52BF527413C6
Bedford–Taylor products of locally uniformly bounded potentials are continuous under convergence in capacity (theorem 7.5.8). For unbounded potentials this fails, because mass can escape into the poles in the limit (example 13.7.6). What survives is a lower semicontinuity statement, which becomes continuity when the total masses do not drop in the limit. Throughout, capacities are the local Monge–Ampère capacities $\operatorname {Cap}_ D$ of definition 7.4.2, used in coordinate charts as in definition 7.5.5, and not the global capacity $c_\omega $ of section 10.9. Accordingly, a Borel function on $X$ is quasi-continuous (definition 7.5.1), and a net of Borel functions on $X$ converges locally in capacity (definition 7.5.5), if this holds in the charts of a finite atlas whose charts have bounded images; by the following lemma, this does not depend on the atlas. We then extend convergence in capacity to functions with poles.
Lemma 13.7.1.AB4F8DB9BF3E Let $(W,z)$ and $(W',z')$ be holomorphic charts of a complex manifold whose images $D=z(W)$ and $D'=z'(W')$ are bounded, and let $K\subset W\cap W'$ be compact. Then there is a constant $C$ such that
\[ \operatorname {Cap}_{D'}^*(z'(E))\leq C\operatorname {Cap}_ D^*(z(E))\qquad \text{for every set }E\subset K, \]
and $\operatorname {Cap}_{D'}(z'(E))\leq C\operatorname {Cap}_ D(z(E))$ for every Borel set $E\subset K$. Consequently, for a net of Borel functions on a complex manifold, convergence locally in capacity in the charts of an atlas whose charts have bounded images implies the same in every chart with bounded image; similarly for quasi-continuity of a Borel function.
Proof.
For every $x\in K$ choose $r_ x>0$ such that the closed ball $\overline{B(z(x),2r_ x)}$ lies in $z(W\cap W')$. Finitely many of the sets $z^{-1}(B(z(x_ i),r_ i))$, $r_ i=r_{x_ i}$, cover $K$; put $B_ i=B(z(x_ i),2r_ i)$ and $K_ i=K\cap z^{-1}(\overline{B(z(x_ i),r_ i)})$. The map $F_ i=z'\circ z^{-1}$ is a biholomorphism from $B_ i$ onto the bounded open set $B_ i'=F_ i(B_ i)\subset D'$. Let $E\subset K$ and $E_ i=E\cap K_ i$. Every competitor for $\operatorname {Cap}_{D'}$ restricts to a competitor for $\operatorname {Cap}_{B_ i'}$, so $\operatorname {Cap}_{D'}(G)\leq \operatorname {Cap}_{B_ i'}(G)$ for Borel sets $G\subset B_ i'$, and taking infima over open sets, $\operatorname {Cap}^*_{D'}\leq \operatorname {Cap}^*_{B_ i'}$ on subsets of $B_ i'$. By proposition 7.4.3(5) and (4), applied to the ball $B_ i\Subset D$ and the compact set $\overline{B(z(x_ i),r_ i)}\subset B_ i$, there is a constant $C_ i$ with
\[ \begin{aligned} \operatorname {Cap}^*_{D'}(z'(E_ i))& \leq \operatorname {Cap}^*_{B_ i'}(z'(E_ i))=\operatorname {Cap}^*_{B_ i}(z(E_ i))\\ & \leq C_ i\operatorname {Cap}^*_ D(z(E_ i))\leq C_ i\operatorname {Cap}^*_ D(z(E)). \end{aligned} \]
By subadditivity of $\operatorname {Cap}^*_{D'}$ (proposition 7.4.3), the assertion holds with $C=\sum _ iC_ i$. If $E$ is a Borel set, then so are $E_ i$, $z(E_ i)$ and $z'(E_ i)$, because $z$ and $z'$ are homeomorphisms onto their images. The restriction argument above and proposition 7.4.3(4),(5) also apply to the capacities of Borel sets, so the same chain of inequalities holds with $\operatorname {Cap}$ in place of $\operatorname {Cap}^*$, and the subadditivity of $\operatorname {Cap}_{D'}$ gives the second assertion with the same constant.
