Paper detail

Continuity of halo functions associated to homothecy invariant density bases

Let $\mathcal{B}$ be a collection of open sets in $\mathbb{R}^{n}$ such that, for any $x \in \mathbb{R}^{n}$, there exists a set $U \in \mathcal{B}$ of arbitrarily small diameter {containing $x$.} $\mathcal{B}$ is said to be a \emph{density basis} provided that, given a measurable set $A \subset \mathbb{R}^{n}$, for a.e. $x \in \mathbb{R}^{n}$ we have $$\lim_{k \rightarrow \infty}\frac{1}{|R_{k}|}\int_{R_{k}}χ_{A} = χ_{A}(x)$$ holds for any sequence of sets $\{R_{k}\}$ in $\mathcal{B}$ containing $x$ whose diameters tend to 0. The geometric maximal operator $M_{\mathcal{B}}$ associated to $\mathcal{B}$ is defined on $L^{1}(\mathbb{R}^n)$ by $M_{\mathcal{B}}f(x) = \sup_{x \in R \in \mathcal{B}}\frac{1}{|R|}\int_{R}|f|$. The \emph{halo function} $ϕ$ of $\mathcal{B}$ is defined on $(1,\infty)$ by $$ϕ(u) = \sup \{\frac{1}{|A|}|\{x \in \mathbb{R}^{n} : M_{\mathcal{B}}χ_{A}(x) > \frac{1}{u}\}| : 0 < |A| < \infty\}\;$$ and on $[0,1]$ by $ϕ(u) = u$. It is shown that the halo function associated to any homothecy invariant density basis is a continuous function on $(1,\infty)$. However, an example of a homothecy invariant density basis is provided such that the associated halo function is not continuous at 1.