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Lemma 12.9.12F7130F1BDC30

Lemma 12.9.12.F7130F1BDC30 Let $Q\subset \mathbb R^ m$, $m>2$, be a cube. Suppose that $u$ is a smooth strictly positive solution on a neighborhood of $3Q$ of

\[ \operatorname {div}(A\nabla u+Bu)=0, \qquad \lambda I\leq A\leq \Lambda I,\qquad |B|\leq K, \]

where $A$ is a smooth symmetric matrix field and $B$ is a smooth vector field. Then

\[ \sup _{Q/2}u\leq C\inf _{Q/2}u, \]

where $C$ depends only on $m,\lambda ,\Lambda ,K$ and the side length of $Q$. Derivatives of $A$ and $B$ do not enter $C$.

Proof. We first estimate positive and negative powers, then compare their small moments by an estimate for $\log u$.

For $p\ne 0,1$, test the weak equation by $\eta ^2u^{p-1}$, where $\eta $ is a smooth cutoff. The principal term is

\[ (p-1)\int \eta ^2u^{p-2}\langle A\nabla u,\nabla u\rangle . \]

The other terms contain respectively $2\eta u^{p-1}A\nabla u\cdot \nabla \eta $, $(p-1)\eta ^2u^{p-1}B\cdot \nabla u$, and $2\eta u^ pB\cdot \nabla \eta $. Taking absolute values after moving the principal term to one side and applying Young's inequality absorbs half of its energy. Thus, for either sign of $p$,

011F0AF31DBF 12.9.13
\begin{equation} \int \eta ^2|\nabla u^{p/2}|^2 \leq C_1p^2(1+|p-1|^{-2}) \int (|\nabla \eta |^2+K^2\eta ^2)u^ p, \end{equation}

with $C_1$ depending only on the ellipticity bounds. Each test is legitimate since this individual smooth positive solution is bounded above and away from zero on the cutoff support.

Put $\beta =m/(m-2)>1$ and choose $p_0=\beta ^{-k-1/2}$, with $k$ to be fixed later. Apply the Euclidean Sobolev inequality to $\eta u^{p/2}$ on nested cubes shrinking from $Q$ to $Q/2$. Choose the cutoff gaps proportional to $2^{-j}$ and the powers $p_ j=p_0\beta ^ j$. The positive powers never equal one: the closest two are $\beta ^{-1/2}$ and $\beta ^{1/2}$. Consequently the constants in (12.9.13), together with the cutoff terms from $\nabla (\eta u^{p/2})$, grow at most polynomially in $p_ j$ and exponentially in $j$. Since $\sum _ j(j+1)\beta ^{-j}<\infty $, their iteration product converges. Negative powers give the same calculation for $u^{-1}$. We obtain

DA143DCFAFAB 12.9.14
\begin{equation} \sup _{Q/2}u\leq C_2\left(\fint _ Q u^{p_0}\right)^{1/p_0}, \qquad \inf _{Q/2}u\geq C_2^{-1} \left(\fint _ Q u^{-p_0}\right)^{-1/p_0}. \end{equation}

Here $C_2$ also depends on $p_0$ and the fixed cube size.

Testing instead by $\eta ^2/u$ gives

\[ \int \eta ^2|\nabla \log u|^2 \leq C_3\int (|\nabla \eta |^2+K^2\eta ^2). \]

For every subcube $S\subset Q$ of side length $\ell $, a cutoff supported in $2S\subset 3Q$, equal to one on $S$, has derivative bounded by $C/\ell $. Poincaré's inequality and Cauchy–Schwarz therefore give

\[ \fint _ S|\log u-(\log u)_ S| \leq C_4(1+K\ell )\leq K_0, \]

where $K_0\geq 1$ is uniform and $(\log u)_ S$ denotes the mean. We spell out the exponential consequence of this mean oscillation bound.

Write $f=\log u$ and fix $a>2$. Select the maximal dyadic subcubes $S$ of $Q$ on which $\fint _ S|f-f_ Q|>aK_0$. Their total measure is at most $|Q|/a$. The parent of each selected cube has average at most $aK_0$, hence $|f_ S-f_ Q|\leq 2^ maK_0$. Outside their union, differentiation of dyadic averages gives $|f-f_ Q|\leq aK_0$ almost everywhere. Repeat this selection inside each chosen cube, subtracting its own mean. The union at generation $j$ has measure at most $a^{-j}|Q|$, and outside generation $j+1$ the accumulated mean changes and last oscillation give

\[ |f-f_ Q|\leq (j2^ ma+a)K_0. \]

The intersection of all generations is null. Choosing $c>0$ so that $\exp (c2^ ma)<a$ and summing over the generations yields

\[ \fint _ Q\exp \! \left(\frac{c|f-f_ Q|}{K_0}\right)\leq C_5, \]

with dimensional constants. Now fix $k$ large enough that $p_0<c/K_0$. Multiplying the estimates for the positive and negative exponentials cancels $f_ Q$ and gives

\[ \left(\fint _ Q u^{p_0}\right) \left(\fint _ Q u^{-p_0}\right)\leq C_5^2. \]

Combining this with (12.9.14) proves the result. Every constant comes from the stated coefficient bounds and the fixed cube. $\square$

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