Machine-learning study of phase transitions in Ising, Blume-Capel, and Ising-metamagnet models

We combine machine-learning techniques with Monte Carlo (MC) simulations and finite-size scaling (FSS) to study continuous and first-order phase transitions in Ising, Blume-Capel, and Ising-metamagnet spin models. We go beyond earlier studies that had concentrated on obtaining the correlation-length exponent ν. In particular, we show (a) how to combine neural networks (NNs), trained with data from MC simulations of Ising-type spin models on finite lattices, with FSS to obtain both thermal magnetic exponents y_{t}=1/ν and y_{h}, respectively, at both critical and tricritical points, (b) how to obtain the NN counterpart of two-scale-factor universality at an Ising-type critical point, and (c) how to get FSS at a first-order transition. We also obtain the FSS forms for the output of our trained NNs as functions of both the temperature and the magnetic field.

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Publication Details

Journal
Physical review. E
Published
2025-05-27
DOI
https://doi.org/10.1103/j3lx-rhyw
Citations
3
Primary Topic
Opinion Dynamics and Social Influence
Type
article
Field-Weighted Citation Impact
3.97

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article

Machine-learning study of phase transitions in Ising, Blume-Capel, and Ising-metamagnet models

Rahul Pandit, Karl J. Friston
3 citations
Physical review. E
Opinion Dynamics and Social Influence
3.97
article

Machine-learning study of phase transitions in Ising, Blume-Capel, and Ising-metamagnet models

Rahul Pandit, Karl J. Friston
article en
3 citations

Abstract

We combine machine-learning techniques with Monte Carlo (MC) simulations and finite-size scaling (FSS) to study continuous and first-order phase transitions in Ising, Blume-Capel, and Ising-metamagnet spin models. We go beyond earlier studies that had concentrated on obtaining the correlation-length exponent ν. In particular, we show (a) how to combine neural networks (NNs), trained with data from MC simulations of Ising-type spin models on finite lattices, with FSS to obtain both thermal magnetic exponents y_{t}=1/ν and y_{h}, respectively, at both critical and tricritical points, (b) how to obtain the NN counterpart of two-scale-factor universality at an Ising-type critical point, and (c) how to get FSS at a first-order transition. We also obtain the FSS forms for the output of our trained NNs as functions of both the temperature and the magnetic field.

Physical review. EVol. 111(6)
Indian Institute of Science Bangalore (IN)
Science and Engineering Research Board
Climate action
Openalex Percentile: Top 7%
Opinion Dynamics and Social Influence
3.97
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