Proof.
Step 1: proof of (2). Let $w_ j$, $\chi _ j$, $S$ and $\alpha _ j$ be as in (2), and put $f_ j=\chi _ j^2\mathrm e^{w_ j}$, so that $S=\sum _ jf_ j$. Then $\partial f_ j=\chi _ j\mathrm e^{w_ j}(\chi _ j\partial w_ j+2\partial \chi _ j)=\chi _ j\mathrm e^{w_ j}\alpha _ j$, so that $\partial S=\sum _ j\chi _ j\mathrm e^{w_ j}\alpha _ j$. Since $\chi _ j$ and $w_ j$ are real, $\bar\partial f_ j=\overline{\partial f_ j}=\chi _ j\mathrm e^{w_ j}\bar\alpha _ j$ with $\bar\alpha _ j=\chi _ j\bar\partial w_ j+2\bar\partial \chi _ j$, and
\[ \begin{aligned} \partial \bar\partial f_ j& =\partial (\chi _ j\mathrm e^{w_ j})\wedge \bar\alpha _ j+\chi _ j\mathrm e^{w_ j}\, \partial \bar\alpha _ j\\ & =\mathrm e^{w_ j}\bigl ((\partial \chi _ j+\chi _ j\partial w_ j)\wedge (\chi _ j\bar\partial w_ j+2\bar\partial \chi _ j)\\ & \qquad +\chi _ j\partial \chi _ j\wedge \bar\partial w_ j+\chi _ j^2\partial \bar\partial w_ j+2\chi _ j\partial \bar\partial \chi _ j\bigr )\\ & =\mathrm e^{w_ j}\bigl (\alpha _ j\wedge \bar\alpha _ j+\chi _ j^2\partial \bar\partial w_ j+2\chi _ j\partial \bar\partial \chi _ j-2\partial \chi _ j\wedge \bar\partial \chi _ j\bigr ), \end{aligned} \]
where the last line follows by expanding $\alpha _ j\wedge \bar\alpha _ j=\chi _ j^2\partial w_ j\wedge \bar\partial w_ j+2\chi _ j\partial w_ j\wedge \bar\partial \chi _ j+2\chi _ j\partial \chi _ j\wedge \bar\partial w_ j+4\partial \chi _ j\wedge \bar\partial \chi _ j$. Next, $\partial \bar\partial \log S=\partial \bar\partial S/S-\partial S\wedge \bar\partial S/S^2$, and since $\sum _ l\chi _ l^2\mathrm e^{w_ l}=S$,
\[ \sum _ j\frac{\mathrm e^{w_ j}\alpha _ j\wedge \bar\alpha _ j}S-\frac{\partial S\wedge \bar\partial S}{S^2} =\frac1{S^2}\sum _{j,l}\mathrm e^{w_ j+w_ l}\bigl (\chi _ l^2\, \alpha _ j\wedge \bar\alpha _ j-\chi _ j\chi _ l\, \alpha _ j\wedge \bar\alpha _ l\bigr ). \]
In the last sum the terms with $j=l$ vanish, and for $j<l$ the terms with indices $(j,l)$ and $(l,j)$ add up to $\mathrm e^{w_ j+w_ l}(\chi _ j\alpha _ l-\chi _ l\alpha _ j)\wedge \overline{(\chi _ j\alpha _ l-\chi _ l\alpha _ j)}$. Multiplying by $\mathrm i/2\pi $ and using $\mathrm{dd}^{\mathrm{c}}=\frac{\mathrm i}{2\pi }\partial \bar\partial $, we obtain (6.17.2). The first term on the right of (6.17.2) is semipositive, because the coefficients $\mathrm e^{w_ j+w_ l}/(2\pi S^2)$ are positive and, for a $(1,0)$-form $\gamma =\sum _ k\gamma _ k\, \mathrm dz_ k$, the coefficient matrix $(\gamma _ k\bar\gamma _{k'})$ of $\mathrm i\gamma \wedge \bar\gamma $ is positive semidefinite.
We now prove (1) in three steps.
