We consider the dilute Curie-Weiss model of size N , which is a generalization of the classical Curie-Weiss model in which the dependency structure between the spins is encoded not by the complete graph but by the (directed) Erdős-Rényi graph on N vertices in which every edge appears independently with probability p ( N ). In the high-temperature regime with an external magnetic field ( 0<β <1,h∈ R 0 < β < 1 , h ∈ R ) we prove for p³N²→ ∞ p 3 N 2 → ∞ sharp cumulant bounds for the magnetization under the annealed Gibbs measure, which imply a central limit theorem with rate, moderate and large deviation principles, a concentration inequality, a normal approximation with Cramér correction and mod-Gaussian convergence.
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Apostel et al. (2026) studied this question.
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