On homogeneous Newton-Sobolev spaces of functions in metric measure spaces of uniformly locally controlled geometry
Ryan Gibara, Ilmari Kangasniemi, Nageswari Shanmugalingam
TL;DR
This work analyzes when the homogeneous Dirichlet space $D^{1,p}(X)$, defined via upper gradients, coincides with the tame Newton-Sobolev class $N^{1,p}(X)+\mathbb{R}$ on unbounded metric measure spaces with uniformly locally $p$-controlled geometry. It develops a unifying framework based on $p$-modulus, MEC$_p$ property, and uniformization to establish broad non-coincidence results (including globally doubling and Ahlfors-regular settings) and to pinpoint a sharp dichotomy in the hyperbolic setting. A central highlight is the complete classification on standard hyperbolic space $\mathbb{H}^n$: $D^{1,p}(\mathbb{H}^n)=N^{1,p}(\mathbb{H}^n)+\mathbb{R}$ if and only if $1\le p\le n-1$, with counterexamples when $p>n-1$. The paper also develops trace theory and end-analytic characterizations that identify when a $D^{1,p}$ function actually lies in $N^{1,p}$ via behavior along curves to infinity, providing practical criteria for boundary data at infinity.
Abstract
We study the large-scale behavior of Newton-Sobolev functions on complete, connected, proper, separable metric measure spaces equipped with a Borel measure $μ$ with $μ(X) = \infty$ and $0 < μ(B(x, r)) < \infty$ for all $x \in X$ and $r \in (0, \infty)$ Our objective is to understand the relationship between the Dirichlet space $D^{1,p}(X)$, defined using upper gradients, and the Newton-Sobolev space $N^{1,p}(X)+\mathbb{R}$, for $1\le p<\infty$. We show that when $X$ is of uniformly locally $p$-controlled geometry, these two spaces do not coincide under a wide variety of geometric and potential theoretic conditions. We also show that when the metric measure space is the standard hyperbolic space $\mathbb{H}^n$ with $n\ge 2$, these two spaces coincide precisely when $1\le p\le n-1$. We also provide additional characterizations of when a function in $D^{1,p}(X)$ is in $N^{1,p}(X)+\mathbb{R}$ in the case that the two spaces do not coincide.
