Published online by Cambridge University Press: 10 August 2018
Let $f:X\rightarrow X$ be a continuous dynamical system on a compact metric space
$X$ and let
$\unicode[STIX]{x1D6F7}:X\rightarrow \mathbb{R}^{m}$ be an
$m$-dimensional continuous potential. The (generalized) rotation set
$\text{Rot}(\unicode[STIX]{x1D6F7})$ is defined as the set of all
$\unicode[STIX]{x1D707}$-integrals of
$\unicode[STIX]{x1D6F7}$, where
$\unicode[STIX]{x1D707}$ runs over all invariant probability measures. Analogous to the classical topological entropy, one can associate the localized entropy
$\unicode[STIX]{x210B}(w)$ to each
$w\in \text{Rot}(\unicode[STIX]{x1D6F7})$. In this paper, we study the computability of rotation sets and localized entropy functions by deriving conditions that imply their computability. Then we apply our results to study the case where
$f$ is a subshift of finite type. We prove that
$\text{Rot}(\unicode[STIX]{x1D6F7})$ is computable and that
$\unicode[STIX]{x210B}(w)$ is computable in the interior of the rotation set. Finally, we construct an explicit example that shows that, in general,
$\unicode[STIX]{x210B}$ is not continuous on the boundary of the rotation set when considered as a function of
$\unicode[STIX]{x1D6F7}$ and
$w$. In particular,
$\unicode[STIX]{x210B}$ is, in general, not computable at the boundary of
$\text{Rot}(\unicode[STIX]{x1D6F7})$.