FBD81D436A6A
The fixed Kähler form $\omega $ serves as a reference: volumes, norms and the Laplacians of obstacles are taken with respect to $\omega $, also when an envelope is formed with respect to a different background. We call the elements of $\mathrm{PSH}(X,\theta )$ (definition 6.14.3) potentials; they are pointwise defined functions, not identically $-\infty $. Recall from definition 10.3.7 that $u$ is more singular than $v$, written $u\preceq v$, if $u\leq v+C$ for some constant $C$. We write $u\sim v$, and say that $u$ and $v$ have the same singularity type, if $u\preceq v$ and $v\preceq u$.
Two facts are used constantly. First, pluripolar sets have Lebesgue measure zero (see the remarks after definition 5.47.2). Second, if two quasi-plurisubharmonic functions satisfy $u\leq v$ almost everywhere, then $u\leq v$ everywhere, by lemma 6.14.4(1). Consequently, an inequality between quasi-plurisubharmonic functions that holds quasi-everywhere, that is, outside a pluripolar set (definition 5.47.2), holds everywhere. In particular, if $u\sim v$, then $u$ and $v$ have the same pole set and $u-v$ is bounded outside it.
Quasi-continuity on $X$ is the notion of definition 7.5.1, read in local charts as in section 13.7: a Borel function $f\colon X\to [-\infty ,+\infty ]$ is quasi-continuous if its restriction to every coordinate chart, identified with a bounded open set $D\subset \mathbb C^ n$, is quasi-continuous for the Monge–Ampère capacity $\operatorname {Cap}_ D$ of definition 7.4.2. The following lemma shows that it suffices to check this on the charts of one atlas; in proposition 16.27.18 we show that quasi-continuous functions are also continuous outside open sets of small global capacity.
Lemma 16.11.1.33A40EB62C98 Let $D$ and $D'$ be coordinate charts of $X$, identified with bounded open subsets of $\mathbb C^ n$.
For every compact set $L\subset D\cap D'$ there is a constant $c$ such that $\operatorname {Cap}_ D(E)\leq c\operatorname {Cap}_{D'}(E)$ for every Borel set $E\subset L$.
If $E\subset X$ is pluripolar, then $\operatorname {Cap}_ D^*(E\cap D)=0$.
If a Borel function $f\colon X\to [-\infty ,+\infty ]$ is quasi-continuous on each chart of an atlas of $X$, then it is quasi-continuous on every coordinate chart.
Proof.
Assertions (1) and (3) are contained in lemma 13.7.1: (1) is its inequality for Borel sets, applied with the roles of $D$ and $D'$ exchanged, and (3) is its final assertion.
For (2) we first observe that if $W\subset D$ is open, then every competitor $v$ for $\operatorname {Cap}_ D$ restricts to a plurisubharmonic function on $W$ with values in $[0,1]$, and the restriction of the Bedford–Taylor measure $(\mathrm{dd}^{\mathrm{c}}v)^ n$ to $W$ is the Bedford–Taylor measure of this restriction. Hence $\operatorname {Cap}_ D(E)\leq \operatorname {Cap}_ W(E)$ for every Borel set $E\subset W$, and, taking infima over the open sets $G$ with $A\subset G\subset W$, also $\operatorname {Cap}_ D^*(A)\leq \operatorname {Cap}_ W^*(A)$ for every set $A\subset W$.
Now cover $D$ by countably many open balls $B_ k$, in the coordinates of $D$, with $\overline{B_ k}\subset D$. Since the condition in definition 5.47.2 is local, $E\cap B_ k$ is pluripolar in $B_ k$, so $\operatorname {Cap}_{B_ k}^*(E\cap B_ k)=0$ by theorem 5.47.8. By the observation above, $\operatorname {Cap}_ D^*(E\cap B_ k)=0$, and the countable subadditivity of $\operatorname {Cap}_ D^*$ (proposition 7.4.3) gives $\operatorname {Cap}_ D^*(E\cap D)=0$.
