---
title: Random Regular Graphs
url: https://www.emergentmind.com/topics/random-regular-graph
type: topic
---

# Random Regular Graphs

Searching arXiv for recent and foundational papers on random regular graphs to ground the article.
A random regular graph is a random graph in which every vertex has the same degree. In the standard uniform model \(G(n,d)\), one chooses uniformly from all simple \(d\)-regular graphs on the labeled vertex set \([n]=\{1,\dots,n\}\); equivalently, one may use the configuration model, in which each vertex receives \(d\) half-edges, a uniform perfect matching of the \(nd\) half-edges is sampled, and conditioning on simplicity yields the uniform law on simple \(d\)-regular graphs [1511.01175, 2503.10499]. Because typical instances are sparse, homogeneous, and locally tree-like, random regular graphs form a canonical setting for asymptotic enumeration, exact and approximate sampling, extremal subgraph questions, interacting particle systems, and disordered quantum models [1908.11388, 1712.00367].

## 1. Ensemble, configuration model, and local weak limit

For a simple graph \(G=(V,E)\) on \([n]\), \(d\)-regularity means
\[
\deg_G(v)=d \qquad \text{for all } v\in V.
\]
The state space \(\mathcal G_{n,d}\) consists of all simple \(d\)-regular graphs on \([n]\), and the uniform random \(d\)-regular graph is the uniform distribution on \(\mathcal G_{n,d}\) [1511.01175]. A broader notation \(\mathcal G(n,\mathbf d)\) is used for a prescribed degree sequence \(\mathbf d=(d_1,\dots,d_n)\); the regular case is \(\mathbf d=(d,\dots,d)\) [1906.02886].

The configuration model realizes the same object before conditioning on simplicity. In the formulation used for the random \(d\)-regular configuration model, one partitions \([dN]\) into \(N\) blocks of size \(d\), chooses a uniform perfect matching of the \(dN\) half-edges, and interprets each matched pair as an edge between the corresponding vertices; the result is a random \(d\)-regular multigraph on \([N]\) [2503.10499]. This multigraph is simple with asymptotically positive probability, so high-probability statements proved in the configuration model transfer to the uniform simple model with positive limiting probability [2503.10499].

A central structural fact is local convergence to the infinite \(d\)-regular tree \(\mathbb T_d\). For a uniformly chosen vertex \(i\in[N]\), the radius-\(r\) ball \(B_G(i,r)\) converges in distribution to the radius-\(r\) ball around the root in \(\mathbb T_d\); the same remains valid for \(r=\varepsilon\log N\) with small fixed \(\varepsilon>0\) [2503.10499]. This local weak limit is the basis for transferring tree-based recursion, cavity, and branching arguments to large finite random regular graphs.

## 2. Local geometry, expansion, and effective tree structure

Random regular graphs are locally tree-like in a stronger asymptotic sense than local weak convergence alone. For asymptotically almost every \(G\sim\mathcal G(n,d)\), all but \(o(n)\) vertices have neighborhoods of radius \(\lfloor \log_{d-1}\log n\rfloor\) that are trees, and the diameter is \((1+o(1))\log_{d-1} n\) [1503.04895]. The same paper uses edge-expansion estimates of the form
\[
\Psi_E(G,\varepsilon n)\ge d-2-\delta
\]
for asymptotically almost every \(d\)-regular graph, together with a positive isoperimetric constant, to control spreading processes and metastability [1503.04895].

For random regular graphs of connectivity \(K+1=3\), the number of vertices at graph distance \(x\) from a given vertex grows as
\[
N(x)\sim K^x,
\]
and the typical distance between two random vertices scales as
\[
D\sim \frac{\ln L}{\ln K}.
\]
At distances \(x\) much smaller than the diameter, such graphs look like regular trees with branching number \(K\), while loops are typically long [1908.11388]. This makes random regular graphs a precise, controllable setting for “infinite-dimensional” geometry without the boundary effects of the Bethe lattice: they are finite and homogeneous, and all vertices are equivalent [1908.11388].

