Proposition 15.8.4.29A74E6E8A18 If $f$ is bounded and lower semicontinuous, then $p=P_\theta (f)$ is locally bounded on $X\setminus Z$, and
15.8.3 Quasi-continuous obstacles5E57580F8E39
We now extend the contact property to discontinuous obstacles. Continuous approximations of an obstacle need not preserve every competitor of its envelope pointwise. For lower semicontinuous obstacles, the approximation of lemma 5.40.5 repairs this, and quasi-continuity then allows us to pass to limits of weighted measures. An unbounded obstacle is truncated at finite levels; in an arbitrary smooth background this produces signed products, whose limits are controlled by lemma 5.29.17 before we restrict to the region where the product is positive. The strict analytic barrier $\rho $ and its pole set $Z$ are those fixed above.
Proof. Using the infimum construction in the proof of proposition 16.28.3, take continuous $f_ j\uparrow f$ with common bounds $m\leq f_ j\leq M$, and shift $\rho $ below $m$. The envelopes $p_ j=P_\theta (f_ j)$ increase and satisfy
Their regularized limit $q=(\lim _ jp_ j)^*$ is therefore $\theta $-plurisubharmonic. Outside a pluripolar set it equals the pointwise limit, which is at most $f$; hence $q\leq p=P_\theta (f)$.
We prove the reverse inequality without using a domination theorem. Let $u$ be any competitor for $P_\theta (f)$, and let $u_ t\leq f$ be the potentials given by lemma 5.40.5, which satisfy this inequality everywhere. For fixed $t,\eta >0$, the sets
are open, increase with $j$, and cover $X$. By compactness, $u_ t\leq f_ j+\eta $ everywhere for all large $j$. Thus $u_ t-\eta $ is a competitor for $p_ j$, and $q\geq u_ t-\eta $. Letting first $\eta \downarrow 0$ and then $t\downarrow 0$, we obtain $q\geq u$ almost everywhere, hence everywhere by lemma 5.24.3. Taking the supremum over all competitors $u$ gives $q\geq p$, so $q=p$.
For fixed $k$, the set $U_ k=\{ p<f_ k\} $ is open. If $j\geq k$, then $p_ j\leq p<f_ k\leq f_ j$ on $U_ k$, so theorem 15.8.1 gives $\mathrm{MA}_\theta (p_ j)=0$ there. On every relatively compact open subset of $X\setminus Z$ the functions $p_ j$ have common bounds. After a common smooth correction and a finite expansion, the local Bedford–Taylor continuity along increasing sequences shows that their measures converge to $\mathrm{MA}_\theta (p)$ there. Since the measure of an open set is at most the lower limit of the measures of the approximating sequence, $\mathrm{MA}_\theta (p)$ vanishes on $U_ k\setminus Z$. The union of these sets is $\{ p<f\} \setminus Z$, and the extended measure does not charge the pluripolar set $Z$. $\square$
Proposition 15.8.5.BDE06B833BC8 The conclusion of proposition 15.8.4 holds for every bounded quasi-continuous obstacle $f$.
Proof. By lemma 5.29.15, there are bounded lower semicontinuous $f_ j$ with common bounds and $f_ j\downarrow f$ quasi-everywhere. The envelopes $p_ j=P_\theta (f_ j)$ decrease to $p=P_\theta (f)$. Indeed, the common lower barrier shows that the limit is not identically $-\infty $; the limit lies below $f$ quasi-everywhere and is thus a competitor for $P_\theta (f)$, while monotonicity gives the other inequality. All these functions have common local bounds off $Z$.
For fixed $k$, put $H_ k=\min \{ 1,(f-p_ k)_+\} $ on $X\setminus Z$, a bounded quasi-continuous function there. If $j\geq k$, then on $\{ H_ k>0\} $ we have $p_ j\leq p_ k<f\leq f_ j$ outside a pluripolar set, so proposition 15.8.4 gives $H_ k\mathrm{MA}_\theta (p_ j)=0$ off $Z$.