$\square$
Quasi-plurisubharmonic functions are quasi-continuous, and quasi-continuity is preserved by the following operations.
Lemma 16.11.2.1BA71B27F698 Let $\theta '$ be a smooth closed real $(1,1)$-form on $X$.
Every $u\in \mathrm{PSH}(X,\theta ')$ is quasi-continuous. In particular, every potential $u\in \mathrm{PSH}(X,\theta )$ is quasi-continuous.
Finite maxima and minima of quasi-continuous functions on $X$ are quasi-continuous.
If $f$ is quasi-continuous on $X$ and $g\colon X\to [-\infty ,+\infty ]$ is a Borel function that agrees with $f$ outside a pluripolar set, then $g$ is quasi-continuous.
Proof.
(1) By lemma 5.4.2 every point of $X$ has a neighborhood on which $\theta '=\mathrm{dd}^{\mathrm{c}}h$ for a smooth function $h$, so $X$ is covered by finitely many coordinate balls $D_ i$ on which $\theta '=\mathrm{dd}^{\mathrm{c}}h_ i$ with $h_ i$ smooth near $\overline{D_ i}$. On $D_ i$ the function $u+h_ i$ is plurisubharmonic by lemma 6.14.4(2), hence quasi-continuous by theorem 7.5.2, and so is $u=(u+h_ i)-h_ i$, because $h_ i$ is continuous and real. By lemma 16.11.1(3), $u$ is quasi-continuous on every chart.
(2) Let $f_1,\ldots ,f_ k$ be quasi-continuous, let $K$ be a compact subset of a chart $D$, and let $\varepsilon >0$. Choose open sets $G_ i\subset D$ with $\operatorname {Cap}_ D(G_ i)<\varepsilon /k$ such that $f_ i$ is continuous on $K\setminus G_ i$. By subadditivity, $G=G_1\cup \cdots \cup G_ k$ has capacity less than $\varepsilon $, and all the $f_ i$, hence also their maximum and minimum, are continuous on $K\setminus G$.
(3) Let $D$ be a chart, $K\subset D$ compact and $\varepsilon >0$. The set $\{ f\ne g\} $ is pluripolar, so by lemma 16.11.1(2) its intersection with $D$ is contained in an open set $G'\subset D$ with $\operatorname {Cap}_ D(G')<\varepsilon /2$. If $G\subset D$ is an open set with $\operatorname {Cap}_ D(G)<\varepsilon /2$ such that $f$ is continuous on $K\setminus G$, then $\operatorname {Cap}_ D(G\cup G')<\varepsilon $, and $g=f$ is continuous on $K\setminus (G\cup G')$.
$\square$
Definition 16.11.3.A4F165851008 Let $f\colon X\to [-\infty ,+\infty ]$ be a Borel function, called an obstacle, and put
\[ \mathcal A_\theta (f)=\{ v\in \mathrm{PSH}(X,\theta ):v\leq f \text{ quasi-everywhere}\} . \]
The members of $\mathcal A_\theta (f)$ are called the competitors for $f$. If $\mathcal A_\theta (f)$ is nonempty and uniformly bounded above, the obstacle envelope of $f$ is
\[ P_\theta (f)=\bigl (\sup \mathcal A_\theta (f)\bigr )^*, \]
where ${}^*$ denotes the upper semicontinuous regularization. If $\mathcal A_\theta (f)$ is empty, we put $P_\theta (f)=-\infty $. If $\mathcal A_\theta (f)$ is nonempty but not uniformly bounded above, $P_\theta (f)$ is not defined, and whenever we use $P_\theta (f)$ for an obstacle that is not bounded above, we verify the upper bound first. If $f\leq b$ quasi-everywhere for a constant $b$, the upper bound is automatic: every competitor satisfies $v\leq b$ quasi-everywhere, hence almost everywhere, and therefore everywhere by lemma 6.14.4(1).
