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15.37.12 Common envelopes and dominated continuityBD25F1249EB6

Let $u_ j\in \mathcal E_\varphi $ converge in $L^1$, with measures dominated by one finite non-pluripolar measure $\nu $. To keep the limit in $\mathcal E_\varphi $, we construct, after passing to a subsequence, a common lower envelope in this class. Partitioning the contact set of a finite rooftop according to the obstacle it touches shows that the rooftop measure is again dominated by $\nu $, with no factor depending on the number of obstacles. A summable integration error, combined with the lower mass bound $\kappa $, then prevents the stretched rooftops from collapsing, uniformly in the number of obstacles.

Lemma 15.37.13.E5ED88B4042A Suppose $u_ j\in \mathcal E_\varphi $, $u_ j\to u\in \mathrm{PSH}(X,\theta )$ in $L^1(X)$, and $\mu _{u_ j}\leq \nu $ for a fixed finite non-pluripolar measure $\nu $. There is a subsequence, denoted again by $u_ j$, such that

\[ h=P_\theta \left(\inf _ j u_ j\right)\in \mathcal E_\varphi . \]

In particular $u\in \mathcal E_\varphi $.

Proof. We first bound stretched rooftops of the tail of the sequence from below and then add the finitely many remaining terms.

The suprema of an $L^1$-convergent sequence are bounded, so (15.37.2) gives a constant $C$ with $u_ j\leq \varphi +C$ for all $j$. After a common translation we may assume $u_ j\leq \varphi \leq 0$, and then $u\leq \varphi $. Since $\mu _{u_ j}\leq \nu $, lemma 5.44.2 gives

\[ I_ j=\int _ X|\mathrm{e}^{u_ j}-\mathrm{e}^ u|\, \mathrm{d}\mu _{u_ j}\longrightarrow 0. \]

We extract, once and for all, a subsequence with $I_ j\leq 2^{-j}$ along which $u_ j\to u$ almost everywhere for smooth volume.

For $N\geq j$ put $p_{j,N}=P_\theta (u_ j,\ldots ,u_ N)$. These rooftops belong to $\mathcal E_\varphi $ by proposition 16.28.64. Partition their contact sets according to the first index at which the minimum is attained. Ordered contact on these disjoint pieces gives both

EEB0F315C2A3 15.37.14
\begin{equation} \mu _{p_{j,N}}\leq \nu , \qquad \int _ X|\mathrm{e}^{p_{j,N}}-\mathrm{e}^ u|\, \mathrm{d}\mu _{p_{j,N}} \leq \sum _{\ell =j}^ N I_\ell \leq 2^{1-j}. \end{equation}

The first bound has no factor $N$, because each piece is controlled by the restriction of the same measure $\nu $ to that piece.

Fix a real number $B\geq 1$ and set $r_{j,N}=Q_ B(p_{j,N},\varphi )$. It belongs to $\mathcal E_\varphi $ by the stretching lemma, so $\mu _{r_{j,N}}(X)\geq \kappa $. With $D_{j,N}=\{ B^{-1}r_{j,N}+(1-B^{-1})\varphi =p_{j,N}\} $, contact support and positivity give

\[ \mu _{r_{j,N}}\leq B^ n\mathbf1_{D_{j,N}}\mu _{p_{j,N}} \leq B^ n\nu . \]

On this contact set, $\varphi \leq 0$ gives $\mathrm{e}^{p_{j,N}}\leq \mathrm{e}^{r_{j,N}/B}$. Consequently

9D97DEE5D482 15.37.15
\begin{equation} \int _ X\mathrm{e}^ u\, \mathrm{d}\mu _{r_{j,N}} \leq B^ n2^{1-j} +B^ n\nu (X)\exp \! \left(\frac{\sup _ X r_{j,N}}B\right). \end{equation}

On the other hand, choose $K>0$ with $B^ n\nu (\{ u\leq -K\} )<\kappa /2$; this is possible because $u\not\equiv -\infty $ and $\nu $ does not charge its pole set. The measure domination then gives $\mu _{r_{j,N}}(\{ u\leq -K\} )<\kappa /2$, and the lower mass bound yields

\[ \int _ X\mathrm{e}^ u\, \mathrm{d}\mu _{r_{j,N}}\geq \mathrm{e}^{-K}\kappa /2. \]

Choose $j$ so large that $B^ n2^{1-j}<\mathrm{e}^{-K}\kappa /4$. Then (15.37.15) bounds $\sup _ Xr_{j,N}$ from below, independently of $N$. Since the sequence decreases in $N$ and is bounded above by $\varphi $, its limit $R$ is not identically $-\infty $. It satisfies, for every $\ell \geq j$,

5FB1B43EDC20 15.37.16
\begin{equation} B^{-1}R+(1-B^{-1})\varphi \leq u_\ell , \qquad R\leq \varphi . \end{equation}

The second inequality follows already from $r_{j,N}\leq p_{j,N}\leq \varphi $.

