23–25 Sept 2026
Accademia Polacca Delle Scienze
Europe/Warsaw timezone

A new exact fractal mean-field analysis in phase transition

25 Sept 2026, 12:00
30m
Accademia Polacca Delle Scienze

Accademia Polacca Delle Scienze

Vicolo Doria 2, Rome
Regular talk Session 8

Speaker

Prof. Fernando de Oliveira (University of Brasilia)

Description

Moving beyond simple associations, researchers need tools to quantify how variables influence each other in space and time. Correlation functions provide a mathematical framework for characterizing these essential dependencies, revealing insights into causality, structure, and hidden patterns within complex systems. In physical systems with many degrees of freedom, such as gases, liquids, and solids, a statistical analysis of these correlations is essential. For a field $\Psi(\vec{x},t)$ that depends on spatial position $\vec{x}$ and time $t$, it is often necessary to understand the correlation with itself at another position and time $\Psi(\vec{x}_0,t_0)$. This specific function is called the autocorrelation function. In this context, the autocorrelation function for order--parameter fluctuations, introduced by Fisher[1], provides an important mathematical framework for understanding the second-order phase transition at equilibrium. However, his analysis is restricted to a Euclidean space of dimension $d$, and an exponent $\eta$ is introduced to correct the spatial behavior of the correlation function at $T=T_c$. In recent work, Lima et al[2] demonstrated that at $T_c$ a fractal analysis is necessary for a complete description of the correlation function. In this study, we investigate the fundamental physics and mathematics underlying phase transitions, emphasizing the deep interplay between scaling behavior, critical exponents, and fractal geometry. {In particular, we show that the application of modern fractional differentials allows us to write down an equation for the correlation function that recovers the correct exponents below the upper critical dimension.} We obtain the exact expression for the Fisher exponent $\eta$. Furthermore, we examine the Rushbrooke scaling relation, which has been questioned in certain magnetic systems, and, drawing on results from the Ising model, we confirm that both our relations and the Rushbrooke scaling law hold even when $d$ is not an integer[3].\

[1] M. E. Fisher, Journal of Mathematical Physics 5, 944322 (1964).\

[2] Lima et al, Phys. Rev. E 110, L062107 (2024).\

[3] Lima et al, Physical Review E 112 (4), 044109 (2025).

Primary authors

Prof. Alex Hansen (Norwegian University of Science and Technology) Dr Henrique Lima (Universidade de Brasília) Prof. Ismael Carrasco (University of Brasilia) Prof. Fernando de Oliveira (University of Brasilia)

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