In dense degree regimes, random regular graphs also fall into robust-expander classes. In particular, graphs on \(n\) vertices with minimum degree at least \((\tfrac12+o_n(1))n\) are robust expanders, so a random \(d\)-regular graph with \(d>(\tfrac12+o(1))n\) satisfies this condition with high probability [2301.10131]. This robust-expansion viewpoint underlies asymptotic results on perfect matchings and Poisson overlap statistics.

## 3. Sampling, counting, and coupling with binomial random graphs

Algorithmic generation of uniform or nearly uniform random regular graphs has been a longstanding theme. Bayati, Kim, and Saberi gave a nearly-linear-time sequential algorithm for graphs with a prescribed degree sequence when
\[
d_{\max}=O(m^{1/4-\tau}),
\]
producing almost uniform samples in time \(O(m\,d_{\max})\); for regular graphs, they showed that if
\[
d=O(n^{1/2-\tau}),
\]
their algorithm generates an asymptotically uniform \(d\)-regular graph, improving the previous \(d=O(n^{1/3-\tau})\) range due to Kim and Vu [0702124].

A different line, based on switchings in the configuration model, yielded exact and approximate uniform samplers with explicit complexity guarantees. The sampler REG generates \(d\)-regular graphs uniformly at random in expected time
\[
O(nd^3)
\]
for \(d=o(n^{1/2})\), while the approximate sampler REG\(^*\) runs in expected time
\[
O(dn)
\]
and outputs a \(d\)-regular graph whose distribution differs from uniform by \(o(1)\) in total variation distance, again for \(d=o(n^{1/2})\) [1511.01175]. The exact algorithm preserves uniformity by equalizing expected visit counts across strata of pairings, and the approximate version drops the rejection machinery while retaining asymptotic correctness [1511.01175].

Coupling random regular graphs to binomial random graphs provides a complementary transfer principle. Kim and Vu conjectured that if \(d\gg \log n\), then \(\mathcal G(n,d)\) should be asymptotically sandwichable between two Erdős–Rényi graphs with edge probabilities \((1+o(1))d/n\). Gao, Isaev, and McKay proved the conjecture with perfect containment on both sides for all
\[
d\gg \frac{n}{\sqrt{\log n}},
\]
and for smaller \(d=O(n/\sqrt{\log n})\) obtained a weaker sandwich in which the upper parameter is approximately \((d/n)\log n\) [1906.02886]. In the near-regular setting this becomes a general tool for transferring Hamiltonicity, universality, chromatic number, small subgraph counts, diameter, independence number, and edge-percolation thresholds from \(\mathcal G(n,p)\) to \(\mathcal G(n,\mathbf d)\) [1906.02886].

## 4. Factors, perfect matchings, and sprinkling

Uniform perfect matchings in dense regular robust expanders exhibit strong edge-uniformity. If \(G\) is a \(d\)-regular robust \((\nu,\tau)\)-expander on \(n\) vertices, \(M\) is a uniformly chosen perfect matching of \(G\), and \(e\in E(G)\), then
\[
\mathbb P[e\in M]=(1+o_n(1))\,d^{-1}.
\]
Moreover, for any fixed matching \(N\subseteq E(G)\), the random variable \(|M\cap N|\) is asymptotically Poisson with parameter \(d^{-1}|N|\), and for a spanning \(r\)-regular subgraph \(N\subseteq G\) with \(r\le n^{1/50}\), \(|M\cap E(N)|\) is asymptotically Poisson with parameter \(rn/(2d)\) [2301.10131]. Since random \(d\)-regular graphs with \(d>(\tfrac12+o(1))n\) are robust expanders with high probability, these asymptotics describe the typical dense random-regular case as well [2301.10131].

