{"title":"Efficient Approximation of the CREM Gibbs Measure and the Hardness Threshold","authors":"Fu-Hsuan Ho","doi":"10.1007/s10955-025-03411-2","DOIUrl":null,"url":null,"abstract":"<div><p>The continuous random energy model (CREM) is a toy model of disordered systems introduced by Bovier and Kurkova in 2004 based on previous work by Derrida and Spohn in the 80s. In a recent paper by Addario-Berry and Maillard, they raised the following question: what is the threshold <span>\\(\\beta _G\\)</span>, at which sampling approximately the Gibbs measure at any inverse temperature <span>\\(\\beta >\\beta _G\\)</span> becomes algorithmically hard? Here, sampling approximately means that the Kullback–Leibler divergence from the output law of the algorithm to the Gibbs measure is of order <i>o</i>(<i>N</i>) with probability approaching 1, as <span>\\(N\\rightarrow \\infty \\)</span>, and algorithmically hard means that the running time, the numbers of vertices queries by the algorithms, is beyond of polynomial order. The present work shows that when the covariance function <i>A</i> of the CREM is concave, for all <span>\\(\\beta >0\\)</span>, a recursive sampling algorithm on a renormalized tree approximates the Gibbs measure with running time of order <span>\\(O(N^{1+\\varepsilon })\\)</span>. For <i>A</i> non-concave, the present work exhibits a threshold <span>\\(\\beta _G<\\infty \\)</span> such that the following hardness transition occurs: (a) For every <span>\\(\\beta \\le \\beta _G\\)</span>, the recursive sampling algorithm approximates the Gibbs measure with a running time of order <span>\\(O(N^{1+\\varepsilon })\\)</span>. (b) For every <span>\\(\\beta >\\beta _G\\)</span>, a hardness result is established for a large class of algorithms. Namely, for any algorithm from this class that samples the Gibbs measure approximately, there exists <span>\\(z>0\\)</span> such that the running time of this algorithm is at least <span>\\(e^{zN}\\)</span> with probability approaching 1. In other words, it is impossible to sample approximately in polynomial-time the Gibbs measure in this regime. Additionally, we provide a lower bound of the free energy of the CREM that could hold its value.</p></div>","PeriodicalId":667,"journal":{"name":"Journal of Statistical Physics","volume":"192 3","pages":""},"PeriodicalIF":1.3000,"publicationDate":"2025-03-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10955-025-03411-2.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Statistical Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s10955-025-03411-2","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
引用次数: 0
Abstract
The continuous random energy model (CREM) is a toy model of disordered systems introduced by Bovier and Kurkova in 2004 based on previous work by Derrida and Spohn in the 80s. In a recent paper by Addario-Berry and Maillard, they raised the following question: what is the threshold \(\beta _G\), at which sampling approximately the Gibbs measure at any inverse temperature \(\beta >\beta _G\) becomes algorithmically hard? Here, sampling approximately means that the Kullback–Leibler divergence from the output law of the algorithm to the Gibbs measure is of order o(N) with probability approaching 1, as \(N\rightarrow \infty \), and algorithmically hard means that the running time, the numbers of vertices queries by the algorithms, is beyond of polynomial order. The present work shows that when the covariance function A of the CREM is concave, for all \(\beta >0\), a recursive sampling algorithm on a renormalized tree approximates the Gibbs measure with running time of order \(O(N^{1+\varepsilon })\). For A non-concave, the present work exhibits a threshold \(\beta _G<\infty \) such that the following hardness transition occurs: (a) For every \(\beta \le \beta _G\), the recursive sampling algorithm approximates the Gibbs measure with a running time of order \(O(N^{1+\varepsilon })\). (b) For every \(\beta >\beta _G\), a hardness result is established for a large class of algorithms. Namely, for any algorithm from this class that samples the Gibbs measure approximately, there exists \(z>0\) such that the running time of this algorithm is at least \(e^{zN}\) with probability approaching 1. In other words, it is impossible to sample approximately in polynomial-time the Gibbs measure in this regime. Additionally, we provide a lower bound of the free energy of the CREM that could hold its value.
期刊介绍:
The Journal of Statistical Physics publishes original and invited review papers in all areas of statistical physics as well as in related fields concerned with collective phenomena in physical systems.