For the consequences, let $(W',z')$ be a chart with bounded image and $K'\subset W'$ compact. Cover $K'$ by finitely many compact sets $K_ i'\subset W'\cap W_ i$, where the $(W_ i,z_ i)$ are charts of the given atlas. Suppose that $(f_ a)$ converges to $f$ locally in capacity in the charts $W_ i$. By subadditivity, the outer capacity in $D'=z'(W')$ of the image of $K'\cap \{ f_ a>f+\delta \} $ is at most the sum over $i$ of the outer capacities of the images of $K_ i'\cap \{ f_ a>f+\delta \} $. By the first part, each of these is at most a constant times the corresponding outer capacity in $z_ i(W_ i)$, which tends to zero; similarly for $\{ f_ a<f-\delta \} $.
If $f$ is quasi-continuous in the charts $W_ i$ and $\varepsilon >0$, choose open sets $G_ i\subset z_ i(W_ i)$ of small capacity such that $f$ is continuous on $K_ i'\setminus z_ i^{-1}(G_ i)$. By the first part, $z'(K_ i'\cap z_ i^{-1}(G_ i))$ has outer capacity at most $C_ i\operatorname {Cap}_{z_ i(W_ i)}(G_ i)$ in $D'$, so it is contained in an open set $G_ i'\subset D'$ with $\operatorname {Cap}_{D'}(G_ i')<\varepsilon /N$, where $N$ is the number of sets $K_ i'$, provided the $G_ i$ are chosen small enough. Then $G'=\bigcup _ iG_ i'$ satisfies $\operatorname {Cap}_{D'}(G')<\varepsilon $, and the set $F=K'\setminus z'^{-1}(G')$ is the union of the finitely many relatively closed sets $F\cap K_ i'$, on each of which $f$ is continuous; hence $f$ is continuous on $F$.
$\square$
Definition 13.7.2.019A8D37A03F For $s,t\in [-\infty ,\infty )$ put $d_*(s,t)=|\arctan s-\arctan t|$, where $\arctan (-\infty )=-\pi /2$. A net $(u_ a)$ of plurisubharmonic functions on a bounded open set $D\subset \mathbb C^ n$ converges in extended capacity to a plurisubharmonic function $u$ if, for every compact set $K\subset D$ and every $\delta >0$, the outer capacity of $K\cap \{ d_*(u_ a,u)>\delta \} $ tends to zero, the capacity being taken as in definition 7.5.5. A net of $\theta $-plurisubharmonic functions on a compact manifold converges in extended capacity if the local plurisubharmonic functions obtained by adding smooth local potentials of $\theta $ do so on the charts of a finite coordinate cover by charts with bounded images. This does not depend on the choice of the local potentials or of the cover, by lemma 13.7.3 below.
Lemma 13.7.3.274B700496A8 Let $(u_ k)$ be a sequence of plurisubharmonic functions on a bounded open set $D\subset \mathbb C^ n$ that is locally uniformly bounded above, and let $u$ be plurisubharmonic on $D$. Then $u_ k\to u$ in extended capacity if and only if $\max \{ u_ k,-C\} \to \max \{ u,-C\} $ locally in capacity for every $C>0$. A decreasing sequence of plurisubharmonic functions with plurisubharmonic limit converges to it in extended capacity. Extended capacity convergence of $\theta $-plurisubharmonic functions on a compact manifold does not depend on the choices made in definition 13.7.2. If a sequence $(u_ k)$ in $\mathrm{PSH}(X,\theta )$ converges in extended capacity to an element of $\mathrm{PSH}(X,\theta )$, then the suprema $\sup _ Xu_ k$ are bounded above.
Proof.