As for the capacity $\operatorname {Cap}_ D$ (definition
7.4.2) and the relative extremal functions of section
5.47, a competitor is a member of the family whose supremum defines the object under consideration; we always say which obstacle, envelope or capacity is meant.
Proposition 16.11.4.641F3FEC623D Let $f$ be a Borel obstacle.
If $\mathcal A_\theta (f)$ is nonempty and uniformly bounded above, then $P_\theta (f)\in \mathcal A_\theta (f)$; thus $P_\theta (f)$ is the largest competitor for $f$.
If $f$ is upper semicontinuous, then every competitor $v$ for $f$ satisfies $v\leq f$ everywhere.
The envelope does not change when $f$ is modified on a pluripolar set, and $P_\theta (f+c)=P_\theta (f)+c$ for $c\in \mathbb R$. If $g$ is a Borel obstacle with $f\leq g$ quasi-everywhere and $\mathcal A_\theta (g)$ is uniformly bounded above, then $P_\theta (f)\leq P_\theta (g)$.
Suppose that $\mathcal A_\theta (f)$ is nonempty and uniformly bounded above, and let $g$ be a Borel obstacle with $f-c\leq g\leq f+c$ quasi-everywhere for a constant $c\geq 0$. Then $\mathcal A_\theta (g)$ is nonempty and uniformly bounded above, and
\[ P_\theta (f)-c\leq P_\theta (g)\leq P_\theta (f)+c. \]
In particular the two envelopes have the same pole set and differ by at most $c$ outside it.
Let Borel obstacles $f_ j$ decrease pointwise to $f$, and suppose that $\mathcal A_\theta (f_1)$ is uniformly bounded above. Then $P_\theta (f_ j)$ decreases pointwise to $P_\theta (f)$. Here the families may be empty; in particular, $P_\theta (f_ j)$ decreases to the constant $-\infty $ if and only if $\mathcal A_\theta (f)=\varnothing $.
Proof.
(1) Cover $X$ by finitely many coordinate balls on which $\theta $ has smooth local potentials $h$ (lemma 5.4.2). Applying theorem 5.10.2 on each ball to the plurisubharmonic functions $v+h$, $v\in \mathcal A_\theta (f)$, and taking the union of the resulting countable subfamilies, we find competitors $v_1,v_2,\ldots $ with $(\sup _ kv_ k)^*=P_\theta (f)$. The finite maxima $w_ k=\max \{ v_1,\ldots ,v_ k\} $ are again competitors, and they increase with $k$. Each $w_ k$ satisfies $w_ k\leq f$ outside a pluripolar set $N_ k$, and $N=\bigcup _ kN_ k$ is pluripolar by theorem 5.47.8. By corollary 5.47.11, $\sup _ kw_ k=P_\theta (f)$ outside a pluripolar set $N'$. Hence $P_\theta (f)\leq f$ outside $N\cup N'$. Since the family is nonempty and uniformly bounded above, $P_\theta (f)$ is $\theta $-plurisubharmonic by theorem 5.10.2. Thus $P_\theta (f)$ is a competitor, and by construction it dominates every competitor.
(2) Let $v$ be a competitor, let $x\in X$, and choose a coordinate ball $B(x,r)$ and a smooth function $h$ with $\mathrm{dd}^{\mathrm{c}}h=\theta $ near its closure. Since $v+h$ is plurisubharmonic and $v\leq f$ outside a Lebesgue null set, the sub-mean value inequality gives
\[ v(x)+h(x)\leq \frac1{|B(x,r)|}\int _{B(x,r)}(v+h)\, \mathrm dV_{2n} \leq \sup _{B(x,r)}(f+h). \]
As $r\to 0$, the right side tends to at most $f(x)+h(x)$, because $f+h$ is upper semicontinuous. Hence $v(x)\leq f(x)$.
