Phase Transition in a Random Minima Model: Mean Field Theory and Exact Solution on the Bethe Lattice
Peter Sollich, Satya N Majumdar, Alan J Bray

TL;DR
This paper investigates the phase transition in the number of minima in random landscapes on non-Euclidean lattices, using mean field theory and exact solutions on the Bethe lattice, revealing different critical behaviors and phase transitions.
Contribution
It introduces a mean field theory and an exact Bethe lattice solution for minima distributions, uncovering novel phase transition behaviors and exponents in random landscapes.
Findings
A phase transition at $z_c=2$ with an extensive number of minima above this point.
On the Bethe lattice, a transition with mean field exponent $eta=1/2$ for connectivity $ extgreater 2$.
Inclusion of maxima and minima leads to an additional first order transition.
Abstract
We consider the number and distribution of minima in random landscapes defined on non-Euclidean lattices. Using an ensemble where random landscapes are reweighted by a fugacity factor for each minimum they contain, we construct first a `two-box' mean field theory. This exhibits an ordering phase transition at above which one box contains an extensive number of minima. The onset of order is governed by an unusual order parameter exponent , motivating us to study the same model on the Bethe lattice. Here we find from an exact solution that for any connectivity there is an ordering transition with a conventional mean field order parameter exponent , but with the region where this behaviour is observable shrinking in size as in the mean field limit of large . We show that the behaviour in the transition region can also be understood…
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