Fix a compact set $K$ and let $M$ be an upper bound for all $u_ k$ and $u$ on $K$. On $[-\infty ,M]$, the function $\max \{ s,-C\} $ is a Lipschitz function of $\arctan s$: it is constant for $\arctan s\leq \arctan (-C)$, and the derivative of the tangent is bounded on the compact interval $[\arctan (-C),\arctan M]$. Hence extended capacity convergence implies capacity convergence of the truncations. Conversely, $|\arctan s-\arctan \max \{ s,-C\} |\leq \pi /2-\arctan C$ for all $s$, so that
\[ d_*(u_ k,u)\leq |\max \{ u_ k,-C\} -\max \{ u,-C\} |+2(\pi /2-\arctan C), \]
where we also used $|\arctan s-\arctan t|\leq |s-t|$ for finite $s,t$. Choosing $C$ with $2(\pi /2-\arctan C)<\delta /2$, the set $\{ d_*(u_ k,u)>\delta \} $ is contained in $\{ |\max \{ u_ k,-C\} -\max \{ u,-C\} |>\delta /2\} $, which proves the equivalence.
Adding the same bounded real function $h$ to $s$ and $t$ changes $d_*$ by at most a bounded factor: since $1+\sigma ^2\leq 2(1+h^2)(1+(\sigma +h)^2)$, the formula $\arctan t-\arctan s=\int _ s^ t\mathrm d\sigma /(1+\sigma ^2)$ gives $d_*(s+h,t+h)\leq 2(1+h^2)d_*(s,t)$. Now let $(W_ i,h_ i)$ and $(W'_ l,h'_ l)$ be two choices of a finite cover of $X$ by charts with bounded images and of smooth local potentials $h_ i$ of $\theta $ on $W_ i$ and $h'_ l$ on $W'_ l$, and suppose that $u_ k+h_ i\to u+h_ i$ in extended capacity on every $W_ i$. Fix $l$, a compact set $K\subset W'_ l$ and $\delta >0$, and cover $K$ by finitely many compact sets $K_ i\subset W_ i\cap W'_ l$. The smooth function $h'_ l-h_ i$ is bounded on $K_ i$, say by $H_ i$, so the inequality just proved, applied with $h=h'_ l-h_ i$, gives
\[ K_ i\cap \{ d_*(u_ k+h'_ l,u+h'_ l)>\delta \} \subset K_ i\cap \{ d_*(u_ k+h_ i,u+h_ i)>\delta /(2+2H_ i^2)\} . \]
By lemma 13.7.1, the outer capacity of the left side, computed in the chart $W'_ l$, is at most a constant times the outer capacity of the right side, computed in $W_ i$, which tends to zero. By subadditivity of outer capacity, the outer capacity of $K\cap \{ d_*(u_ k+h'_ l,u+h'_ l)>\delta \} $ in $W'_ l$ tends to zero. Thus extended capacity convergence does not depend on the choice of the cover or of the local potentials.
If $u_ k$ decreases to $u$, then for every $C$ the truncations decrease to the bounded plurisubharmonic function $\max \{ u,-C\} $, so they converge in capacity by proposition 7.5.6; the equivalence just proved gives extended capacity convergence.
For the global assertion, put $m_ k=\sup _ Xu_ k$ and $v_ k=u_ k-m_ k$. By proposition 10.3.1, $\int _ X|v_ k|\, \omega ^ n\leq M_0$ for a constant $M_0$. Suppose that $m_ k\to +\infty $ along a subsequence, to which we pass. By Markov's inequality, the $\omega ^ n$-volume of $\{ u_ k<m_ k/2\} =\{ v_ k<-m_ k/2\} $ is at most $2M_0/m_ k$, which tends to zero. On the other hand, let $(W,z)$ be one of the charts of definition 13.7.2, with smooth local potential $h$ of $\theta $, and let $K\subset W$ be a compact set of positive volume, with $|h|\leq H$ and $u+h\leq M$ on $K$. On $K\cap \{ u_ k\geq m_ k/2\} $ we have $u_ k+h\geq m_ k/2-H$, so for large $k$ this set is contained in $K\cap \{ d_*(u_ k+h,u+h)>\delta _0\} $, where $\delta _0=(\pi /2-\arctan M)/2$. The outer capacity in $z(W)$ of the image of the latter set tends to zero, and hence so does its Lebesgue measure, by proposition 7.4.3(3). Since Lebesgue measure in the chart and the $\omega ^ n$-volume are comparable on $K$, the volume of $K\cap \{ u_ k\geq m_ k/2\} $ tends to zero, whereas by the first observation it tends to the volume of $K$, which is positive. This contradiction shows that the suprema are bounded above.