Let $g$ be continuous with compact support in $X\setminus Z$. The continuity of bounded products against quasi-continuous weights from section 5.27 applies to the fixed quasi-continuous coefficient $gH_ k$. Consequently $H_ k\mathrm{MA}_\theta (p)=0$ off $Z$. As $k\to \infty $, the sets $\{ H_ k>0\} $ exhaust $\{ p<f\} \setminus Z$, and $Z$ is not charged because it is pluripolar. $\square$
For an unbounded obstacle, we truncate and use the convergence of signed products in lemma 5.29.17.
Theorem 15.8.6.6F087EC35E2E Let $\theta $ be smooth and big. Let $f$ be a quasi-continuous obstacle, finite almost everywhere, such that $p=P_\theta (f)\not\equiv -\infty $. Then $p\leq f$ quasi-everywhere and
As before, the measure $\mathrm{MA}_\theta (p)$ may have infinite total mass.
Proof. As in the proof of theorem 16.28.5, the local envelope theorem and a countable Choquet family give $p\leq f$ quasi-everywhere. Set $f_ j=\max (f,-j)$ and $p_ j=P_\theta (f_ j)$. Then $p$ is a competitor for every $f_ j$. Since $f_ j\leq f_1$ and $f_1$ is finite almost everywhere, the finite-sublevel argument in section 5.40 gives a common upper bound for all competitors. Thus the envelopes $p_ j$ are $\theta $-plurisubharmonic and uniformly bounded above. Choose $M$ strictly larger than this bound.
The obstacle $g_ j=\min (f_ j,M)$ is bounded and quasi-continuous. Since $p_ j<M$ and $p_ j\leq f_ j$ quasi-everywhere, $p_ j$ is a competitor for $P_\theta (g_ j)$; the reverse inequality follows from $g_ j\leq f_ j$. Thus $p_ j=P_\theta (g_ j)$, and proposition 15.8.5 gives contact support for $p_ j$ with respect to $g_ j$. Because $p_ j<M$, no contact occurs at the artificial upper cutoff, so
5ACCF67CCE26
15.8.7
Each $p_ j$ is locally bounded off $Z$, with a lower barrier of the form $\rho -C_ j$. The sequence decreases to $p$: its limit is not identically $-\infty $ because it dominates $p$, and it lies below $f$ quasi-everywhere, so it is itself a competitor for $P_\theta (f)$.
Fix a Hermitian form $\Omega \geq \theta $. For integers $C,k\geq 1$, consider the bounded $\Omega $-plurisubharmonic functions
and set
extended by zero on $Z$. This function is bounded and quasi-continuous. Indeed, off $Z$ the function $p_ k$ is a finite quasi-plurisubharmonic function, truncation by bounded continuous functions preserves quasi-continuity, and the pluripolar set $Z$ can be removed by an open set of arbitrarily small capacity. At a pole of $p$ the second factor vanishes.
For $j\geq k$, on $\{ H_{k,C}>0\} $ we have, outside pluripolar sets,
By plurifine locality, the signed measure $\nu _{j,C}=(\theta +\mathrm{dd}^{\mathrm{c}}v_{j,C})^ n$ therefore agrees there with $\mathrm{MA}_\theta (p_ j)$, and (15.8.7) gives
For fixed $C$, the potentials $v_{j,C}$ have common global bounds and decrease to $v_ C$, so lemma 5.29.17 yields
On the set where $H_{k,C}$ is positive we have $p>-C$, so the restricted product in theorem 13.14.3 identifies $H_{k,C}(\theta +\mathrm{dd}^{\mathrm{c}}v_ C)^ n$ with the positive measure $H_{k,C}\mathrm{MA}_\theta (p)$; on the complement the coefficient is zero. Hence $\mathrm{MA}_\theta (p)$ vanishes on $\{ H_{k,C}>0\} $.
Finally, if $p(x)$ is finite and $p(x)<f(x)$, then $p_ k(x)<f(x)$ for large $k$ and $p(x)>-C$ for large $C$. The countable union of the sets $\{ H_{k,C}>0\} $ therefore covers $\{ p<f\} $ outside $Z\cup \{ p=-\infty \} $. Both excluded sets are pluripolar, and the theorem follows. $\square$
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