Frost Patterns: The Secret of Jerky Growth ✛ ✎

Original: "On the geometry of locally growing Loewner chains"
· Eveliina Peltola, Anne Schreuder
arXiv:2607.01142 · 2026-07-01 · arXiv non-exclusive · independent analysis · 2 min
Mathematicians have shown that complex shapes can grow not smoothly, but in fits and starts, like frost patterns on glass.

A frost pattern on a window doesn’t spread evenly: it branches out, seizes voids, advances in jerks. Much like that, the growth of many shapes in nature can be described by a mathematical scheme invented a century ago. Here, a differential equation works like a recipe: you feed in a signal, a driving function, and the recipe tells you how the shape will change. The classic recipe demanded the signal be continuous, like slowly turning a knob. But life is full of sharp jolts.

Even smooth control sometimes throws curveballs. In one problem, a spiral winds around a circle for a long time, then suddenly swallows the entire circle in an instant, like a frost flower suddenly blooming outward.

Mathematicians Eveliina Peltola and Anne Schrøder allowed the signal to “jump” and discovered that each jump adds not a point but a whole chunk to the shape. Sometimes these are bubbles — open regions that suddenly turn up inside, like air pockets in a frost pattern. Other times, they’re dense clusters of boundary points, firmly stuck to the edge. This picture is very important for the Schramm–Loewner evolution (SLE), a branch of mathematics that studies random fractal curves. These curves resemble coastlines or lightning bolts, and their behavior is governed by the laws of probability. When jumps occur in such stochastic processes, the very bubbles and clusters described in the paper appear. This provides a key to numerical simulation of rare events — for instance, sudden ruptures in materials.

Imagine a Markov chain — a sequence of random steps where the next step depends only on the current one. The driving function in such models behaves similarly: its “memory” of the past is limited, and jumps can trigger cascading changes across the whole shape.

Now the theory is ready to describe growth in jerks, and the frost lace on your window gains a coherent meaning. Each pattern is a chronicle of temperature and humidity jumps, frozen into the structure of the ice. And mathematics is learning to read that chronicle to better understand the nonlinear effects around us — from the growth of biofilms to the spread of cracks.

Although the growth equation looks harmless, it can generate astonishing shapes. In one problem, a spiral, winding smoothly, suddenly at the last moment captures an entire disk, as if a frost flower instantly unfurled all its petals.

\partial_t^+ g_t(z) = \frac{2}{g_t(z)-W(t)}
Evolution of the conformal map of the hull
\text{hcap}(K_t) = 2t
Half-plane capacity of the hull grows at rate 2
Scientists
Ludwig BoltzmannJohn von NeumannJosiah Willard GibbsHenri PoincaréAndrey Markov
Concepts
Cope's rule exponential growth topological pattern formation topology central limit theorem limit homotopy Baldwin effect phylogenetic network brain connectivity