$\square$
The lower semicontinuity of non-pluripolar products under convergence in capacity is proved with the following cutoff weights. They vanish where one of the potentials is at most $-C$, and multiplied by them, non-pluripolar products become Bedford–Taylor products of bounded potentials.
Lemma 13.7.4.88D1663D1111 Let $D\subset \mathbb C^ n$ be a bounded open set and $1\leq p\leq n$. For $1\leq j\leq p$ let $(v_{j,k})_{k\geq 1}$ be a sequence of plurisubharmonic functions on $D$ that is locally uniformly bounded above and converges in extended capacity to a plurisubharmonic function $v_ j$, and suppose that the non-pluripolar products $R_ k=\langle \mathrm{dd}^{\mathrm{c}}v_{1,k}\wedge \cdots \wedge \mathrm{dd}^{\mathrm{c}}v_{p,k}\rangle $ and $R=\langle \mathrm{dd}^{\mathrm{c}}v_1\wedge \cdots \wedge \mathrm{dd}^{\mathrm{c}}v_ p\rangle $ are locally finite. For $C,\varepsilon >0$ put
\[ v_{j,k}^ C=\max \{ v_{j,k},-C\} ,\qquad a_{j,k}=\frac{v_{j,k}^ C+C}{v_{j,k}^ C+C+\varepsilon },\qquad a_ k=\prod _ j a_{j,k}, \]
and define $v_ j^ C$, $a_ j$ and $a$ from the $v_ j$ in the same way. Then:
the functions $a_ k$ and $a$ are Borel and take values in $[0,1]$, the function $a$ is quasi-continuous, and $a_ k\to a$ locally in capacity as $k\to \infty $;
$a_ kR_ k=a_ k\, \mathrm{dd}^{\mathrm{c}}v_{1,k}^ C\wedge \cdots \wedge \mathrm{dd}^{\mathrm{c}}v_{p,k}^ C$ and $aR=a\, \mathrm{dd}^{\mathrm{c}}v_1^ C\wedge \cdots \wedge \mathrm{dd}^{\mathrm{c}}v_ p^ C$, where the products on the right are Bedford–Taylor products;
for fixed $C$, the weight $a$ increases to the indicator function of $\bigcap _ j\{ v_ j>-C\} $ as $\varepsilon \downarrow 0$, and these indicator functions increase to the indicator function of the complement of the union of the pole sets of the $v_ j$ as $C\to \infty $.
Proof.
(1) The weights are Borel functions of the Borel functions $v_{j,k}$ and $v_ j$, and they take values in $[0,1]$ because $v_{j,k}^ C+C\geq 0$ and $v_ j^ C+C\geq 0$. Let $K\subset D$ be compact and $\delta >0$. By theorem 7.5.2 there are open sets $G_ j\subset D$ with $\operatorname {Cap}_ D(G_ j)<\delta /p$ such that $v_ j$ is continuous on $K\setminus G_ j$. Then $a$, a continuous function of $v_1^ C,\ldots ,v_ p^ C$, is continuous on $K\setminus \bigcup _ jG_ j$, and $\operatorname {Cap}_ D(\bigcup _ jG_ j)<\delta $ by subadditivity; thus $a$ is quasi-continuous. By lemma 13.7.3, $v_{j,k}^ C\to v_ j^ C$ locally in capacity. Since $s\mapsto (s+C)/(s+C+\varepsilon )$ is Lipschitz with constant $1/\varepsilon $ on $[-C,\infty )$, and since $|\prod _ jb_ j-\prod _ jb_ j'|\leq \sum _ j|b_ j-b_ j'|$ for numbers in $[0,1]$, the set where $|a_ k-a|>\delta $ is contained in the union over $j$ of the sets where $|v_{j,k}^ C-v_ j^ C|>\varepsilon \delta /p$. By subadditivity of outer capacity, $a_ k\to a$ locally in capacity.
