Proof.
As in proposition 10.31.15, we build a concave weight from the distribution of $\varphi -u$ and apply the preceding lemma. The moment bound on $\mu $ now yields a differential inequality for this weight, which bounds the depth of $\varphi -u$ under $\mu _ u$.
The envelope identity gives $u\leq \varphi \leq 0$. Put $x=\varphi -u$, defined off the poles, and $N=2n+1$. Since $x\leq -u$ and $\mu _ u\leq \mu $, Hölder's inequality gives the uniform first-moment bound
\[ B:=\int _ Xx\, \mu _ u \leq \int _ X(-u)\, \mathrm{d}\mu \leq \mu (X)^{1-1/m}A_ m^{1/m}=:A_1. \]
Let $H(t)=\mu _ u(\{ x>t\} )$ and $T=\sup \{ t\geq 0:H(t)>0\} $, with $T=0$ if this set is empty; at this point $T$ may be infinite. If $T<\infty $, zero domination applied to $u$ and $\varphi -t$ for $t>T$ gives $u\geq \varphi -T$. It is therefore enough to bound $T$. We may assume $T>1$, and we choose any $S$ with $1<S<T$.
Define, for $t\geq 0$,
\[ g(t)= \begin{cases} ((1+t)^{3/2}H(t))^{-1},& 0\leq t\leq S,\\ (1+t)^{-3/2},& t>S, \end{cases} \qquad F(t)=1+\int _0^ t g(s)\, \mathrm{d}s, \]
and set $W(t)=\int _0^ t F(s)^{1/N}\, \mathrm{d}s$ and $\chi (-t)=-W(t)$. Since $H(S)>0$, $F$ is bounded on the whole half-line, although its bound may depend on $S$ and $u$. It is locally Lipschitz and nondecreasing. Hence $\chi $ has bounded derivative, is increasing and concave, and satisfies the hypotheses of the preceding lemma. Also $W(t)\geq t$ and $W(t)\leq tF(t)^{1/N}$.
Since $H(t)\leq M$, Tonelli's theorem gives a bound independent of $S$ and $u$:
\[ \int _ X F(x)\, \mu _ u =\mu _ u(X)+\int _0^\infty g(t)H(t)\, \mathrm{d}t \leq 3\max (1,M)=:K. \]
Let $p=P_\theta (\varphi -W(x))\in \mathcal E_\varphi $, the envelope of the preceding lemma for this $\chi $. On its contact set the lemma bounds its measure by $F(x)^{n/N}\mu _ u$. Hence, using $N=2n+1$ and the Cauchy–Schwarz inequality,
\[ \begin{split} \int _ X(\varphi -p)^{1/2}\, \mu _ p & \leq \int _ X x^{1/2}F(x)^{(n+1/2)/N}\, \mu _ u\\ & \leq \left(\int _ Xx\, \mu _ u\right)^{1/2} \left(\int _ XF(x)\, \mu _ u\right)^{1/2} \leq \sqrt{KB}. \end{split} \]
The identity $P_\theta [p]=\varphi $ implies $p-\sup _ Xp\leq \varphi $. Since $p\leq \varphi \leq 0$ and $\mu _ p(X)\geq \ell $, the last integral is at least $\ell \sqrt{-\sup _ Xp}$. Consequently
\[ 0\leq -\sup _ Xp\leq KA_1/\ell ^2=:D. \]
Using $W(x)\leq \varphi -p\leq -p$, and applying the moment hypothesis to $p-\sup _ Xp$, we obtain
9E93E3C5CAED
10.31.55
\begin{equation} \int _ XW(x)^ m\, \mathrm{d}\mu \leq 2^{m-1}\bigl (A_ m+D^ m\mu (X)\bigr )<C_0, \end{equation}
where we choose $C_0=1+2^{m-1}(A_ m+D^ m\mu (X))$. This constant is independent of $S$ and $u$.
For $0<t\leq S$, Chebyshev's inequality and $\mu _ u\leq \mu $ give
\[ H(t)\leq C_0W(t)^{-m}, \qquad F'(t)\geq \frac{W(t)^ m}{C_0(1+t)^{3/2}} \quad \text{for almost every }t. \]
Since $W'=F^{1/N}$, the derivative of $(W')^{N+1}$ is at least
\[ \frac{N+1}{NC_0}\, \frac{W^ mW'}{(1+t)^{3/2}}. \]
All functions being differentiated are absolutely continuous on compact intervals. Integrating from $0$ to $t$ and using $W(0)=0$ gives
\[ (W'(t))^{N+1} \geq \frac{N+1}{NC_0(m+1)} \frac{W(t)^{m+1}}{(1+t)^{3/2}}. \]
In particular
\[ W'(t)\geq c_0(1+t)^{-\gamma }W(t)^\kappa , \quad \gamma =\frac{3}{2(N+1)}<1,\quad \kappa =\frac{m+1}{N+1}>1, \]
with $c_0>0$ independent of $S$ and $u$. Integrating the derivative of $W^{1-\kappa }$ over $[1,S]$ yields
\[ (\kappa -1)c_0\int _1^ S(1+t)^{-\gamma }\, \mathrm{d}t \leq W(1)^{1-\kappa }-W(S)^{1-\kappa }\leq 1, \]
because $W(1)\geq 1$. Since the integral on the left diverges as $S\to \infty $, every $S<T$ is bounded by a constant independent of $S$ and $u$, and hence so is $T$. The zero-domination argument at the beginning of the proof now gives $u\geq \varphi -C$. The case $T\leq 1$, which includes $B=0$, was covered there as well.
$\square$
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