arXiv Analytics

Sign in

arXiv:2309.09913 [math.PR]AbstractReferencesReviewsResources

Sharp Phase Transition for Multi Overlap Gap Property in Ising $p$-Spin Glass and Random $k$-SAT Models

Eren C. Kızıldağ

Published 2023-09-18Version 1

The Ising $p$-spin glass and the random $k$-SAT models exhibit symmetric multi Overlap Gap Property ($m$-OGP), an intricate geometrical property which is a rigorous barrier against many important classes of algorithms. We establish that for both models, the symmetric $m$-OGP undergoes a sharp phase transition and we identify the phase transition point for each model: for any $m\in\mathbb{N}$, there exists $\gamma_m$ (depending on the model) such that the model exhibits $m$-OGP for $\gamma>\gamma_m$ and the $m$-OGP is provably absent for $\gamma<\gamma_m$, both with high probability, where $\gamma$ is some natural parameter of the model. Our results for the Ising $p$-spin glass model are valid for all large enough $p$ that remain constant as the number $n$ of spins grows, $p=O(1)$; our results for the random $k$-SAT are valid for all $k$ that grow mildly in the number $n$ of Boolean variables, $k=\Omega(\ln n)$. To the best of our knowledge, these are the first sharp phase transition results regarding the $m$-OGP. Our proofs are based on an application of the second moment method combined with a concentration property regarding a suitable random variable. While a standard application of the second moment method fails, we circumvent this issue by leveraging an elegant argument of Frieze~\cite{frieze1990independence} together with concentration.

Related articles: Most relevant | Search more
arXiv:1809.07742 [math.PR] (Published 2018-09-20)
Capacity lower bound for the Ising perceptron
arXiv:2104.07629 [math.PR] (Published 2021-04-15)
Spin glass to paramagnetic transition in Spherical Sherrington-Kirkpatrick model with ferromagnetic interaction
arXiv:1706.08462 [math.PR] (Published 2017-06-26)
Is the Riemann zeta function in a short interval a 1-RSB spin glass ?