(2) Fix $k$, and let $O=\bigcap _ j\{ v_{j,k}>-C\} $, a plurifine open set. For every integer $m\geq C$, the set $O$ is contained in the level-$m$ set $O_ m=\bigcap _ j\{ v_{j,k}>-m\} $ of the tuple $(v_{j,k})_ j$, and on $O$ the truncations $\max \{ v_{j,k},-m\} $ coincide with $v_{j,k}$, hence with $v_{j,k}^ C$. By lemma 13.2.2, $\mathbf1_{O_ m}R_ k$ is the Bedford–Taylor product of the truncations at level $m$ restricted to $O_ m$, and by theorem 5.47.22 this product coincides on $O$ with $\bigwedge _ j\mathrm{dd}^{\mathrm{c}}v_{j,k}^ C$. Hence $\mathbf1_ OR_ k=\mathbf1_ O\bigwedge _ j\mathrm{dd}^{\mathrm{c}}v_{j,k}^ C$. The weight $a_ k$ vanishes outside $O$, because $a_{j,k}=0$ wherever $v_{j,k}\leq -C$, and multiplying by $a_ k$ gives the first identity. The same argument, applied to the tuple $(v_ j)_ j$, gives the second.
(3) Where $v_ j>-C$ we have $v_ j^ C+C>0$, so $a_ j$ increases to $1$ as $\varepsilon \downarrow 0$; where $v_ j\leq -C$ we have $a_ j=0$. Hence $a$ increases to the indicator function of $\bigcap _ j\{ v_ j>-C\} $, and these sets increase to $\bigcap _ j\{ v_ j>-\infty \} $ as $C\to \infty $.
$\square$
Theorem 13.7.5.67C4F7EC316E Let $T_{j,k}=\theta _ j+\mathrm{dd}^{\mathrm{c}}u_{j,k}$ and $T_ j=\theta _ j+\mathrm{dd}^{\mathrm{c}}u_ j$ be closed positive currents on $X$, for $1\leq j\leq p\leq n$ and $k\geq 1$, and suppose that $u_{j,k}\to u_ j$ in extended capacity as $k\to \infty $, for every $j$. Put $R_ k=\langle T_{1,k}\wedge \cdots \wedge T_{p,k}\rangle $ and $R=\langle T_1\wedge \cdots \wedge T_ p\rangle $. Then for every smooth strongly positive $(n-p,n-p)$-form $\eta $ on $X$,
\[ \varliminf _ k\int _ X R_ k\wedge \eta \geq \int _ X R\wedge \eta . \]
If moreover $\varlimsup _ k\int _ X R_ k\wedge \omega ^{n-p}\leq \int _ X R\wedge \omega ^{n-p}$, then $R_ k\to R$ weakly. The lower inequality also holds locally, on any complex manifold and for compactly supported $\eta $, whenever the local products are finite and the potentials converge in extended capacity and are locally uniformly bounded above.
Proof.
Lower inequality. Work on a coordinate ball $B$ such that $\overline B$ lies in a larger coordinate ball, add fixed smooth local potentials of the $\theta _ j$, defined near $\overline B$, and denote the resulting plurisubharmonic functions by $v_{j,k}$ and $v_ j$. By lemma 13.7.3 (including its independence assertion, which allows us to use the chart $B$), $v_{j,k}\to v_ j$ in extended capacity on $B$, and the $v_{j,k}$ are uniformly bounded above on $B$, because the suprema of the $u_{j,k}$ are bounded above. The local non-pluripolar products of the $v_{j,k}$ and of the $v_ j$ are the restrictions of $R_ k$ and $R$ to $B$, and they are finite by theorem 13.5.4. For $C,\varepsilon >0$ let $v_{j,k}^ C$, $v_ j^ C$, $a_ k$ and $a$ be as in lemma 13.7.4. By that lemma, the weights take values in $[0,1]$, $a$ is quasi-continuous, $a_ k\to a$ locally in capacity, and
\[ a_ k R_ k=a_ k\bigwedge _ j\mathrm{dd}^{\mathrm{c}}v_{j,k}^ C,\qquad aR=a\bigwedge _ j\mathrm{dd}^{\mathrm{c}}v_ j^ C \]
on $B$. Moreover, the plurisubharmonic functions $v_{j,k}^ C\geq -C$ are uniformly bounded on $B$, and they converge to $v_ j^ C$ locally in capacity, by lemma 13.7.3.
