Lattice Gauge Theory for Condensed Matter Physics: Ferromagnetic Superconductivity as its Example

TL;DR

This paper reviews lattice gauge theory (LGT) basics for condensed matter physics and demonstrates its application to ferromagnetic superconductivity, revealing phase diagrams and topological excitations through Monte Carlo simulations.

Contribution

It introduces LGT to condensed matter physics and applies it to ferromagnetic superconductivity, providing new insights into phase behavior and topological features.

Findings

LGT effectively models ferromagnetic superconductivity.

Monte Carlo simulations reveal complex phase diagrams.

Identification of vortices of Cooper pairs as topological excitations.

Abstract

Recent theoretical studies of various strongly-correlated systems in condensed matter physics reveal that the lattice gauge theory(LGT) developed in high-energy physics is quite a useful tool to understand physics of these systems. Knowledges of LGT are to become a necessary item even for condensed matter physicists. In the first part of this paper, we present a concise review of LGT for the reader who wants to understand its basics for the first time. For illustration, we choose the abelian Higgs model, a typical and quite useful LGT, which is the lattice verison of the Ginzburg-Landau model interacting with a U(1) gauge field (vector potential). In the second part, we present an account of the recent progress in the study of ferromagnetic superconductivity (SC) as an example of application of LGT to topics in condensed matter physics, . As the ferromagnetism (FM) and SC are competing orders with each other, large fluctuations are expected to take place and therefore nonperturbative methods are required for theoretical investigation. After we introduce a LGT describing the FMSC, we study its phase diagram and topological excitations (vortices of Cooper pairs) by Monte-Carlo simulations.