Bosonization of 2D Fermions due to Spin and Statistical Magnetic Field Coupling and Possible Nature of Superconductivity and Pseudogap Phases Below E_g

TL;DR

This paper explores how spin interactions induce bosonization of anyons in 2D systems, and proposes a model explaining the pseudogap phase and phase transitions in high-temperature superconductors.

Contribution

It introduces a bosonization mechanism via spin and magnetic field coupling and applies it to interpret experimental phase diagrams of high-T_c superconductors.

Findings

Exact cancellation of fractional statistics terms in anyon gas energy calculations.

Bosonization of anyons due to spin-magnetic field coupling.

Qualitative and quantitative agreement with experimental phase diagrams.

Abstract

A ground state energy variational calculation of anyon gas with Hamiltonian included the interaction of spins of particles with anyon vector potential induced, i.e. statistical, magnetic field exhibits exact cancelation of terms connected with fractional statistics. This leads to bosonization of anyons due to coupling of their spins with statistical magnetic field. We presume that at the dense gas fluctuations of effective spins destroy the coupling and bosons become anyons. At the assumption that pseudogap (PG) boundary is temperature independent and when anyons are fermions we use this model to interpret experimental phase diagrams of Tallon and Loram hole and electron doped High-T_c superconductors below PG energy E_g and find the qualitative and quantitative agreement. We do the hypothesis that phase transition (PT) of bosons into Bose-Einstein condensate is not of second order, but of first order, close to second one, PG regime is meta stable phase of bosons, and E_g=0 is the critical point of this PT. Bosons undergo PT into fermions on PG boundary. Described in the literature non-Fermi quasi-particles might be related to bosons with effective spins.