Hostname: page-component-77f85d65b8-lfk5g Total loading time: 0 Render date: 2026-03-29T08:11:07.290Z Has data issue: false hasContentIssue false

Percolation on irregular high-dimensional product graphs

Published online by Cambridge University Press:  20 December 2023

Sahar Diskin*
Affiliation:
School of Mathematical Sciences, Tel Aviv University, Tel Aviv, Israel
Joshua Erde
Affiliation:
Institute of Discrete Mathematics, Graz University of Technology, Graz, Austria
Mihyun Kang
Affiliation:
Institute of Discrete Mathematics, Graz University of Technology, Graz, Austria
Michael Krivelevich
Affiliation:
School of Mathematical Sciences, Tel Aviv University, Tel Aviv, Israel
*
Corresponding author: Sahar Diskin; Email: sahardiskin@mail.tau.ac.il
Rights & Permissions [Opens in a new window]

Abstract

We consider bond percolation on high-dimensional product graphs $G=\square _{i=1}^tG^{(i)}$, where $\square$ denotes the Cartesian product. We call the $G^{(i)}$ the base graphs and the product graph $G$ the host graph. Very recently, Lichev (J. Graph Theory, 99(4):651–670, 2022) showed that, under a mild requirement on the isoperimetric properties of the base graphs, the component structure of the percolated graph $G_p$ undergoes a phase transition when $p$ is around $\frac{1}{d}$, where $d$ is the average degree of the host graph.

In the supercritical regime, we strengthen Lichev’s result by showing that the giant component is in fact unique, with all other components of order $o(|G|)$, and determining the sharp asymptotic order of the giant. Furthermore, we answer two questions posed by Lichev (J. Graph Theory, 99(4):651–670, 2022): firstly, we provide a construction showing that the requirement of bounded degree is necessary for the likely emergence of a linear order component; secondly, we show that the isoperimetric requirement on the base graphs can be, in fact, super-exponentially small in the dimension. Finally, in the subcritical regime, we give an example showing that in the case of irregular high-dimensional product graphs, there can be a polynomially large component with high probability, very much unlike the quantitative behaviour seen in the Erdős-Rényi random graph and in the percolated hypercube, and in fact in any regular high-dimensional product graphs, as shown by the authors in a companion paper (Percolation on high-dimensional product graphs. arXiv:2209.03722, 2022).

Information

Type
Paper
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2023. Published by Cambridge University Press
Figure 0

Figure 1. The induction step in Lemma 16.

Figure 1

Figure 2. The vertex $u\in Q$ and its exposed neighbourhood in $T_2$, and a vertex $x\in T_2$ and its exposed neighbourhood in $T_1$. Note that in the course of the exploration process, all the vertices in $N_{G_p}(x,T_2)$ move from $T_1$ to $Q$, the vertex $x$ (and, subsequently, all the vertices from $N_{G_p}(u,T_2)$) move to $S_2$, and, finally, the vertex $u$ moves to $S_1$.

Figure 2

Figure 3. An extension of a partition $A\cup B$ of $W$ to a partition $A'\cup B'$ of $M_{z}$. Each $A'-B'$ two-path (solid) can be extended into an $A-B$ six-path (solid and dashed). Note that some vertices in these paths may lie outside of $M_{z}$.

Figure 3

Figure 4. A visualisation of the graph $G^2[M_{z}]$ in the case $t=4,z=2$ and $s=2$. Here, each circle is a copy of $H(t-z,s)$ and the black tubes represent the edges of $J(t,z)$. A pair of copies of $H(t-z,s)$ have been displayed, where the vertices of $M_{z}$ inside each copy have been coloured according to whether they lie in $A'$ (blue) or $B'$ (orange). Inside the black tube corresponding to the edge of $J(t,z)$ between this pair of vertices there is some matching, represented by the dashed (purple) edges. Note that this matching may not respect the structure of the $H$ copies in each circle. Each vertex $I$ of $J(t,z)$ is then coloured according to whether it is $A'$-dominated (blue), $B'$-dominated (orange) or evenly balanced (green), corresponding to $\chi (I)=1,2,$ and $3$, respectively.

Figure 4

Figure 5. A summary of the typical component structure of percolated high-dimensional product graphs.