Step 2: a curvature estimate. By lemma 6.14.1, applied on the compact manifold $X$ to the finitely many smooth forms below, there is a constant $A>0$, depending only on the fixed geometry, such that $\chi _ j\mathrm{dd}^{\mathrm{c}}\chi _ j-\frac{\mathrm i}{2\pi }\partial \chi _ j\wedge \bar\partial \chi _ j\geq -A\omega $ for every $j$. Let $W\subset X$ be open, and for the indices $j$ with $W\cap \operatorname{Supp}\chi _ j\neq \varnothing $ let $w_ j$ be smooth real functions on $W$ such that
\[ \mathrm{dd}^{\mathrm{c}}w_ j\geq -m\theta \quad \text{on }W,\qquad \mathrm e^{w_ j}\leq \mathrm e^{C_ B}\mathrm e^{w_ i}\quad \text{on }W\cap U_ i\cap \operatorname{Supp}\chi _ j \]
for all such $i,j$. We claim that $S=\sum _ j\chi _ j^2\mathrm e^{w_ j}$ is positive on $W$ and that
\[ \theta +\frac1m\mathrm{dd}^{\mathrm{c}}\log S\geq -\frac{2JA\mathrm e^{C_ B}}m\omega \qquad \text{on }W. \]
Let $x\in W$ and choose $i$ with $x\in U_ i$. Then $\chi _ i(x)=1$, so $S(x)\geq \mathrm e^{w_ i(x)}>0$, and $\mathrm e^{w_ j}/S\leq \mathrm e^{C_ B}$ at $x$ for every $j$ with $\chi _ j(x)\neq 0$. Since $S>0$ on $W$, the identity (6.17.2) of (2) holds on $W$. If $\chi _ j(x)=0$, the $j$th summand of the last term in (6.17.2) vanishes at $x$, because the nonnegative function $\chi _ j$ attains its minimum at $x$, so that $\partial \chi _ j(x)=0$. Hence the last term is at least $-2JA\mathrm e^{C_ B}\omega $ at $x$. The coefficients $\chi _ j^2\mathrm e^{w_ j}/S$ are nonnegative with sum one, so the middle term is at least $-m\theta $, and the first term is semipositive. This proves the claim.
Step 3: $G_ m$ is quasi-plurisubharmonic and satisfies the curvature bound. Since the kernels $a_{j,m}$ may vanish, we apply Step 2 to smooth approximations of $\log a_{j,m}$ and pass to the limit. Fix $x_0\in X$ and a small coordinate ball $W$ about $x_0$ such that $W\subset U'_ j$ whenever $x_0\in \operatorname{Supp}\chi _ j$, and $W\cap \operatorname{Supp}\chi _ j=\varnothing $ otherwise; then the indices $j$ with $W\cap \operatorname{Supp}\chi _ j\neq \varnothing $ are those with $x_0\in \operatorname{Supp}\chi _ j$. Choose a smooth function $g$ on $W$ with $\mathrm{dd}^{\mathrm{c}}g=\theta $, and for each such $j$ write $h_ j-g=\operatorname{Re}b_ j$ on $W$ with $b_ j$ holomorphic, by lemma 6.14.2. Since $h_ j=g+\operatorname{Re}b_ j$ on $W$, we have $a_{j,m}=\mathrm e^{-mh_ j}K_{j,m}=\mathrm e^{-mg}k_ j$ on $W$, where, by (6.15.2) and since $|\mathrm e^{-mb_ j/2}|^2=\mathrm e^{-m\operatorname{Re}b_ j}$, $k_ j=\mathrm e^{-m\operatorname{Re}b_ j}K_{j,m}=\sum _\ell |\mathrm e^{-mb_ j/2}e_\ell |^2$ for an orthonormal basis $(e_\ell )$ of the space defining $K_{j,m}$.
