On The Hausdorff Dimension Of Two Dimensional Badly Approximable Vector
Yi Lou
Abstract
Let $Ψ=(ψ_1,\dots,ψ_m)$ be an approximation function and denote by $\mathcal{A}_m(Ψ)$ the set of $Ψ$-approximable vectors in $[0,1]^m$. The associated set of weighted $Ψ$-badly approximable vectors is defined by $$\mathcal{B}_m(Ψ)=\mathcal{A}_m(Ψ)\setminus\bigcap \limits_{0<c<1}\mathcal{A}_m(cΨ).$$ In this paper, we study the Hausdorff dimension of $\mathcal{B}_m(Ψ)$ in the weighted power-law setting $ψ_i(q)=q^{-τ_i}$. Our main result establishes a sharp local Hausdorff dimension formula for $\mathcal{B}_2(Ψ_{\boldsymbolτ})$ when $\boldsymbolτ=(τ_1,τ_2)$ satisfies $τ_1\geqτ_2>0$ and $τ_1+τ_2>1$. We show that for any ball $B\subseteq[0,1]^2$, $$\dim_{\mathcal{H}}(B\cap \mathcal{B}_2(Ψ_{\boldsymbol τ})) = \dim_{\mathcal{H}} \mathcal{A}_2(Ψ_{\boldsymbol τ}) =\min \left\{\frac{3+τ_1-τ_2}{1+τ_1},\frac{3}{1+τ_2}\right\}.$$ The proof extends the Cantor-type construction and mass distribution arguments of Koivusalo, Levesley, Ward, and Zhang from the unweighted to the weighted setting, and is independent of recent results on weighted exact approximation.
