\documentclass[fleqn,a4paper]{article} \usepackage[utf8]{inputenc} % why not type "Bézout" with unicode? \usepackage[T1]{fontenc} % vector fonts plz \usepackage{fullpage,amsmath,amssymb,latexsym,graphicx} \usepackage{newtxtext,newtxmath} % Times for PR \usepackage{appendix} \usepackage[dvipsnames]{xcolor} \usepackage[ colorlinks=true, urlcolor=MidnightBlue, citecolor=MidnightBlue, filecolor=MidnightBlue, linkcolor=MidnightBlue ]{hyperref} % ref and cite links with pretty colors \usepackage[ style=phys, eprint=true, maxnames = 100 ]{biblatex} \usepackage{anyfontsize,authblk} \begin{document} \title{ When is the annealed complexity correct? } \author{Jaron Kent-Dobias} \affil{\textsc{DynSysMath}, Istituto Nazionale di Fisica Nucleare, Sezione di Roma} \maketitle \begin{abstract} The difference between quenched and annealed averages is crucial for disordered systems. In isotropic mean-field systems, they differ when replica symmetry is broken. When computing the average free energy in equilibrium, there are robust conditions to understand when {\oldstylenums1}\textsc{rsb} is sufficient. When computing the average complexity, or the number of stationary points of the energy, there is only robust reasoning at the ground state, where a {\oldstylenums1}\textsc{rsb} equilibrium implies that the annealed complexity \emph{at the ground state} is correct. Here, we demonstrate that in the mixed spherical models, the annealed complexity can be wrong away from the ground state even when the equilibrium free energy is guaranteed to be at most {\oldstylenums1}\textsc{rsb} everywhere. Therefore, simple equilibrium order cannot be used to assume a simple landscape geometry. \end{abstract} Parisi construction, $f''(q)^{-1/2}$ is concave \end{document}