Low-energy properties of the ferromagnetic metallic phase in manganites: Slave fermion approach to the quantum double exchange model

TL;DR

This paper develops a slave fermion mean-field theory for the quantum double-exchange model to explain the low-energy magnetic and thermodynamic properties of ferromagnetic manganites, revealing spin-charge separation and robust quasiparticle features.

Contribution

It introduces a novel slave fermion approach to the quantum double-exchange model, providing insights into the low-energy behavior of ferromagnetic manganites.

Findings

Electron spectral function shows an incoherent asymmetric peak.

Gauge fluctuations are fully screened by the Anderson-Higgs mechanism.

The mean-field state remains stable with spin-charge separation at low energy.

Abstract

We study the low energy properties of the one-orbital quantum double-exchange model by using the slave fermion formulation. We construct a mean-field theory which gives a simple explanation for the magnetic and thermodynamic properties of the ferromagnetic metallic phase in manganites at low energy. The resulting electron spectral function and tunneling density of states show an incoherent asymmetric peak with weak temperature dependence, in addition to a quasiparticle peak. We also show that the gauge fluctuations in the ferromagnetic metallic phase are completely screened due to the Anderson-Higgs mechanism. Therefore, the mean-field state is robust against gauge fluctuations and exhibits spin-charge separation at low energy.