A Renormalized Ginzburg-Landau Framework for Dimensional Crossover and Fluctuation Specific Heat in High- T c Superconductors in a Magnetic Field

arXiv:2609.28705 · cond-mat.supr-con · Submitted 2026-09-23 · Read on arXiv

cond-mat.supr-con

Submitted: 2026-09-23

Updated: 2026-09-23

Comments: 18 pages, 11 figures

License: http://creativecommons.org/licenses/by/4.0/

The gist: This paper presents a theoretical analysis of phase transitions and critical phenomena in high-temperature superconductors using a renormalized Ginzburg-Landau framework.

Terminology

Abstract

This paper presents a theoretical analysis of phase transitions and critical phenomena in high-temperature superconductors using a renormalized Ginzburg-Landau framework. Rather than assuming a conventional linear temperature dependence, we treat the quadratic coefficient as a self-consistent, Hartree-renormalized quantity determined by fluctuation-loop corrections. This renormalization regularizes mean-field divergences and yields a finite, dimensionality-dependent specific-heat anomaly near the transition. When an external magnetic field is applied, minimal coupling quantizes order-parameter fluctuations into discrete Landau levels, reducing the effective dimensionality via an effective spectral dimension. In this framework, the intrinsic fluctuation-coupling strength self-consistently determines the temperature width of the critical Ginzburg region, while the cyclotron energy of the quantized fluctuations uniquely establishes both the specific-heat peak position and the upper-critical-field crossover boundary. Comparison with YBa 2 Cu 3 O 7-δ experimental data demonstrates that this approach captures the suppression of the sharp mean-field discontinuity and accurately reproduces the vortex-lattice topological structure under finite magnetic fields.

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