Theorem 13.15.13.8B2A9680933C Let $u_ j,u\in \mathrm{PSH}(X,\omega )$ be nonpositive and suppose $u_ j\to u$ in capacity. Assume
Then $\mu _ u$ is finite and $\mu _{u_ j}\rightharpoonup \mu _ u$.
8B2A9680933CTheorem 13.15.13.8B2A9680933C Let $u_ j,u\in \mathrm{PSH}(X,\omega )$ be nonpositive and suppose $u_ j\to u$ in capacity. Assume
Then $\mu _ u$ is finite and $\mu _{u_ j}\rightharpoonup \mu _ u$.
Proof. Choose $T_0$ such that every tail $\mu _{u_ j}(\{ u_ j<-T\} )$ with $T\geq T_0$ is at most one. By lemma 13.15.3, $\mu _{u_ j}(X)\leq C(1+T_0)^{r_ n}+1$, so the tail condition already gives a uniform bound for the total masses.
With the cutoffs $\eta _ T$ of (13.15.10), the fixed-level argument in the proof of theorem 13.15.9, applied with $w\equiv 1$, gives
The masses of the measures on the left are bounded by the uniform bound for the total masses. Since $\eta _ T(-u)$ increases to one off the pole set as $T\to \infty $, monotone convergence proves $\mu _ u(X)<+\infty $.
For a continuous test function $f:X\to \mathbb R$, the error made by inserting $\eta _ T(-u_ j)$ is at most $\| f\| _\infty \mu _{u_ j}(\{ u_ j<-T\} )$, which is small for large $T$, uniformly in $j$. For the limit potential, the corresponding error tends to zero because $\mu _ u$ is finite and does not charge the pole set. Let first $j\to \infty $ with $T$ fixed, and then $T\to \infty $. $\square$
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