Proposition 5.46.3.09F56C9DE42C Let $u,v$ be quasi-plurisubharmonic functions on a complex manifold such that every point has a neighborhood on which $u-C\leq v\leq u+C$ for some constant $C$. Then $u$ and $v$ have the same pole set $S=\{ u=-\infty \} =\{ v=-\infty \} $, and
\[ \mathbf1_ S\mathrm{dd}^{\mathrm{c}}u=\mathbf1_ S\mathrm{dd}^{\mathrm{c}}v. \]
Consequently, for any smooth real $(1,1)$-forms $\theta ,\beta $,
\[ \mathbf1_ S(\theta +\mathrm{dd}^{\mathrm{c}}u)=\mathbf1_ S(\beta +\mathrm{dd}^{\mathrm{c}}v). \]
Proof.
The two local inequalities show that the pole sets agree. Off $S$ put $w=u-v$, and give $w$ arbitrary bounded values on $S$. Since $S$ has Lebesgue measure zero, this defines the locally bounded distribution $u-v$. The coefficient measures of $\mathrm{dd}^{\mathrm{c}}w$ are locally finite, since after a smooth correction the complex Hessians of $u$ and $v$ are positive currents of order zero. Taking the Euclidean trace shows that $\Delta w$ is a signed Radon measure, so lemma 5.46.1 gives $w\in W^{1,2}_{\mathrm{loc}}$.
Consequently, the real and imaginary parts of the coefficient measures of $\mathrm{dd}^{\mathrm{c}}w$ are continuous linear functionals on $W^{1,2}_0$ of a smaller ball, since a second distributional derivative of $w$ is a first derivative of its $L^2$ gradient. Let $\nu $ be any one of these real signed measures, with Jordan decomposition $\nu =\nu ^+-\nu ^-$. Choose a compact set $K$ contained in the intersection of $S$ with a positive set of a Hahn decomposition, so that $\nu ^-(K)=0$. For $\epsilon >0$, take an open neighborhood $O$ of $K$ in the ball with $\nu ^-(O)<\epsilon $. The test functions $\varphi _ j$ of lemma 5.46.2, applied to $u$, satisfy
\[ \nu ^+(K)\leq \int \varphi _ j\, \mathrm d\nu ^+ =\langle \nu ,\varphi _ j\rangle +\int \varphi _ j\, \mathrm d\nu ^- \leq |\langle \nu ,\varphi _ j\rangle |+\epsilon . \]
By continuity on the Sobolev space, the first term tends to zero. Letting $\epsilon \downarrow 0$ and using inner regularity gives $\nu ^+(S)=0$ locally, and the same argument applied to $-\nu $ gives $\nu ^-(S)=0$. Thus all coefficient measures of $\mathrm{dd}^{\mathrm{c}}w$ vanish on $S$, which proves the first identity. Since smooth forms also give $S$ zero mass, the second identity follows.
$\square$
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