Anatomy of a young giant component in the random graph

TL;DR

This paper provides a detailed, simplified description of the structure of the giant component in Erdős-Rényi random graphs near the phase transition, enabling precise analysis of its properties.

Contribution

It offers a new, explicit model for the giant component in the supercritical regime, capturing its structure and allowing for analysis of diameter and mixing times.

Findings

The giant component's structure is contiguous with a model involving a 3-regular graph, paths, and Galton-Watson trees.

Derived asymptotics for the diameter of the giant component.

Analyzed the mixing time of random walks on the giant component.

Abstract

We provide a complete description of the giant component of the Erd\H{o}s-R\'enyi random graph $G(n,p)$ as soon as it emerges from the scaling window, i.e., for $p = (1+\epsilon)/n$ where $\epsilon^3 n \to \infty$ and $\epsilon=o(1)$. Our description is particularly simple for $\epsilon = o(n^{-1/4})$, where the giant component $C_1$ is contiguous with the following model (i.e., every graph property that holds with high probability for this model also holds w.h.p. for $C_1$). Let $Z$ be normal with mean $\frac23 \epsilon^3 n$ and variance $\epsilon^3 n$, and let $K$ be a random 3-regular graph on $2\lfloor Z\rfloor$ vertices. Replace each edge of $K$ by a path, where the path lengths are i.i.d. geometric with mean $1/\epsilon$. Finally, attach an independent Poisson($1-\epsilon$)-Galton-Watson tree to each vertex. A similar picture is obtained for larger $\epsilon=o(1)$, in which case the random 3-regular graph is replaced by a random graph with $N_k$ vertices of degree $k$ for $k\geq 3$, where $N_k$ has mean and variance of order $\epsilon^k n$. This description enables us to determine fundamental characteristics of the supercritical random graph. Namely, we can infer the asymptotics of the diameter of the giant component for any rate of decay of $\epsilon$, as well as the mixing time of the random walk on $C_1$.