A more structural decomposition question is whether the edge-disjoint union of two random regular graphs behaves like a random regular graph of the combined degree. The conjectural statement is that the distribution of the edge-disjoint union of two random regular graphs on the same vertex set is asymptotically equivalent to a random regular graph of degree \(d_1+d_2\), provided the combined degree grows with \(n\). This has been verified in several regimes: when \(d_1=1\), \(d_2\to\infty\), and \(d_2=o(n^{1/3})\); when
\[
\min\{d_1,d_2,n-d_1-d_2\}=\omega(n/\log n);
\]
and in a dense–sparse regime specified by
\[
\frac{d_2^2}{\min\{d_2,n-d_2\}} \le \frac{2d_1}{3\log n}.
\]
The same work also proves an asymptotic formula for the expected number of spanning regular subgraphs in a random regular graph [2309.00190].

The reduction underlying these sprinkling results identifies concentration of
\[
|\mathcal R_{d_1}(G_{d_1+d_2})|
\]
—the number of spanning \(d_1\)-regular subgraphs of a random \((d_1+d_2)\)-regular graph—as equivalent to the desired coupling between the union model and \(G(n,d_1+d_2)\) [2309.00190]. This is a distinctly regular-graph analogue of the classical sprinkling method for \(G(n,p)\). A plausible implication is that many multi-round exposure arguments in the Erdős–Rényi setting should have regular-graph counterparts whenever factor-count concentration is available.

## 5. Propagation processes, cover times, and finite-graph phase transitions

Bootstrap percolation on random regular graphs leads to an extremal optimization problem: the size of a minimal contagious set. For a \((k+1)\)-regular random graph with threshold \(l\), the cavity method yields several quantitative conjectures, notably
\[
\theta_{\min}(4,3)=\frac16,\qquad \theta_{\min}(5,4)=\frac14,
\]
meaning that 5-regular random graphs with threshold 3, and 6-regular random graphs with threshold 4, have contagious sets of asymptotic density \(1/6\) and \(1/4\), respectively [1407.7361]. Equivalently, these are the minimal fractions of vertices that have to be removed from a 5-regular random graph to destroy its 3-core, and from a 6-regular random graph to destroy its 4-core [1407.7361].

For the contact process on a uniform random \(d\)-regular graph with \(d\ge3\), initialized from full occupancy, the extinction time grows exponentially with the vertex number when \(\lambda>\lambda_1(\mathbb T^d)\), and the normalized extinction time converges in distribution to \(\mathrm{Exp}(1)\) for asymptotically almost every graph [1503.04895]. A more recent result identifies a finite-graph analogue of the second tree critical value \(\lambda_2(d)\). On the random \(d\)-regular configuration model on \([N]\), started from \(\xi_0=\{1\}\), let \(I_k\) be the time of the \(k\)-th reinfection of vertex \(1\). Conditional on survival for \(\omega(1)\) time, for every \(\epsilon\in(0,1)\),
\[
I_{\lfloor\log^\epsilon N\rfloor}=\Theta_{\mathbb P}(\log^\epsilon N)\quad\text{if }\lambda>\lambda_2(d),
\]
whereas
\[
I_{\lfloor\log^\epsilon N\rfloor}=\frac{1}{c_\lambda}\log N+\Theta_{\mathbb P}(\log^\epsilon N)\quad\text{if }\lambda_1(d)<\lambda<\lambda_2(d),
\]
with \(c_\lambda\) the Malthusian growth parameter on \(\mathbb T_d\) [2503.10499]. This identifies the second transition as one between linear reinfections and reinfections following a long healthy period.

Random-walk exploration also acquires explicit asymptotics on random regular graphs. For the biased random walk that always prefers previously unvisited edges, on a random \(r\)-regular graph \(G_r\) with fixed odd \(r\ge3\),
\[
C_V(G_r)\sim \frac{1}{r-2}n\log n,\qquad
C_E(G_r)\sim \frac{r}{2(r-2)}n\log n
\]
with high probability, for vertex and edge cover times respectively [1805.05780]. In parallel, the random-cluster Glauber dynamics on random \(\Delta\)-regular graphs mixes in \(\Theta(n\log n)\) for every \(q\ge1\), \(\Delta\ge3\), and \(p<p_u(q,\Delta)\), with high probability over the graph; via Ullrich’s comparison, this yields \(O(n^2\log n)\) mixing for the Swendsen–Wang dynamics of the \(q\)-state Potts model in the same tree-uniqueness regime [2008.02264].