For $\delta >0$ the function $\log (k_ j+\delta )$ is smooth, by lemma 6.15.3, and plurisubharmonic: it is the increasing limit of the logarithms of the finite partial sums of these squared moduli together with $|\sqrt\delta |^2$, which are plurisubharmonic by proposition 5.10.3, and since the limit is continuous, theorem 5.10.2 applies. Put $w_ j^\delta =\log (k_ j+\delta )-mg$, so that $\mathrm{dd}^{\mathrm{c}}w_ j^\delta \geq -m\theta $. On $W\cap U_ i\cap \operatorname{Supp}\chi _ j$, which lies in $\overline{U'_ j}\cap \overline{U'_ i}$, lemma 6.16.2 and the identities $a_{j,m}=\mathrm e^{-mg}k_ j$, $a_{i,m}=\mathrm e^{-mg}k_ i$ give $k_ j\leq \mathrm e^{C_ B}k_ i$, and since $\mathrm e^{C_ B}\geq 1$ also $k_ j+\delta \leq \mathrm e^{C_ B}(k_ i+\delta )$. Thus the functions $w_ j^\delta $ satisfy the hypotheses of Step 2 on $W$, and the function
\[ \frac1m\log \sum _ j\chi _ j^2\mathrm e^{w_ j^\delta }+g' \]
is plurisubharmonic on $W$, where $g'$ is a smooth function on $W$ with $\mathrm{dd}^{\mathrm{c}}g'=\theta +(2JA\mathrm e^{C_ B}/m)\omega $, given by lemma 6.14.2. Indeed, by Step 2 this function is smooth with positive semidefinite complex Hessian, so proposition 5.9.2(1) applies.
As $\delta \downarrow 0$, the sums $\sum _ j\chi _ j^2\mathrm e^{w_ j^\delta }=\mathrm e^{-mg}\sum _ j\chi _ j^2(k_ j+\delta )$ decrease to $R_ m$, so these functions decrease to $G_ m+g'$, which is not identically $-\infty $, since $G_ m\geq v_{i,m}$ on $U_ i$. By theorem 5.10.1, $G_ m+g'$ is plurisubharmonic on $W$. Hence $G_ m$ is quasi-plurisubharmonic, and the curvature bound holds with $c'=2JA\mathrm e^{C_ B}$, which depends only on the fixed geometry.
Step 4: the singularities of $G_ m$ are gentle. Each summand of $R_ m$ is smooth by lemma 6.15.3. On $U_ i$ we have $a_{i,m}\leq R_ m\leq J\mathrm e^{C_ B}a_{i,m}$ by lemma 6.16.2, and $a_{i,m}$ is comparable with $\sum _ k|g_ k|^2$ for local generators $g_ k$ of $\mathcal I(m(\varphi +h_ i))=\mathcal I(m\varphi )$. Thus $G_ m$ has analytic singularities of type $(m^{-1},\mathcal I(m\varphi ))$, and $\exp (mG_ m)=R_ m$ is smooth on $X$.
Now let $\pi \colon Y\to X$ be any log resolution of $\mathcal I(m\varphi )$, with $\pi ^*\mathcal I(m\varphi )=\mathcal O(-D)$. Its restriction $\pi ^{-1}(B_ j)\to B_ j$ satisfies $\pi ^*\mathcal I(m(\varphi +h_ j))=\mathcal O(-D)$ on $\pi ^{-1}(B_ j)$, so by lemma 6.15.3, applied with the volume form $\omega ^ n/n!$, the pulled-back kernel $K_{j,m}\circ \pi $ is locally $|s_ D|^2$ times a smooth strictly positive function on $\pi ^{-1}(B_ j)$. The factors $\mathrm e^{-mh_ j}\circ \pi $ and $\chi _ j^2\circ \pi $ are smooth, and the latter vanishes outside the closed set $\pi ^{-1}(\operatorname{Supp}\chi _ j)\subset \pi ^{-1}(B_ j)$; hence $(R_ m\circ \pi )/|s_ D|^2$ is smooth on $Y$, and it is strictly positive because at every point some $\chi _ i\circ \pi $ equals one. Therefore $G_ m\circ \pi $ is locally the sum of $m^{-1}\log |s_ D|^2$ and a smooth function. These are exactly the requirements of definition 6.14.12.
$\square$
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