Let $\chi \geq 0$ be a smooth function with compact support in $B$. By the weighted capacity continuity of theorem 7.5.8,
\[ \int \chi \, aR\wedge \eta =\lim _ k\int \chi \, a_ kR_ k\wedge \eta \leq \varliminf _ k\int \chi R_ k\wedge \eta , \]
where the inequality holds because $0\leq a_ k\leq 1$ and $R_ k\wedge \chi \eta $ is a positive measure. Now let $\varepsilon \downarrow 0$ and then $C\to \infty $. By lemma 13.7.4(3), the weights $a$ increase to the indicator function of the complement of the union of the pole sets of the $v_ j$, which $R$ does not charge; so monotone convergence gives $\int \chi R\wedge \eta \leq \varliminf _ k\int \chi R_ k\wedge \eta $. This is the local lower inequality; it used only the finiteness of the local products, the extended capacity convergence and the local upper bounds. A finite partition of unity by such functions $\chi $ (proposition 5.2.6) gives the global inequality.
Convergence. By (13.5.5), the masses $\int _ XR_ k\wedge \omega ^{n-p}$ are bounded, since the shifted backgrounds depend only on the fixed forms $\theta _ j$. Near a compact subset $L$ of a chart with Euclidean form $\beta $, we have $\beta \leq c\, \omega $ for some $c>0$ (lemma 6.14.1), and hence $R_ k\wedge \beta ^{n-p}\leq c^{n-p}R_ k\wedge \omega ^{n-p}$ by (13.2.8). Therefore the trace measures of the $R_ k$ are locally uniformly bounded, and by theorem 5.3.7 every subsequence of $(R_ k)$ has a weakly convergent subsequence. Its limit $R'$ is positive, and $R'-R$ is positive, by the lower inequality applied to all smooth strongly positive forms $\eta $ on $X$. The additional hypothesis gives $\int _ X(R'-R)\wedge \omega ^{n-p}\leq 0$, because $\omega ^{n-p}$ is a test form on the compact manifold $X$. Hence the positive measure $(R'-R)\wedge \omega ^{n-p}$ vanishes, so the trace measures of $R'-R$, which are bounded on compact subsets of charts by multiples of it, vanish as well, and $R'-R=0$ by theorem 5.3.7. Thus every subsequence of $(R_ k)$ has a further subsequence converging weakly to $R$, which proves $R_ k\to R$.
$\square$
Example 13.7.6.ACAEA8D8BE87 On $\mathbb P^1$ let $\omega _{\mathrm{FS}}$ be the Fubini–Study form of example 10.6.7, which has total mass one, and put $u=\log |z|^2-\log (1+|z|^2)$ and $u_ k=\max \{ u,-k\} $. As computed in that example, $u$ extends smoothly across infinity and $\omega _{\mathrm{FS}}+\mathrm{dd}^{\mathrm{c}}u=[0]$. Each $u_ k$ is bounded and $\omega _{\mathrm{FS}}$-plurisubharmonic, so $\omega _{\mathrm{FS}}+\mathrm{dd}^{\mathrm{c}}u_ k$ has mass one by proposition 13.5.1. The sequence $u_ k$ decreases to $u$, hence converges to it in extended capacity (lemma 13.7.3), and the measures $\omega _{\mathrm{FS}}+\mathrm{dd}^{\mathrm{c}}u_ k$ converge weakly to $[0]$, because $u_ k\to u$ in $L^1$. However, $\langle [0]\rangle =0$ by example 13.5.6. The weak limit retains the mass that the non-pluripolar product discards at the pole, so the mass hypothesis in theorem 13.7.5 cannot be omitted.
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