Pome

Theorem 15.5.1CA29182325B0

Theorem 15.5.1.CA29182325B0 Let $p>1$ and let $u\in \mathrm{PSH}(X,\omega )\cap L^\infty (X)$ solve

\[ \mathrm{MA}_\omega (u)=f\, \mathrm{d}V,\qquad 0\leq f\in L^ p(\mathrm{d}V). \]

Then $u$ is Hölder continuous with every exponent

\[ 0<\beta <\frac{2(p-1)}{np+3(p-1)}. \]

The Hölder constants are uniform for a fixed bound $-C_0\leq u\leq 0$ and a fixed bound for $\| f\| _ p$. In particular, the continuous solutions constructed in theorem 14.19.2 have this regularity.

Proof. After adding a constant we may assume $-C_0\leq u\leq 0$. Choose

\[ 0<\eta <\frac{p-1}{np+p-1},\qquad \alpha =2\eta <1. \]

For small $\delta >0$ set

\[ c=\delta ^\alpha ,\qquad e=Ac+2K\delta ,\qquad r=-C_0-1,\qquad v_\delta =\frac{\Phi _{c,\delta }+er}{1+e}. \]

The curvature estimate of lemma 5.42.1 gives $v_\delta \in \mathrm{PSH}(X,\omega )$. Evaluating the infimum defining $\Phi _{c,\delta }$ at $t=\delta $ gives $\Phi _{c,\delta }\leq R_\delta u\leq 0$. On the other hand,

\[ \Phi _{c,\delta }\geq u-K(\delta ^2+\delta ), \]

since $R_ tu+Kt^2\geq u$, $Kt\geq 0$ and $-c\log (t/\delta )\geq 0$ for $0<t\leq \delta $. For small $\delta $ this lower bound is at least $r$, and therefore

\[ v_\delta \leq \Phi _{c,\delta }\leq R_\delta u\leq 0. \]

The Hermitian form $\omega $ is semipositive and big, so theorem 15.4.1 applies in the background $\omega $. Together with the $L^1$ estimate of lemma 5.42.2, it gives

\[ \sup _ X(v_\delta -u)_+ \leq C\left(\int _ X(v_\delta -u)_+\, \mathrm{d}V\right)^\eta \leq C\| R_\delta u-u\| _1^\eta \leq C\delta ^\alpha . \]

Since $e\leq C\delta ^\alpha $ and $u-r\leq C_0+1$, it follows that

2D7C0ED421F7 15.5.2
\begin{equation} \Phi _{c,\delta }-u =(1+e)(v_\delta -u)+e(u-r)\leq C\delta ^\alpha . \end{equation}

We now bound the minimizing radius from below. Fix $z$ and a radius $t=t(z)\in (0,\delta ]$ at which the infimum is attained. The lower estimate at this radius and (15.5.2) give

\[ -c\log (t/\delta ) \leq \Phi _{c,\delta }(z)-u(z)+K(\delta ^2+\delta ) \leq C\delta ^\alpha =Cc. \]

Thus $t(z)\geq a\delta $ with the constant $a=\mathrm{e}^{-C}>0$, which is independent of $z$ and $\delta $. Since $R_ su+Ks^2$ is increasing in $s$,

\[ \begin{split} R_{a\delta }u+K(a\delta )^2 & \leq R_ tu+Kt^2\\ & =\Phi _{c,\delta }+K\delta ^2+K\delta -Kt+c\log (t/\delta )\\ & \leq \Phi _{c,\delta }+K\delta ^2+K\delta . \end{split} \]

Combining this with (15.5.2) and the lower bound $R_ su-u\geq -Ks^2$, and setting $s=a\delta $, we obtain

\[ \| R_ su-u\| _\infty \leq Cs^\alpha \]

for every sufficiently small $s>0$.

Finally, let $x,y$ be points at a small distance $d$. The gradient estimate $\| \nabla R_ su\| _\infty \leq C/s$ gives

\[ |u(x)-u(y)|\leq 2Cs^\alpha +C d/s. \]

With $s=d^{1/(1+\alpha )}$, both terms are bounded by a constant times $d^{\alpha /(1+\alpha )}$, and larger distances are controlled by the bound on the oscillation. This proves Hölder continuity with exponent $\alpha /(1+\alpha )$. Letting $\eta $ approach its upper endpoint gives every $\beta $ in the theorem; smaller exponents follow on compact $X$ by changing the constant. $\square$

Cite this page

Comments

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