Pub Date : 2025-12-23DOI: 10.1140/epjb/s10051-025-01112-z
Rahul Chhimpa, Avinash Chand Yadav
We propose a simple model for a sample space reducing (SSR) stochastic process, where the dynamical variable denoting the size of the state space is continuous. In general, one can view the model as a constrained multiplicative stochastic process such that the size of the state space cannot be smaller than a visibility parameter (epsilon .) We study the survival time statistics that reveal a subtle difference from the discrete version of the process. A straightforward generalization can explain the noisy SSR process, characterized by a tunable parameter (lambda in [0, 1].) We also examine the statistics of the size of the state space that follows a power-law distributed probability ({mathbb {P}}_{epsilon }(zle epsilon ) sim z^{-alpha },) with a nontrivial value of the exponent as a function of the tunable parameter (alpha = 1+lambda .)
{"title":"Continuous sample space reducing stochastic process","authors":"Rahul Chhimpa, Avinash Chand Yadav","doi":"10.1140/epjb/s10051-025-01112-z","DOIUrl":"10.1140/epjb/s10051-025-01112-z","url":null,"abstract":"<p>We propose a simple model for a sample space reducing (SSR) stochastic process, where the dynamical variable denoting the size of the state space is continuous. In general, one can view the model as a constrained multiplicative stochastic process such that the size of the state space cannot be smaller than a visibility parameter <span>(epsilon .)</span> We study the survival time statistics that reveal a subtle difference from the discrete version of the process. A straightforward generalization can explain the noisy SSR process, characterized by a tunable parameter <span>(lambda in [0, 1].)</span> We also examine the statistics of the size of the state space that follows a power-law distributed probability <span>({mathbb {P}}_{epsilon }(zle epsilon ) sim z^{-alpha },)</span> with a nontrivial value of the exponent as a function of the tunable parameter <span>(alpha = 1+lambda .)</span></p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"98 12","pages":""},"PeriodicalIF":1.7,"publicationDate":"2025-12-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145831447","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-22DOI: 10.1140/epjb/s10051-025-01105-y
Vasanth Kumar Babu, Rahul Pandit
The Ising spin model has long been the foundational model for studying phase transitions in theoretical statistical physics. In the wake of the explosion of machine-learning (ML) techniques in recent years, the Ising model has been used for ML applications to phase transitions. In this overview, we discuss the applications of ML, via both supervised and unsupervised learning, to the study of phases and transitions in the Ising model. We also discuss transfer learning and provide some examples of its use for neural networks trained on Ising model spin configurations. We conclude with a summary and some future directions.
{"title":"Artificial intelligence and machine learning for phases and transitions in the Ising model: an overview","authors":"Vasanth Kumar Babu, Rahul Pandit","doi":"10.1140/epjb/s10051-025-01105-y","DOIUrl":"10.1140/epjb/s10051-025-01105-y","url":null,"abstract":"<p>The Ising spin model has long been the foundational model for studying phase transitions in theoretical statistical physics. In the wake of the explosion of machine-learning (ML) techniques in recent years, the Ising model has been used for ML applications to phase transitions. In this overview, we discuss the applications of ML, via both supervised and unsupervised learning, to the study of phases and transitions in the Ising model. We also discuss transfer learning and provide some examples of its use for neural networks trained on Ising model spin configurations. We conclude with a summary and some future directions.</p>","PeriodicalId":787,"journal":{"name":"The European Physical Journal B","volume":"98 12","pages":""},"PeriodicalIF":1.7,"publicationDate":"2025-12-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145831420","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-12-17DOI: 10.1140/epjb/s10051-025-01088-w
Haifa A. Alyousef, Shaimaa A. M. Abdelmohsen, Areej Saleh Alqarny, Najla Alotaibi, Younis Ejaz, Muhammad Imran, Hafiz Muhammd Tahir Farid
The rapid progress of various renewable energy conversion methods has driven an increasing demand for efficient energy storage systems. Transition metal oxides are widely utilized as electrodes in supercapacitor devices; nonetheless, however, they suffer from significant drawbacks such as limited surface area and inadequate conductivity. Doping has been recognized as an efficient approach to overcome these limitations. This current research utilized a hydrothermal technique to increase the capacitive characteristics of CoMoO3 by doping with barium ion (Ba2+). Several physical studies were utilized to confirm the crystal structure, enhanced morphology and surface area of Ba-doped CoMoO3, while the physiochemical parameters of doped electrode sample were assessed using several analytical techniques. The examination of energy storage applications included a 3.0 M KOH for performing cyclic voltammetry (CV) studies, galvanic charge–discharge (GCD), and electrochemical impedance spectroscopy (EIS). Ba-doped CoMoO3 nanocomposites exhibit significant Cs values of approximately 1001 F/g with Ed of (20.48 Wh/kg) and Pd of (192 W/kg) showcasing superior charge–discharge cyclic performance. The Ba-doped CoMoO3 electrode material exhibited superior electrochemical properties, rendering it a viable candidate for future supercapacitor devices.