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| -rw-r--r-- | frsb_kac-rice.tex | 14 |
1 files changed, 6 insertions, 8 deletions
diff --git a/frsb_kac-rice.tex b/frsb_kac-rice.tex index 1427085..880cca7 100644 --- a/frsb_kac-rice.tex +++ b/frsb_kac-rice.tex @@ -10,6 +10,9 @@ filecolor=MidnightBlue, linkcolor=MidnightBlue ]{hyperref} % ref and cite links with pretty colors +\usepackage[style=phys,eprint=true]{biblatex} + +\addbibresource{frsb_kac-rice.bib} \begin{document} \title{Full solution for counting stationary points of mean-field complex energy landscapes} @@ -53,8 +56,8 @@ to the topological characteristics of those minima. Perhaps the most interesting application of this computation is in the context of -optimization problems, see for example \cite{gamarnik2021overlap,alaoui2022sampling,huang2021tight}. A question -that appears there is how to define a `threshold level'. This notion was introduced \cite{cugliandolo1993analytical} in the context of the $p$-spin model, as the energy at which the patches of the same energy in phase-space percolate - hence +optimization problems, see for example \cite{Gamarnik_2021_The, ElAlaoui_2022_Sampling, Huang_2021_Tight}. A question +that appears there is how to define a `threshold level'. This notion was introduced \cite{Cugliandolo_1993_Analytical} in the context of the $p$-spin model, as the energy at which the patches of the same energy in phase-space percolate - hence explaining why dynamics never go below that level. The notion of a `threshold' for more complex landscapes has later been invoked several times, never to our knowledge in a clear and unambiguous @@ -1268,11 +1271,6 @@ Integrating by parts, \end{appendix} - -\bibliographystyle{plain} -\bibliography{frsb_kac-rice} - - - +\printbibliography \end{document} |