(3) A modification of $f$ on a pluripolar set does not change $\mathcal A_\theta (f)$, since the union of two pluripolar sets is pluripolar. Moreover $\mathcal A_\theta (f+c)=\mathcal A_\theta (f)+c$, and $\mathcal A_\theta (f)\subset \mathcal A_\theta (g)$ if $f\leq g$ quasi-everywhere. These relations between the families of competitors give the three assertions.
(4) By (3), $\mathcal A_\theta (f)-c\subset \mathcal A_\theta (g)\subset \mathcal A_\theta (f)+c$. Hence $\mathcal A_\theta (g)$ is nonempty and uniformly bounded above, and the two inequalities follow from (3).
(5) By (3) the envelopes $P_\theta (f_ j)$ decrease; if some family $\mathcal A_\theta (f_ j)$ is empty, then so are all later ones and $\mathcal A_\theta (f)$. Let $v$ be the pointwise limit of $P_\theta (f_ j)$. Suppose first that $v(x_0)>-\infty $ for some $x_0$. Then $\sup _ XP_\theta (f_ j)\geq v(x_0)$ for every $j$, so $v\in \mathrm{PSH}(X,\theta )$ by corollary 10.3.6. By (1), $v\leq P_\theta (f_ j)\leq f_ j$ outside a pluripolar set $N_ j$, so $v\leq \inf _ jf_ j=f$ outside the pluripolar set $\bigcup _ jN_ j$. Thus $v$ is a competitor for $f$ and $v\leq P_\theta (f)$; the reverse inequality follows from $P_\theta (f)\leq P_\theta (f_ j)$. Suppose next that $v\equiv -\infty $. A competitor $w$ for $f$ would be a competitor for every $f_ j$, so $w\leq P_\theta (f_ j)$ for all $j$ and $w\leq v$, which is impossible. Hence $\mathcal A_\theta (f)=\varnothing $ and $P_\theta (f)=-\infty =v$.
$\square$
Definition 16.11.5.F80B4C1B3032 For $u,v\in \mathrm{PSH}(X,\theta )$, the rooftop envelope of $u$ and $v$ is
\[ P_\theta (u,v)=P_\theta (\min \{ u,v\} ). \]
We also put $P_\theta (u,-\infty )=P_\theta (-\infty ,u)=-\infty $ for $u\in \mathrm{PSH}(X,\theta )\cup \{ -\infty \} $.
The obstacle $\min \{ u,v\} $ is upper semicontinuous and bounded above. By proposition
16.11.4, a potential is therefore a competitor for it exactly when it lies below both $u$ and $v$ everywhere. Thus $P_\theta (u,v)$ is the largest common minorant of $u$ and $v$ in $\mathrm{PSH}(X,\theta )$ if they have one, and $P_\theta (u,v)=-\infty $ if they have none.
Proposition 16.11.6.046401771DAB The rooftop envelope is commutative, associative, increasing in both arguments and idempotent, that is, $P_\theta (u,u)=u$. For a constant $c$, $P_\theta (u+c,v+c)=P_\theta (u,v)+c$. If $u_ j,v_ j\in \mathrm{PSH}(X,\theta )$ decrease pointwise to $u$ and $v$, where the limits may be identically $-\infty $, then $P_\theta (u_ j,v_ j)$ decreases pointwise to $P_\theta (u,v)$. Finally, for $u\in \mathrm{PSH}(X,\theta )$ and every constant $C\in \mathbb R$, the rooftop envelope $P_\theta (u+C,V_\theta )$ is a potential with $P_\theta (u+C,V_\theta )\sim u$.
Proof.
