A nonnegative $C^{1,1}$ density grows at most quadratically away from each of its zeros. If its zero set separates a small ball, a family of parallel segments crossing the zero set therefore contributes at least a constant times $\sqrt t$ to the volume of $\{ f\leq t\} $ for small $t>0$. Excluding this lower bound makes $\{ f>0\} $ connected, and 14.21.3 then gives uniqueness.
Write $\operatorname {Vol}(E)=\int _ E\mathrm{d}V$ for Borel sets $E$.
Theorem 14.21.13.61851D05B072 Let $u,v\in C^2(X)$ satisfy $A,B\geq 0$ and $A^ n=B^ n=f\, \mathrm{d}V$, where $f\geq 0$ is $C^{1,1}$. If
B72083672909
14.21.14
\begin{equation} \liminf _{t\downarrow 0} \frac{\operatorname {Vol}\{ f\leq t\} }{\sqrt t}=0, \end{equation}
then $\{ f>0\} $ is connected and $u-v$ is constant. In particular this holds when $f^{-1/2}\in L^1(\mathrm{d}V)$, with $f^{-1/2}=+\infty $ on $\{ f=0\} $. The exponent $1/2$ is sharp in every dimension $n\geq 3$.
Proof.
Write $Z=\{ f=0\} $. Condition (14.21.14) first implies $\operatorname {Vol}(Z)=0$. We show that the complement of $Z$ in every sufficiently small coordinate ball is connected. Fix such a ball with convex Euclidean image. If the complement of $Z$ in it were disconnected, choose points $a,b$ in different components and small closed disks centered at $a$ and $b$, perpendicular to the segment $[a,b]$ and contained in those respective components. By making the disks small, all parallel segments between corresponding points stay in the ball. Each segment meets $Z$, since otherwise it would connect the two components.
On a fixed coordinate region containing the closed ball, the gradient of $f$ is Lipschitz with some constant $K>0$. Since $f\geq 0$, we have $\nabla f(z)=0$ at every zero $z$, hence
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14.21.15
\begin{equation} f(x)\leq \frac K2|x-z|^2 \end{equation}
whenever the segment from $z$ to $x$ stays in that region. The endpoint disks are compact and disjoint from $Z$, so the parts of the segments near them contain no zeros. Thus every parallel segment contains a zero at a fixed positive distance from its endpoints. For small $t>0$, (14.21.15) gives on that segment an interval of length $2\sqrt{2t/K}$ contained in $\{ f\leq t\} $. Integrating over the transverse disk, which has positive measure, and using that $\mathrm{d}V$ is comparable to coordinate volume, we obtain
\[ \operatorname {Vol}\{ f\leq t\} \geq c\sqrt t \]
for all sufficiently small $t$, contradicting (14.21.14). This proves the local connectedness assertion.
For each such ball, the complement of $Z$ in it is nonempty, since $Z$ has zero volume, and it lies in one component of $U=X\setminus Z$. Two overlapping balls give the same component, because their open overlap contains a point outside $Z$. Since $X$ is connected, all these balls give the same component. Hence $U$ is connected, and 14.21.3 shows that $u-v$ is constant.
If $f^{-1/2}\in L^1$, then, outside the null zero set,
\[ \frac{\operatorname {Vol}\{ f\leq t\} }{\sqrt t} \leq \int _{\{ f\leq t\} }f^{-1/2}\, \mathrm{d}V\longrightarrow 0 \]
by dominated convergence. This proves the sufficient integrability condition. The sharpness assertion follows from the examples in 14.29, as quantified at the end of that section.
$\square$
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