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Adam Brown-Sarre

Publications and source records attributed to Adam Brown-Sarre.

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Measure theoretic properties of large products of consecutive partial quotients

The theory of uniform approximation of real numbers motivates the study of products of consecutive partial quotients in regular continued fractions. For any non-decreasing positive function $\varphi:\mathbb{N}\to\mathbb{R}_{\geq 2}$, we determine the Lebesgue measure of the set $\mathcal{F}_{\ell}(\varphi)$ of irrational numbers $x$ whose regular continued fraction $x~=~[a_1(x),a_2(x),\ldots]$ is such that, for infinitely many $n\in\mathbb{N}$, there are two numbers $1\leq j<k \leq n$ satisfying \[ a_{k}(x)\cdots a_{k+\ell-1}(x) \geq \varphi(n), \; a_{j}(x)\cdots a_{j+\ell-1}(x) \geq \varphi(n). \] This result generalizes previous work by Tan and Zhou (Nonlinearity, 2024). A consequence of our result is that the strong law of large numbers for products of $\ell$ consecutive partial quotients is impossible even if the block with the largest product is removed. We also compute the Hausdorff dimension of $\mathcal{F}_3(\varphi)$.

math.NT

Metrical properties of weighted products of consecutive L\"uroth digits

The L\"uroth expansion of a real number $x\in (0,1]$ is the series \[ x= \frac{1}{d_1} + \frac{1}{d_1(d_1-1)d_2} + \frac{1}{d_1(d_1-1)d_2(d_2-1)d_3} + \cdots, \] with $d_j\in\mathbb{N}_{\geq 2}$ for all $j\in\mathbb{N}$. Given $m\in \mathbb{N}$, $\mathbf{t}=(t_0,\ldots, t_{m-1})\in\mathbb{R}_{>0}^{m-1}$ and any function $\Psi:\mathbb{N}\to (1,\infty)$, define \[ \mathcal{E}_{\mathbf{t}}(\Psi)\colon= \left\{ x\in (0,1]: d_n^{t_0} \cdots d_{n+m}^{t_{m-1}}\geq \Psi(n) \text{ for infinitely many} \ n \in\mathbb{N} \right\}. \] We establish a Lebesgue measure dichotomy statement (a zero-one law) for $\mathcal{E}_{\mathbf{t}}(\Psi)$ under a natural non-removable condition $\liminf_{n\to\infty} \Psi(n)>~1$. Let $B$ be given by \[ \log B \colon= \liminf_{n\to\infty} \frac{\log(\Psi(n))}{n}. \] For any $m\in\mathbb{N}$, we compute the Hausdorff dimension of $\mathcal{E}_{\mathbf{t}}(\Psi)$ when either $B=1$ or $B=\infty$. We also compute the Hausdorff dimension of $\mathcal{E}_{\mathbf{t}}(\Psi)$ when $1<B< \infty$ for $m=2$.

math.NT