Glass--like transition described by toppling of stability hierarchy

TL;DR

This paper analyzes the glass-like transition in high-dimensional random energy landscapes, focusing on the stability hierarchy of critical points and how it topples during the transition, with implications for complex systems.

Contribution

It introduces a detailed analysis of the instability index distribution and the toppling mechanism during the glass-like transition in high-dimensional landscapes, extending previous models.

Findings

Identification of the critical point $m_c$ for the transition.

Scaling law for the typical instability index near the transition.

Observation of the toppling of stability hierarchy in different models.

Abstract

Building on the work of Fyodorov (2004) and Fyodorov and Nadal (2012) we examine the critical behaviour of population of saddles with fixed instability index $k$ in high dimensional random energy landscapes. Such landscapes consist of a parabolic confining potential and a random part in $N\gg 1$ dimensions. When the relative strength $m$ of the parabolic part is decreasing below a critical value $m_c$, the random energy landscapes exhibit a glass-like transition from a simple phase with very few critical points to a complex phase with the energy surface having exponentially many critical points. We obtain the annealed probability distribution of the instability index $k$ by working out the mean size of the population of saddles with index $k$ relative to the mean size of the entire population of critical points and observe toppling of stability hierarchy which accompanies the underlying glass-like transition. In the transition region $m=m_c + \delta N^{-1/2}$ the typical instability index scales as $k = \kappa N^{1/4}$ and the toppling mechanism affects whole instability index distribution, in particular the most probable value of $\kappa$ changes from $\kappa = 0$ in the simple phase ($\delta > 0 $) to a non-zero value $ \kappa_{\max} \propto (-\delta)^{3/2}$ in the complex phase ($\delta < 0$). We also show that a similar phenomenon is observed in random landscapes with an additional fixed energy constraint and in the $p$-spin spherical model.