PSH}(X,\theta )$. Since $\pi $ is surjective, $\chi \leq 0$ if and only if $\psi \leq 0$. Moreover,

\[ \chi \preceq \pi ^*\varphi \Longleftrightarrow \psi \preceq \varphi . \]

Thus the candidates defining $P_{\pi ^*\theta }[\pi ^*\varphi ]$ are exactly the pull-backs of the candidates defining $P_\theta [\varphi ]$, and hence

\[ P_{\pi ^*\theta }[\pi ^*\varphi ]=\pi ^*P_\theta [\varphi ]. \]

Finally, the non-pluripolar mass is preserved under bimeromorphic pull-back by proposition 13.13.4. Therefore $\varphi $ is model of positive mass if and only if $\pi ^*\varphi $ is. $\square$

We have the following concavity property of the $P$-envelope.

Proposition 16.4.2.CF5FECD1B547

  1. C852A00815E6

    Suppose that $\varphi \in \mathrm{PSH}(X,\theta )$ and $\lambda \in \mathbb {R}_{>0}$. Then

    \[ P_{\lambda \theta }[\lambda \varphi ]=\lambda P_{\theta }[\varphi ]. \]
  2. 054C3F14E799

    Suppose that $\varphi _1\in \mathrm{PSH}(X,\theta _1)$ and $\varphi _2\in \mathrm{PSH}(X,\theta _2)$. Then

    \[ P_{\theta _1+\theta _2}[\varphi _1+\varphi _2]\geq P_{\theta _1}[\varphi _1]+P_{\theta _2}[\varphi _2]. \]
  3. 7E5E2644837B

    Suppose that $\varphi ,\psi \in \mathrm{PSH}(X,\theta )$ and $\varphi \preceq \psi $. Then

    \[ P_{\theta }[\varphi ]\leq P_{\theta }[\psi ]. \]

Proof. 1 This follows by rescaling the candidates in the definition of the $P$-envelope.

2 Suppose that $\psi _1\in \mathrm{PSH}(X,\theta _1)$ and $\psi _2\in \mathrm{PSH}(X,\theta _2)$ satisfy

\[ \psi _ i\leq 0,\quad \psi _ i\preceq \varphi _ i \]

for $i=1,2$. Then

\[ \psi _1+\psi _2\leq 0,\quad \psi _1+\psi _2\preceq \varphi _1+\varphi _2. \]

It follows from (16.3.6) that

\[ \psi _1+\psi _2\leq P_{\theta _1+\theta _2}[\varphi _1+\varphi _2]. \]

Since $\psi _1$ and $\psi _2$ are arbitrary, we conclude.

3 This follows by inclusion of the defining candidate sets. $\square$

Proposition 16.4.3.8EB68D9BFB64 Let $(\varphi _ j)_{j\in I}$ be a decreasing net of potentials in $\mathrm{PSH}(X,\theta )$ satisfying $P_{\theta }[\varphi _ j]=\varphi _ j$ for each $j\in I$. Set $\varphi \coloneqq \inf _{j\in I} \varphi _ j$. Then $P_{\theta }[\varphi ]=\varphi $.

Proof. Since $P_{\theta }[\varphi _ j]=\varphi _ j$, we have $\sup _ X\varphi _ j=0$. By corollary 5.17.5, we have $\varphi \in \mathrm{PSH}(X,\theta )$, and $\varphi \leq 0$. Therefore, for each $j\in I$,

\[ \varphi \leq P_{\theta }[\varphi ]\leq P_{\theta }[\varphi _ j] =\varphi _ j. \]

Therefore, $\varphi =P_{\theta }[\varphi ]$. $\square$

Proposition 16.4.4.048490BEAC8C Let $(\epsilon _ i)_{i\in I}$ be a decreasing net in $\mathbb {R}_{\geq 0}$ with limit $0$. Take a Kähler form $\omega $ on $X$. Consider a decreasing net $(\varphi _ i)_{i\in I}$ with $\varphi _ i\in \mathrm{PSH}(X,\theta +\epsilon _ i \omega )$ satisfying

B1E48C713966 16.4.5
\begin{equation} P_{\theta +\epsilon _ i\omega }\left[\varphi _ i\right]=\varphi _ i \end{equation}

for every $i\in I$. Set $\varphi \coloneqq \inf _{i\in I}\varphi _ i$. Then $P_{\theta }[\varphi ]=\varphi $, and

243BB43027AE 16.4.6
\begin{equation} \lim _{i\in I}\int _ X \left(\theta + \epsilon _ i \omega \right)^ n_{\varphi _ i}=\int _ X \theta _{\varphi }^ n. \end{equation}

Moreover, if $\int _ X \theta _{\varphi }^ n>0$, then for any prime divisor $E$ over $X$, we have

C4257CD1FB0B 16.4.7
\begin{equation} \lim _{i\in I} \nu \left(\varphi _ i,E\right)=\nu (\varphi ,E). \end{equation}
Note that both (16.4.6) and (16.4.7) fail without the assumption (16.4.5).

