Magnetic Order with Fractionalized Excitations: Applications to $\mathrm{Yb}_2 \mathrm{Ti}_2 \mathrm{O}_7$

TL;DR

This paper investigates the emergence of a magnetically ordered state with fractionalized excitations in $ ext{Yb}_2 ext{Ti}_2 ext{O}_7$, explaining experimental neutron scattering data through fermionic parton mean field theory.

Contribution

It demonstrates that a fractionalized magnetically ordered ground state can be stabilized by quantum fluctuations in a realistic spin model, aligning with experimental observations.

Findings

Fractionalized excitations produce a scattering continuum in the spectrum.

High magnetic fields suppress fractionalization, leading to conventional order.

Theoretical results are consistent with neutron scattering experiments.

Abstract

A recent inelastic neutron scattering experiment on $\mathrm{Yb}_2 \mathrm{Ti}_2 \mathrm{O}_7$ uncovers an unusual scattering continuum in the spin excitation spectrum despite the splayed ferromagnetic order in the ground state. While there exist well defined spin wave excitations at high magnetic fields, the one magnon modes and the two magnon continuum start to strongly overlap upon decreasing the field, and eventually they become the scattering continuum at zero field. Motivated by these observations, we investigate the possible emergence of a magnetically ordered ground state with fractionalized excitations in the spin model with the exchange parameters determined from two previous experiments. Using the fermionic parton mean field theory, we show that the magnetically ordered state with fractionalized excitations can arise as a stable mean field ground state in the presence of sufficiently strong quantum fluctuations. The spin excitation spectrum in such a ground state is computed and shown to have the scattering continuum. Upon increasing the magnetic field, the fractionalized magnetically ordered state is suppressed, and is eventually replaced by the conventional magnetically ordered phase at high fields, which is consistent with the experimental data. We discuss further implications of these results to the experiments and possible improvements on the theoretical analysis.