These results collectively show that random regular graphs are not merely static test cases. They support metastability, dynamic phase transitions, optimal-time MCMC in uniqueness regimes, and exploration laws with explicit constants, all while retaining enough homogeneity for rigorous asymptotics.

## 6. Quantum transport, Anderson localization, and spin glasses

Random regular graphs are a standard substrate for disordered quantum systems because they combine local tree-likeness with global finiteness. In the Anderson model on an RRG of connectivity \(K+1=3\), the Hamiltonian is
\[
\hat H = -\sum_{x\sim y}|x\rangle\langle y|
+\sum_{x=1}^{L} h_x |x\rangle\langle x|,
\qquad h_x\in[-W/2,W/2],
\]
and the graph serves as a proxy for the many-body localization problem on a Fock-space-like graph [1908.11388]. For this connectivity, one study quotes an Anderson transition at
\[
W_{AT}\approx 18.1\pm0.1,
\]
while another uses
\[
W_{AT}\approx 18.2
\]
for the same model [1908.11388, 1805.12354].

The dynamical observable
\[
\Pi(x,t)
\]
—the probability distribution of graph distance from an initial site after time \(t\), projected to a microcanonical window near the band center—reveals four space-time regimes on the RRG. In the delocalized phase, the wave-front position obeys a subdiffusive law
\[
X_{\text{front}}(t)\sim \Gamma(W)\, t^{\beta(W)},\qquad 0<\beta(W)<1,
\]
and the return probability satisfies
\[
\Pi(0,t)\sim \exp[-\Gamma(W)t^{\beta(W)}],
\]
with the Thouless time scaling as
\[
t_{Th}(L)\sim \left(\frac{\ln L}{\ln K}\right)^{1/\beta(W)}.
\]
The same work argues that \(\beta(W)\simeq 1-W/W_{AT}\) over a substantial intermediate-disorder range, and interprets the resulting subdiffusion as relevant to many-body localization on Fock-space-like graphs [1908.11388].

A complementary study of the return probability
\[
R(t)=
\frac{|\langle x|\hat P_{\Delta E} e^{-i\hat H t}\hat P_{\Delta E}|x\rangle|^2}
{|\langle x|\hat P_{\Delta E}|x\rangle|^2}
\]
finds evidence for two distinct phases on the random regular graph: a fully ergodic phase, in which \(R(t)\) decays polynomially with oscillations, and a nonergodic phase, in which the decay is stretched exponential [1805.12354]. Comparing the mean \(\overline{R(t)}\) to the typical value \(\exp(\overline{\log R(t)})\) differentiates an ergodic phase from a nonergodic one, and the paper uses this diagnostic—after benchmarking on PLRBM and Rosenzweig–Porter ensembles—to argue for a nonergodic extended regime in the Anderson model on the RRG [1805.12354].

Random regular graphs also support sparse mean-field spin-glass formulations. For the Ising spin glass on a \(c\)-regular random graph, the local tree-like property motivates cavity/Bethe recursions, but low-temperature analysis requires replica symmetry breaking. A recent construction extends the full RSB scheme to the Ising spin glass on a random regular graph by introducing a martingale approach that replaces the Parisi–Mézard tower of distributions with a well-defined stochastic-process formulation, together with order parameters and self-consistency equations for the free energy [1712.00367]. This suggests that random regular graphs occupy a distinctive position between fully connected SK theory and finite-dimensional disorder: sparse enough to preserve locality, yet mean-field enough to sustain full RSB structures.

Taken together, these developments portray random regular graphs as a unifying substrate for sparse mean-field phenomena. Their local convergence to regular trees supports cavity, branching, and uniqueness arguments; their global homogeneity suppresses boundary artifacts; and their combinatorial rigidity is strong enough to admit exact asymptotics for sampling, factorization, metastability, and quantum transport.

Source: https://www.emergentmind.com/topics/random-regular-graph