Proof. We first observe that $\varphi \in \mathrm{PSH}(X,\theta )$. In fact, for each $i_0\in I$, the tail $(\varphi _ i)_{i\geq i_0}$ lies in $\mathrm{PSH}(X,\theta +\epsilon _{i_0}\omega )$ and decreases to $\varphi $. Since $\sup _ X\varphi _ i=0$ by (16.4.5), the limit is not identically $-\infty $. Thus $\varphi \in \mathrm{PSH}(X,\theta +\epsilon _{i_0}\omega )$ for every $i_0\in I$. Since $\epsilon _{i_0}\to 0$, it follows that $\varphi \in \mathrm{PSH}(X,\theta )$. For every $i\in I$ we have

\[ P_{\theta }[\varphi ]\leq P_{\theta +\epsilon _ i\omega }[\varphi ]\leq P_{\theta +\epsilon _ i\omega }[\varphi _ i]=\varphi _ i. \]

Therefore, $P_{\theta }[\varphi ]\leq \varphi $. The reverse inequality is trivial. Hence $P_{\theta }[\varphi ]=\varphi $.

By the monotonicity theorem theorem 13.13.11 and the multi-linearity of the non-pluripolar product proposition 13.11.4 6, we have

\[ \varliminf _{i\in I} \int _ X \left(\theta + \epsilon _ i \omega \right)^ n_{\varphi _ i} \geq \varliminf _{i\in I} \int _ X \left(\theta + \epsilon _ i \omega \right)^ n_{\varphi } = \int _ X \theta _{\varphi }^ n. \]

We now argue the reverse inequality.

Fix $i_0\in I$. Since passing to the tail $i\geq i_0$ does not change the limsup, we have

\[ \begin{aligned} \varlimsup _{i\in I} \int _ X \left(\theta + \epsilon _ i \omega \right)^ n_{\varphi _ i}=& \varlimsup _{i\geq i_0} \int _{\left\{ \varphi _ i =0\right\} } \left(\theta + \epsilon _ i \omega \right)^ n_{\varphi _ i} \\ \leq & \varlimsup _{i\geq i_0} \int _{\left\{ \varphi _ i =0\right\} } \left(\theta + \epsilon _{i_0} \omega \right)^ n_{\varphi _ i}\\ \leq & \int _{\left\{ \varphi =0\right\} } \left(\theta + \epsilon _{i_0} \omega \right)^ n_{\varphi }, \end{aligned} \]

where in the first line we used (16.4.5) and theorem 16.3.12, and in the last line we used the fact that $\varphi _ i \searrow \varphi $ on the tail $i\geq i_0$, and on this tail, $\varphi _ i \to \varphi $ in $L^1$ as well by corollary 5.17.5, and therefore, corollary 13.13.16 is applicable. Taking the limit with respect to $i_0$, we arrive at the desired conclusion:

\[ \varlimsup _{i\in I} \int _{X} \left(\theta + \epsilon _ i \omega \right)^ n_{\varphi _ i} \leq \varliminf _{i_0\in I}\int _{\{ \varphi =0\} } \left(\theta + \epsilon _{i_0} \omega \right)^ n_{\varphi } = \int _{\{ \varphi =0\} } \theta ^ n_{\varphi } \leq \int _{X} \theta ^ n_{\varphi }, \]

where the equality follows from the multi-linearity of the non-pluripolar product proposition 13.11.4 6 and the last inequality follows from theorem 16.3.12. This finishes the proof of (16.4.6).

It remains to argue (16.4.7). Fix $i_0\in I$. By proposition 5.17.7, there is a constant $B>0$ such that

\[ \nu (\psi ,E)\leq B,\quad \psi \in \mathrm{PSH}(X,\theta +\epsilon _{i_0}\omega ). \]

By 13.13.30 and (16.4.6), for any $\delta \in (0,1)$ there exists $i_{\delta }\geq i_0$ such that for all $i\geq i_{\delta }$ there exists $\psi _ i \in \mathrm{PSH}(X,\theta +\epsilon _ i\omega )$ satisfying $(1-\delta ) \varphi _ i + \delta \psi _ i \leq \varphi $. This implies that for $i\geq i_{\delta }$ we have

\[ (1-\delta )\nu (\varphi _ i,E) + \delta \nu (\psi _ i,E) \geq \nu (\varphi ,E) \geq \nu (\varphi _ i,E). \]

