The dimension of the set of $\psi$-badly approximable points in all ambient dimensions; on a question of Beresnevich and Velani
Let $\psi:\mathbb{N} \to [0,\infty)$, $\psi(q)=q^{-(1+\tau)}$ and let $\psi$-badly approximable points be those vectors in $\mathbb{R}^{d}$ that are $\psi$-well approximable, but not $c\psi$-well approximable for arbitrarily small constants $c>0$. We establish that the $\psi$-badly approximable p...
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Zusammenfassung: | Let $\psi:\mathbb{N} \to [0,\infty)$, $\psi(q)=q^{-(1+\tau)}$ and let
$\psi$-badly approximable points be those vectors in $\mathbb{R}^{d}$ that are
$\psi$-well approximable, but not $c\psi$-well approximable for arbitrarily
small constants $c>0$. We establish that the $\psi$-badly approximable points
have the Hausdorff dimension of the $\psi$-well approximable points, the
dimension taking the value $(d+1)/(\tau+1)$ familiar from theorems of
Besicovitch and Jarn\'ik. The method of proof is an entirely new take on the
Mass Transference Principle by Beresnevich and Velani (Annals, 2006); namely,
we use the colloquially named `delayed pruning' to construct a sufficiently
large $\liminf$ set and combine this with ideas inspired by the proof of the
Mass Transference Principle to find a large $\limsup$ subset of the $\liminf$
set. Our results are a generalisation of some $1$-dimensional results due to
Bugeaud and Moreira (Acta Arith, 2011), but our method of proof is nothing
alike. |
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DOI: | 10.48550/arxiv.2310.01947 |