Asymptotic mutual-information conjecture for the sparse stochastic block model

From papers

Let ff denote the unique viscosity solution of the infinite-dimensional Hamilton–Jacobi equation governing the enriched free energy, and let GN\mathbf{G}_N and σ\sigma^* denote the observed graph and latent spins in the sparse stochastic block model. Mutual-information conjecture. The limiting free energy and mutual information are

limNFN=f(1,0),\lim_{N\to\infty}\overline{F}_N=f(1,0),

and

limN1NI(GN;σ)=12E(c+Δσ1σ2)log(c+Δσ1σ2)c2Δm22f(1,0).\lim_{N\to\infty}\frac{1}{N}I(\mathbf{G}_N;\sigma^*)=\frac{1}{2}\operatorname{\mathbb{E}}\big(c+\Delta \sigma_1^*\sigma_2^*\big)\log\big(c+\Delta \sigma_1^*\sigma_2^*\big)-\frac{c}{2}-\frac{\Delta\overline{m}^2}{2}-f(1,0).

The free-energy upper bound is proved, but the matching lower bound—and hence the full asymptotic mutual-information formula—remains open. In the disassortative regime, the paper gives supporting evidence by matching a known variational formula.

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Sources & referencesView supporting material

Primary source

Tomas Dominguez and Jean-Christophe Mourrat, “Mutual information for the sparse stochastic block model”, arXiv:2209.04513 (2023).

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