Solution of the critical dynamics of the mean-field Kob-Andersen model

We analytically solve the critical dynamics of the Kob-Andersen kinetically constrained model of supercooled liquids on the Bethe lattice, employing a combinatorial argument based on the cavity method. For arbitrary values of graph connectivity z and facilitation parameter m, we demonstrate that the critical behavior of the order parameter is governed by equations of motion equivalent to those found in mode-coupling theory. The resulting predictions for the dynamical exponents are validated through direct comparisons with numerical simulations that include both continuous and discontinuous transition scenarios.

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Publication Details

Journal
Physical review. E
Published
2025-10-03
DOI
https://doi.org/10.1103/yms3-km6k
Citations
1
Primary Topic
Material Dynamics and Properties
Type
article
Field-Weighted Citation Impact
0.52
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article

Solution of the critical dynamics of the mean-field Kob-Andersen model

Gianmarco Perrupato, Tommaso Rizzo
1 citations
Physical review. E
Material Dynamics and Properties
0.52
article

Solution of the critical dynamics of the mean-field Kob-Andersen model

Gianmarco Perrupato, Tommaso Rizzo
article en
1 citations

Abstract

We analytically solve the critical dynamics of the Kob-Andersen kinetically constrained model of supercooled liquids on the Bethe lattice, employing a combinatorial argument based on the cavity method. For arbitrary values of graph connectivity z and facilitation parameter m, we demonstrate that the critical behavior of the order parameter is governed by equations of motion equivalent to those found in mode-coupling theory. The resulting predictions for the dynamical exponents are validated through direct comparisons with numerical simulations that include both continuous and discontinuous transition scenarios.

Physical review. EVol. 112(4)
Institute for Complex Systems (IT), Bocconi University (IT), Sapienza University of Rome (IT)
Openalex Percentile: Top 32%
Material Dynamics and Properties
0.52
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