A new Fractal Mean-Field analysis in phase transition

TL;DR

This paper introduces a fractal mean-field approach to analyze correlations in second-order phase transitions, extending classical theories to non-integer dimensions and linking fractal geometry with critical scaling behavior.

Contribution

It develops a novel fractal framework for understanding correlation functions at criticality, generalizing Fisher's theory to non-integer dimensions and establishing geometric relations between fractal dimensions.

Findings

Derives a relation between correlation fractal dimension and Fisher exponent.

Extends critical scaling laws to non-integer spatial dimensions.

Confirms the validity of Rushbrooke scaling relation in fractal dimensions.

Abstract

Understanding phase transitions requires not only identifying order parameters but also characterizing how their correlations behave across scales. By quantifying how fluctuations at distinct spatial or temporal points are related, correlation functions reveal the structural organization of complex systems. Here, we revisit the theoretical foundations of these correlations in systems undergoing second-order phase transitions, with emphasis on the Ising model extended to non-integer spatial dimensions. Starting from the classical framework introduced by Fisher, we discuss how the standard Euclidean treatment, restricted to integer dimensions, necessitates the introduction of the critical exponent $\eta$ to capture the spatial decay of correlations at $T=T_c$. We suppose that, at criticality, the equilibrium dynamics become effectively confined to the fractal edge of spin clusters. Within this framework, the fractal dimension that governs the correlations in that subspace is directly related to Fisher exponent, which quantifies the singular behavior of the correlation function near criticality. Importantly, this correlation fractal dimension is distinct from the fractal dimension associated with the order parameter. We further derive an explicit geometrical relation connecting the two fractal dimensions, thereby linking spatial self-similarity to the observed scaling behavior at criticality. This treatment naturally extends to non-integer spatial dimensions, which remain valid below the upper critical dimension and produce the correct value of Fisher exponent $\eta$ for a continuous space dimension. Our analysis also confirms that the Rushbrooke scaling relation, continues to hold when the spatial dimension is treated as a continuous parameter, reinforcing the universality of critical scaling and underscoring the role of fractal geometry in characterizing correlations at criticality.