It remains to include the finitely many earlier terms and to verify every defining condition of the relative class. Fix $b\geq 1$, apply the preceding construction with $B=2b$, and let $j$ and $R$ be as above. If $j>1$, let $p_0=P_\theta (u_1,\ldots ,u_{j-1})$ and $S=Q_{2b}(p_0,\varphi )$. By the finite-rooftop and stretching lemmas, neither is identically $-\infty $, and $S\leq \varphi $. If $j=1$, set $S=\varphi $. The potential $H=(R+S)/2$ is $\theta $-plurisubharmonic. For a tail index $\ell \geq j$ we use (15.37.16) and $S\leq \varphi $; for an earlier index we use the analogous inequality for $S$ and $R\leq \varphi $. In either case,

\[ b^{-1}H+(1-b^{-1})\varphi \leq u_\ell \quad \hbox{for every }\ell \geq 1. \]

For $b=1$ this shows that $h=P_\theta (\inf _\ell u_\ell )$ is not identically $-\infty $. For general $b$ the left side is a competitor for $h$, so the same inequality holds with $h$ in place of every $u_\ell $; this is the defining condition of the relative class for $b$. Also $h\leq \varphi $. Thus $h\in \mathcal E_\varphi $.

Finally $h\leq u_ j$ for all $j$, so the almost-everywhere convergence and lemma 5.24.3 give $h\leq u\leq \varphi $. Upward stability proves $u\in \mathcal E_\varphi $. Undoing the common translation proves the lemma as stated. $\square$

Once a common lower envelope is available, convergence in capacity follows from a single integral condition. The proof uses the zero-domination lemma, so infinite masses are allowed.

Proposition 15.37.17.D220D741C684 Suppose $u_ j\in \mathcal E_\varphi $ and, for a fixed $h\in \mathcal E_\varphi $ and a constant $C$,

\[ h\leq u_ j\leq \varphi +C,\qquad u_ j\longrightarrow u\in \mathrm{PSH}(X,\theta )\quad \hbox{in }L^1(X). \]

If

\[ I_ j:=\int _ X|\mathrm{e}^{u_ j}-\mathrm{e}^ u|\, \mu _{u_ j}\longrightarrow 0, \]

then $u\in \mathcal E_\varphi $ and $u_ j\to u$ in capacity.

Proof. The bounds pass to $u$ almost everywhere along a subsequence, and then everywhere by lemma 5.24.3; upward stability gives $u\in \mathcal E_\varphi $. After translating the entire family and its bounds by a common constant, we may assume that all potentials are nonpositive.

It suffices to prove convergence in capacity along a further subsequence of every subsequence. Extract so that $I_ j\leq 2^{-j}$ and $u_ j\to u$ almost everywhere for smooth volume, and form

\[ p_{j,N}=P_\theta (u_ j,\ldots ,u_ N),\qquad p_ j=P_\theta \left(\inf _{\ell \geq j}u_\ell \right). \]

All these envelopes lie above $h$ and below $\varphi +C$; hence none of them is identically $-\infty $, and all belong to $\mathcal E_\varphi $. Partition the contact set of $p_{j,N}$ according to the first index $\ell $ with $p_{j,N}=u_\ell $. Ordered contact on each part gives

\[ \int _ X|\mathrm{e}^{p_{j,N}}-\mathrm{e}^ u|\, \mu _{p_{j,N}} \leq \sum _{\ell =j}^ N I_\ell \leq 2^{1-j}. \]

Only integrals of nonnegative functions occur here, so the estimate holds even if a rooftop has infinite mass.

As $N\to \infty $, $p_{j,N}\downarrow p_ j$; as $j\to \infty $, the $p_ j$ increase, and their regularized limit $p$ is not identically $-\infty $. Both monotone limits hold in capacity by lemma 5.29.19. Moreover $h\leq p\leq u\leq \varphi +C$, where $p\leq u$ follows from the almost-everywhere convergence of the extracted $u_ j$. Thus $p\in \mathcal E_\varphi $.

Apply lemma 13.14.8, first as $N\to \infty $ and then as $j\to \infty $, with the bounded quasi-continuous weights in the preceding estimate. These weights converge in capacity because the exponential is Lipschitz on a common upper half-line. We obtain

\[ \int _ X|\mathrm{e}^ p-\mathrm{e}^ u|\, \mu _ p=0, \qquad \mu _ p(\{ p<u\} )=0. \]

The second equality follows off the poles, which the extended measures ignore. The zero-domination lemma lemma 15.37.9 now gives $p=u$; no finiteness of $\mu _ p$ is needed.

Finally, the upper envelopes $U_ j=(\sup _{\ell \geq j}u_\ell )^*$ decrease to $u$, by theorem 5.25.2 and the almost-everywhere convergence. Applying lemma 5.29.19 to $p_ j\uparrow u$ and $U_ j\downarrow u$, the inequalities $p_ j\leq u_ j\leq U_ j$ give convergence in capacity along this subsequence, and hence for the original sequence. $\square$

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