Pome

Theorem 17.5.20F21AE677873A

Theorem 17.5.20.F21AE677873A Let $u\in \mathcal E(X,\theta ,\phi )$ with $u\leq \phi $. Let $0\leq a<1$, $A>0$ and $\delta >0$, and let $\nu $ be a positive Borel measure on $X$ such that

2646B3091195 17.5.21
\begin{equation} \mu _ u\leq \nu +a\mu _\phi ,\qquad \nu (E)\leq A\operatorname {Cap}_{\theta ,\phi }(E)^{1+\delta } \quad \text{for every Borel set }E\subset X. \end{equation}

Then there is a finite constant $C\geq 0$ such that $\phi -C\leq u\leq \phi $ on $X$. If, in addition, $I=\int _ X(\phi -u)\, \mathrm d\nu <\infty $, then one can take

856E2E7BF89A 17.5.22
\begin{equation} C=2+\frac I{1-a}\left(2\left(\frac A{1-a}\right)^{1/n}\right)^{n/\delta } +\frac1{1-2^{-\delta }}. \end{equation}

Here $\phi -u$ and the sublevel sets $\{ u<\phi -s\} $ are taken on the set where $\phi $ is finite; its complement is pluripolar, hence of zero capacity (proposition 16.25.6) and therefore $\nu $-null.

Proof. We derive a recursive inequality for the capacities of the sublevel sets of $u-\phi $ and iterate it along levels that converge to a finite depth. For $s>0$ put

\[ E_ s=\{ u<\phi -s\} ,\qquad g(s)=\operatorname {Cap}_{\theta ,\phi }(E_ s)^{1/n},\qquad B=\left(\frac A{1-a}\right)^{1/n}. \]

The sets $E_ s$ decrease as $s$ increases, so $g$ is nonincreasing.

We first compare the measures on $E_ s$. Both $u$ and $\phi -s$ belong to $\mathcal E(X,\theta ,\phi )$, so the comparison principle of proposition 16.25.4, applied to $u$ and $\phi -s$, gives $\mu _\phi (E_ s)\leq \mu _ u(E_ s)$. By (17.5.21),

\[ \mu _ u(E_ s)\leq \nu (E_ s)+a\mu _\phi (E_ s)\leq \nu (E_ s)+a\mu _ u(E_ s), \]

and hence $(1-a)\mu _ u(E_ s)\leq \nu (E_ s)$. Since $u$ has full mass relative to $\phi $, proposition 16.25.7 gives $t^ n\operatorname {Cap}_{\theta ,\phi }(E_{s+t})\leq \mu _ u(E_ s)$ for $0<t\leq 1$. Combining this with the last inequality and the capacity bound in (17.5.21), we obtain $t^ ng(s+t)^ n\leq B^ ng(s)^{n(1+\delta )}$, that is,

E2AC3FD3AA08 17.5.23
\begin{equation} t g(s+t)\leq B g(s)^{1+\delta },\qquad s>0,\quad 0<t\leq 1. \end{equation}

By the second assertion of proposition 16.25.7, $g(s)\to 0$ as $s\to \infty $. Choose $s_0>0$ with $2Bg(s_0)^\delta \leq 1$, and put

A41B6BAF1A25 17.5.24
\begin{equation} C=s_0+\frac{2B}{1-2^{-\delta }}g(s_0)^\delta . \end{equation}

We claim that $g(C)=0$. If $g(s_0)=0$, then $C=s_0$ and there is nothing to prove. Otherwise, as long as $g(s_ j)>0$, define inductively

\[ t_ j=2B g(s_ j)^\delta ,\qquad s_{j+1}=s_ j+t_ j. \]

Since $g$ is nonincreasing, $t_ j\leq 2Bg(s_0)^\delta \leq 1$, and (17.5.23) with $s=s_ j$ and $t=t_ j$ gives

\[ g(s_{j+1})\leq \frac{Bg(s_ j)^{1+\delta }}{t_ j}=\frac{g(s_ j)}2. \]

Hence $g(s_ j)\leq 2^{-j}g(s_0)$ and $t_ j\leq 2^{-j\delta }\cdot 2Bg(s_0)^\delta $, so that

\[ s_ j\leq s_0+2B g(s_0)^\delta \sum _{i=0}^\infty 2^{-i\delta }=C \qquad \text{for every }j. \]

If the construction stops because $g(s_ j)=0$ for some $j$, then $g(C)\leq g(s_ j)=0$. Otherwise $g(C)\leq g(s_ j)\leq 2^{-j}g(s_0)$ for every $j$, and again $g(C)=0$. This proves the claim.

Thus $\operatorname {Cap}_{\theta ,\phi }(E_ C)=0$. The capacity bound in (17.5.21) gives $\nu (E_ C)=0$. Since $\phi $ itself is a competitor for $\operatorname {Cap}_{\theta ,\phi }$ (definition 16.25.5), we also have $\mu _\phi (E_ C)\leq \operatorname {Cap}_{\theta ,\phi }(E_ C)=0$. The measure inequality in (17.5.21) therefore gives $\mu _ u(\{ u<\phi -C\} )=0$. As $\phi -C\in \mathcal E(X,\theta ,\phi )$, the domination principle, theorem 16.22.10, yields $u\geq \phi -C$ everywhere.

Now suppose that $I<\infty $. On $E_ s$ the weight $\phi -u$ exceeds $s$, so Markov's inequality gives $\nu (E_ s)\leq I/s$. Taking $t=1$ in the sublevel estimate and using the measure inequality on $E_ s$, we find

\[ g(s+1)^ n\leq \mu _ u(E_ s)\leq \frac{\nu (E_ s)}{1-a} \leq \frac I{(1-a)s}. \]

Choose $s=1+I(2B)^{n/\delta }/(1-a)$ and $s_0=s+1$. Since $(1-a)s>I(2B)^{n/\delta }$, we get $g(s_0)^ n\leq (2B)^{-n/\delta }$, that is, $2Bg(s_0)^\delta \leq 1$. Thus $s_0$ satisfies the condition imposed on it above, and the constant in (17.5.24) is at most $s_0+(1-2^{-\delta })^{-1}$. Since $(2B)^{n/\delta }=\bigl (2(A/(1-a))^{1/n}\bigr )^{n/\delta }$, this is the right side of (17.5.22). The lower bound $\phi -C\leq u$ remains true when $C$ is increased, which proves (17.5.22). $\square$

Cite this page

Comments

Corrections, questions, and mathematical discussion are welcome. Sign in with GitHub to comment. Comments are public.