Commutativity, monotonicity and idempotence follow directly from the description of $P_\theta (u,v)$ as the largest common minorant. For associativity, let also $w\in \mathrm{PSH}(X,\theta )\cup \{ -\infty \} $. A potential lies below $P_\theta (u,v)$ and $w$ if and only if it lies below $u$, $v$ and $w$: when $P_\theta (u,v)\ne -\infty $ this is the maximality of $P_\theta (u,v)$, and otherwise neither condition can be satisfied. Hence $P_\theta (P_\theta (u,v),w)$ and $P_\theta (u,P_\theta (v,w))$ are both the largest common minorant of $u$, $v$ and $w$, or both equal $-\infty $ if there is none. The behavior under constant shifts and decreasing limits follows from proposition 16.11.4, applied to the obstacles $\min \{ u_ j,v_ j\} $, which are bounded above by $\sup _ Xu_1$ and decrease to $\min \{ u,v\} $. If $u$ or $v$ is identically $-\infty $, this limit obstacle has no competitor, in accordance with our convention.
For the last assertion put $B=\max \{ \sup _ Xu,-C\} $. Then $u-B\leq 0$, so $u-B\leq V_\theta $, and also $u-B\leq u+C$. Hence $u-B$ is a common minorant of $u+C$ and $V_\theta $, and
\[ u-B\leq P_\theta (u+C,V_\theta )\leq u+C. \]
$\square$
Example 16.11.7.908479CB91B3 On $\mathbb P^1$ let $\theta =\omega _{\mathrm{FS}}=\mathrm{dd}^{\mathrm{c}}\log (1+|z|^2)$ be the Fubini–Study form of example 10.6.7, in the affine coordinate $z$, so that $\int _{\mathbb P^1}\theta =1$. Put
\[ u_0=\log \frac{|z|^2}{1+|z|^2},\qquad u_\infty =-\log (1+|z|^2). \]
In the coordinate $\zeta =1/z$ near $\infty $ we have $\log (1+|z|^2)=\log (1+|\zeta |^2)-\log |\zeta |^2$, so $\theta =\mathrm{dd}^{\mathrm{c}}\log (1+|\zeta |^2)$ there, while $u_0=-\log (1+|\zeta |^2)$ and $u_\infty =\log (|\zeta |^2/(1+|\zeta |^2))$. Thus the substitution $z\leftrightarrow \zeta $ exchanges the two functions. On $\mathbb C$ we have $\theta +\mathrm{dd}^{\mathrm{c}}u_0=\mathrm{dd}^{\mathrm{c}}\log |z|^2=[0]$ by the Poincaré–Lelong formula (theorem 5.5.6), and $u_0$ is smooth near $\infty $ with $\theta +\mathrm{dd}^{\mathrm{c}}u_0=0$ there. Hence $u_0,u_\infty \in \mathrm{PSH}(\mathbb P^1,\theta )$, with $\theta +\mathrm{dd}^{\mathrm{c}}u_0=[0]$ and $\theta +\mathrm{dd}^{\mathrm{c}}u_\infty =[\infty ]$, the currents of integration at the two points.
Suppose that $w\in \mathrm{PSH}(\mathbb P^1,\theta )$ is a common minorant of $u_0$ and $u_\infty $. Near $0$ the function $u_0$ is $\log |z|^2$ plus a smooth function, so $\nu (u_0,0)=1$ by proposition 6.7.9, and $w\leq u_0$ gives $\nu (w,0)\geq 1$ by the description of Lelong numbers through logarithmic growth in proposition 6.7.1; likewise $\nu (w,\infty )\geq 1$. In dimension one, the Lelong number of a subharmonic function $s$ at a point is the mass that the measure $\mathrm{dd}^{\mathrm{c}}s$ gives to that point (theorem 6.7.6). Hence the positive measure $\theta +\mathrm{dd}^{\mathrm{c}}w$ has atoms of mass at least one at $0$ and at $\infty $, whereas its total mass is $\int _{\mathbb P^1}\theta =1$, because $\langle \mathrm{dd}^{\mathrm{c}}w,1\rangle =\langle w,\mathrm{dd}^{\mathrm{c}}1\rangle =0$. This contradiction shows that $P_\theta (u_0,u_\infty )=-\infty $, although $u_0$ and $u_\infty $ are both $\theta $-plurisubharmonic.
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