Since $\psi _ i\in \mathrm{PSH}(X,\theta +\epsilon _{i_0}\omega )$ for $i\geq i_{\delta }$, we get

\[ \varliminf _{i\in I}\nu (\varphi _ i,E)\geq \frac{\nu (\varphi ,E)-\delta B}{1-\delta }. \]

Letting $\delta \searrow 0$ gives $\varliminf _{i\in I}\nu (\varphi _ i,E)\geq \nu (\varphi ,E)$. The reverse inequality follows from $\varphi \leq \varphi _ i$, and hence we conclude (16.4.7). $\square$

Corollary 16.4.8.953C40C3B9B8 Let $\varphi \in \mathrm{PSH}(X,\theta )_{>0}$ be a model potential. Let $\omega $ be a Kähler form on $X$. Then

\[ \varphi =\inf _{\epsilon >0} P_{\theta +\epsilon \omega }[\varphi ]. \]

Proof. Set

\[ \eta \coloneqq \inf _{\epsilon >0}P_{\theta +\epsilon \omega }[\varphi ]. \]

Since $\varphi $ is model, $\varphi =P_{\theta }[\varphi ]\leq P_{\theta +\epsilon \omega }[\varphi ]$ for every $\epsilon >0$, hence $\varphi \leq \eta \leq 0$.

Next we prove the reverse direction. Applying proposition 16.4.4 to the decreasing net $(P_{\theta +\epsilon \omega }[\varphi ])_{\epsilon >0}$ and using proposition 16.3.10, we get

\[ P_\theta [\eta ]=\eta ,\quad \int _ X\theta _\eta ^ n=\int _ X\theta _\varphi ^ n. \]

Thus $\eta $ is a candidate in the characterization theorem 16.3.15 of $P_\theta [\varphi ]$. Hence $\eta \leq P_\theta [\varphi ]=\varphi $. $\square$

Proposition 16.4.9.3654A10A0CCC Let $(\varphi _ i)_{i\in I}$ be an increasing net of potentials in $\mathrm{PSH}(X,\theta )_{>0}$ uniformly bounded from above. Let $\varphi \coloneqq \operatorname *{sup}_{i\in I}{}\! {}^{*}\varphi _ i$. Then

\[ \operatorname *{sup}_{i\in I}{}\! {}^{*} P_{\theta }[\varphi _ i]=P_{\theta }[\varphi ]. \]

In particular, if $\varphi _ i$ is model for all $i\in I$, then so is $\varphi $.

Proof. We may assume that $I$ is infinite since otherwise, there is nothing to prove.

We write

\[ \eta \coloneqq \operatorname *{sup}_{i\in I}{}\! {}^{*} P_{\theta }[\varphi _ i]. \]

Then it is clear that $\eta \leq P_{\theta }[\varphi ]$.

By corollary 13.13.12, we have

\[ \lim _{i\in I} \int _ X\theta _{\varphi _ i}^ n=\int _ X\theta _{\varphi }^ n>0. \]

We may assume that for each $i\in I$, $\int _ X\theta _{\varphi _ i}^ n<\int _ X\theta _{\varphi }^ n$, since otherwise $P_{\theta }[\varphi _ i]=P_{\theta }[\varphi ]$ by theorem 16.3.15, and the same holds for all $j\geq i$; in that case there is nothing to prove.

So by 13.13.30, we can find a decreasing net $\epsilon _ i\searrow 0$ ($i\in I$) with $\epsilon _ i\in (0,1)$ and $\psi _ i\in \mathrm{PSH}(X,\theta )$ ($i\in I$) such that for all $i\in I$,

\[ (1-\epsilon _ i) \varphi +\epsilon _ i\psi _ i\leq \varphi _ i. \]

We may, for example, take

DC0519B3B917 16.4.10
\begin{equation} \epsilon _ i^{-1}=\frac{1}{2}\left( 1+\left(\frac{\int _ X \theta _{\varphi }^ n}{\int _ X \theta _{\varphi }^ n-\int _ X \theta _{\varphi _ i}^ n}\right)^{1/n} \right). \end{equation}

By the concavity property of the envelope proposition 16.4.2, we have

\[ P_{\theta }[\varphi ]+\epsilon _ i P_{\theta }[\psi _ i]\leq (1-\epsilon _ i) P_{\theta }[\varphi ]+\epsilon _ i P_{\theta }[\psi _ i]\leq P_{\theta }[\varphi _ i]\leq \eta . \]

Each $P_{\theta }[\psi _ i]$ has supremum $0$, hence the family is bounded in $L^1$ by proposition 5.17.3. Thus $\epsilon _ iP_{\theta }[\psi _ i]\to 0$ in $L^1$. The previous inequality then gives $P_{\theta }[\varphi ]\leq \eta $ almost everywhere, and hence everywhere by proposition 5.14.6. $\square$

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