Pome

Proposition 7.11.221036F9F7DDDA

Proposition 7.11.22.1036F9F7DDDA Let $p\geq 1$.

  1. For every $\varphi \in \mathcal E_0(B)$ and every $T>0$,

    \[ \operatorname {Cap}_ B(\{ \varphi <-T\} ) \leq 2^{n+p}(n+1)!\, e_ p(\varphi )T^{-(n+p)}. \]
  2. Let $\varphi _ j\in \mathcal E_0(B)$ converge in $L^1_{\mathrm{loc}}(B)$, let $u$ be the plurisubharmonic representative of the limit (theorem 5.10.4), and suppose that $E_ p=\sup _ je_ p(\varphi _ j)<\infty $. For every compact set $K\subset B$ there is a constant $C_{K,p}$, depending only on $K$, $p$ and the ball $B$, such that

    52F9E68B74CF 7.11.23
    \begin{equation} \operatorname {Cap}_ B^*(K\cap \{ u<-T\} ) \leq C_{K,p}E_ p^{p/(n+p)}T^{-p}\qquad (T>0). \end{equation}

    In particular, $\operatorname {Cap}^*_ B(K\cap \{ u=-\infty \} )=0$ for every compact set $K\subset B$.

Proof. (1) Let $h$ be a competitor for $\operatorname {Cap}_ B$, that is, $h\in \mathrm{PSH}(B)$ and $0\leq h\leq 1$. The set $\{ \varphi <-T\} $ is open, because $\varphi $ is upper semicontinuous, and it is relatively compact in $B$, because $\varphi $ has zero boundary values. Hence $\nu =\mathbf1_{\{ \varphi <-T\} }(\mathrm{dd}^{\mathrm{c}}h)^ n$ is a finite measure, and it is dominated by $(\mathrm{dd}^{\mathrm{c}}h)^ n$. The tail estimate (7.11.3) of theorem 7.11.2, applied to $\nu $ and $w=h$, involves the constant $\kappa _{n,p}=2^{n+p}(n+1)!M^ n$, where $M\leq 1$ is the oscillation of $h$ on $B$, but not the mass of $\nu $; it gives

\[ \int _{\{ \varphi <-T\} }(\mathrm{dd}^{\mathrm{c}}h)^ n=\nu (\{ \varphi <-T\} ) \leq 2^{n+p}(n+1)!\, e_ p(\varphi )T^{-(n+p)}. \]

Taking the supremum over $h$ proves (1).

(2) Choose an open set $U$ and compact sets $L,L'\subset B$ with $K\subset U\Subset \operatorname{Int}L$ and $L\subset \operatorname{Int}L'$. By the Chern–Levine–Nirenberg inequality (theorem 7.2.5, with the base current $1$ and the pair $L\subset \operatorname{Int}L'$), there is a constant $C_ L$ with $\int _ L(\mathrm{dd}^{\mathrm{c}}h)^ n\leq C_ L$ for every competitor $h$, since $\| h\| _{L^\infty (L')}\leq 1$. The finite measure $\mathbf1_ L(\mathrm{dd}^{\mathrm{c}}h)^ n$ is dominated by $(\mathrm{dd}^{\mathrm{c}}h)^ n$ and has mass at most $C_ L$, so the constant $A_ p$ of theorem 7.11.2 for this measure and $w=h$ is at most

\[ C_{K,p}=\Bigl (1+\frac pn\Bigr )\bigl (2^{n+p}(n+1)!\bigr )^{p/(n+p)}C_ L^{n/(n+p)}. \]

Hence the moment estimate (7.11.4), applied to $\varphi _ j$, gives

\[ \int _ L(-\varphi _ j)^ p(\mathrm{dd}^{\mathrm{c}}h)^ n \leq C_{K,p}E_ p^{p/(n+p)} \]

for all $j$ and all competitors $h$.

We pass this bound to the limit $u$. Since the $\varphi _ j$ are nonpositive, $u\leq 0$ almost everywhere, and hence everywhere by the submean inequality. Fix $S>0$. The truncations $\max \{ \varphi _ j,-S\} $ take values in $[-S,0]$ and converge to the plurisubharmonic function $\max \{ u,-S\} $ in $L^1_{\mathrm{loc}}(B)$, since $t\mapsto \max \{ t,-S\} $ is $1$-Lipschitz. Since $\mathbf1_ L(\mathrm{dd}^{\mathrm{c}}h)^ n\leq (\mathrm{dd}^{\mathrm{c}}h)^ n$, lemma 7.11.9 shows that they also converge in $L^1(\mathbf1_ L(\mathrm{dd}^{\mathrm{c}}h)^ n)$. As $t\mapsto t^ p$ is Lipschitz on $[0,S]$ and $(-\max \{ \varphi _ j,-S\} )^ p\leq (-\varphi _ j)^ p$, it follows that

\[ \begin{aligned} \int _ L(-\max \{ u,-S\} )^ p(\mathrm{dd}^{\mathrm{c}}h)^ n & =\lim _{j\to \infty }\int _ L(-\max \{ \varphi _ j,-S\} )^ p(\mathrm{dd}^{\mathrm{c}}h)^ n\\ & \leq C_{K,p}E_ p^{p/(n+p)}. \end{aligned} \]

Letting $S\to \infty $, monotone convergence gives the same bound for $\int _ L(-u)^ p(\mathrm{dd}^{\mathrm{c}}h)^ n$. The set $U\cap \{ u<-T\} $ is open, because $u$ is upper semicontinuous, and it contains $K\cap \{ u<-T\} $. By Chebyshev's inequality its $(\mathrm{dd}^{\mathrm{c}}h)^ n$-measure is at most $C_{K,p}E_ p^{p/(n+p)}T^{-p}$. Taking the supremum over $h$ bounds $\operatorname {Cap}_ B(U\cap \{ u<-T\} )$, and hence the outer capacity in (7.11.23). Finally, $K\cap \{ u=-\infty \} $ is contained in $K\cap \{ u<-T\} $ for every $T$, so letting $T\to \infty $ shows that it has zero outer capacity. $\square$

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