About me

I am an Associate Professor (Universitetslektor) working at Uppsala University and holder of the title of docent (Finnish: dosentti, equivalent to habilitation). I am interested in interactions between various aspects of pure mathematics, focussing on dimension theory, random geometry, and dynamical systems.

Previously, I was holder of the Horizons Europe Marie Skłodowska-Curie Action European Fellowship (MSCA-EF) “Dimension and Dynamics” working at the University of Oulu (Finland) and FWF Lise Meitner Senior Fellow at the University of Vienna (Austria). I was also at the University of Waterloo (Canada) for a postdoc fellowship and completed my doctorate at the University of St Andrews (Scotland) under the supervision of Kenneth Falconer and Mike Todd.


Recent Updates

Below are the most recent pages that I added to this webpage. They may take the form of articles or news items. A full list of either can be found on the News tab.

Jyväskylä Summer School 2025

Jyväskylä Summer School 2025

I am teaching the summer school course Random Geometry and Embeddability (MA3) at the 34$^{th}$ Jyväskylä summer school course. Here you can (eventually) find extra information on the course such as exercises, resources, and handwritten notes.

Article: Dynamical covering sets

Article: Dynamical covering sets

A few days ago, I uploaded a joint article with Balazs Barany and Henna Koivusalo to arXiv. The article is called Dynamical covering sets in self-similar sets and I will briefly summarise the paper here.

TLDR: Imagine you are trying to cover the circle $\mathbb{S}^1$ with randomly centred balls $B(x_k,r_k)$, where $x_k$ is distributed uniformly on $\mathbb{S}^1$ and $r_k$ is a decreasing sequence. The Dvoretzky covering question1 asks for conditions on $r_k$ for the whole circle to be covered almost surely. Similarly, one can ask for when the cover is of full measure, or what size the covering set is.

In this article, we study an analogous dynamical problem for symbolic balls (cylinders) in self-similar sets, where we pick our initial point according to Bernoulli measures. We obtain a single pressure formula that describes the entire dimension theory, which shows distinct regions to the (known) homogeneous case.