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A large deviation principle for block models

Published online by Cambridge University Press:  30 June 2025

Christian Borgs
Affiliation:
Berkeley AI Research Group, Department of Electrical Engineering and Computer Science, University of California, Berkeley, CA, USA
Jennifer Chayes
Affiliation:
Department of EECS, Math, Stat, School of Information, University of California, Berkeley, CA, USA
Julia Gaudio
Affiliation:
Department of Industrial Engineering and Management Sciences, Northwestern University, Evanston, IL, USA
Samantha Petti
Affiliation:
Department of Math, Tufts University, Medford, MA, USA
Subhabrata Sen*
Affiliation:
Department of Statistics, Harvard University, Cambridge, MA, USA
*
Corresponding author: Subhabrata Sen; Email: subhabratasen@fas.harvard.edu
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Abstract

We initiate a study of large deviations for block model random graphs in the dense regime. Following [14], we establish an LDP for dense block models, viewed as random graphons. As an application of our result, we study upper tail large deviations for homomorphism densities of regular graphs. We identify the existence of a ‘symmetric’ phase, where the graph, conditioned on the rare event, looks like a block model with the same block sizes as the generating graphon. In specific examples, we also identify the existence of a ‘symmetry breaking’ regime, where the conditional structure is not a block model with compatible dimensions. This identifies a ‘reentrant phase transition’ phenomenon for this problem – analogous to one established for Erdős–Rényi random graphs [13, 14]. Finally, extending the analysis of [34], we identify the precise boundary between the symmetry and symmetry breaking regimes for homomorphism densities of regular graphs and the operator norm on Erdős–Rényi bipartite graphs.

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Type
Paper
Copyright
© The Author(s), 2025. Published by Cambridge University Press
Figure 0

Figure 1. Illustration of the graphon $f_{p,q,r}^{\gamma }$.

Figure 1

Figure 2. Illustration of the graphon $f_p^{\gamma }$.

Figure 2

Figure 3. Illustration of the transformation $I_{45} \mapsto \tau (I_{45})$.

Figure 3

Figure 4. The construction of $\alpha ^{-1}$. The tall solid vertical lines represent the divisions between the intervals $W_{0,1}, \ldots W_{0,3}$, and the tall dashed vertical lines represent the divisions between the intervals $H_1, \ldots H_4$. All arrows indicate that the respective transformations map the specified vertex intervals to vertex intervals by translation.

Figure 4

Figure 5. The construction of $\beta ^{-1}$. The tall solid vertical lines represent the divisions between the intervals $W_{0,1}, \ldots W_{0,3}$, and the tall dashed vertical lines represent the divisions between the intervals $H_1, \ldots H_4$. The arrows corresponding to $\tau ^{-1}$ illustrate that $\tau ^{-1}$ map intervals to intervals by translation. The arrows depicting $\beta ^{-1}$ show that $\beta ^{-1}$ maps adjacent intervals of the form $\tau ^{-1}(b_{\ell }^{ij})$ (shown by horizontal line segments) to vertex intervals by translation.

Figure 5

Figure 6. For $W_0$ the graphon above and $H$ a triangle, the block $I_1 \times I_2$ is not relevant. Increasing the number of edges between $I_1$ and $I_2$ will not increase the number of triangles in the graph since any triangle has at least two vertices coming only from $I_3$.

Figure 6

Figure 7. Illustration of the graphon $f = (f_{ij})_{i,j \in [m]}$ for $m = 3$. The indicated point in the graphon $f$ is in the $(1,2)$ block. The point is mapped to a point in the function $f_{12}$, with a scaled position.

Figure 7

Figure 8. Construction of $g^{\varepsilon }$.