A tale of stars and cliques

TL;DR

This paper explores the structure of certain hypergraphs, revealing a phase transition between star-like and t-thick configurations, and shows how all such hypergraphs can be decomposed into these components.

Contribution

It introduces a new rescaling phenomenon in hypergraphs, characterizes the densest structures, and provides a decomposition framework for these hypergraphs.

Findings

Densest hypergraphs are either star-dominated or t-thick structures.

A phase transition occurs in hypergraph structure based on edge count.

All hypergraphs in the studied class can be decomposed into t-thick, star, and sparse components.

Abstract

We show that for an infinitely many natural numbers $k$ there are $k$-uniform hypergraphs which admit a `rescaling phenomenon' as described in [9]. More precisely, let $\mathcal{A}(k,I, n)$ denote the class of $k$-graphs on $n$ vertices in which the sizes of all pairwise intersections of edges belong to a set $I$. We show that if $k=rt^2$ for some $r\ge 1$ and $t\ge 2$, and~$I$ is chosen in some special way, the densest graphs in $\mathcal{A}(rt^2,I, n)$ are either dominated by stars of large degree, or basically, they are `$t$-thick' $rt^2$-graphs in which vertices are partitioned into groups of $t$ vertices each and every edge is a union of $tr$ such groups. It is easy to see that, unlike in stars, the maximum degree of $t$-thick graphs is of a lower order than the number of its edges. Thus, if we study the graphs from $\mathcal{A}(rt^2,I, n)$ with a prescribed number of edges $m$ which minimize the maximum degree, around the value of $m$ which is the number of edges of the largest $t$-thick graph, a rapid, discontinuous phase transition can be observed. Interestingly, these two types of $k$-graphs determine the structure of all hypergraphs in $\mathcal{A}(rt^2,I, n)$. Namely, we show that each such hypergraph can be decomposed into a $t$-thick graph $H_T$, a special collection $H_S$ of stars, and a sparse `left-over' graph $H_R$.