Spin-charge bound states and emerging fermions in a quantum spin liquid

TL;DR

This paper investigates how holes behave in a quantum spin liquid within a single band model, revealing the formation of long-lived spinon-holon bound states and their potential experimental signatures, linking to pseudogap phenomena.

Contribution

It introduces a field theory approach showing the emergence of spinon-holon bound states in a QSL and connects these to observable features like Fermi arcs.

Findings

Long-lived spinon-holon bound states form due to diverging scattering cross-sections.

Emergent fermions exhibit quasiparticle peaks detectable in spectroscopy.

Fermi pockets resemble Fermi arcs observed in pseudogap phases.

Abstract

The complex interplay between charge and spin dynamics lies at the heart of strongly correlated quantum materials, and it is a fundamental topic in basic research with far reaching technological perspectives. We explore in this paper the dynamics of holes in a single band extended $t-J$ model where the background spins form a $\mathbb{Z}_{2}$ quantum spin liquid (QSL). Using a field theory approach based on a parton construction, we show that while the electrons for most momenta fractionalize into uncorrelated charge carrying holons and spin carrying spinons as generally expected for a QSL, the spinon-holon scattering cross-section diverges for certain momenta signalling strong correlations. By deriving an effective low-energy Hamiltonian describing this dynamics, we demonstrate that these divergencies are due to the formation of long lived spinon-holon bound states. We then show that quantum gas microscopy with atoms in optical lattices provides an excellent platform for verifying and probing the internal spatial structure of these emergent fermions. The fermions will furthermore show up as clear quasiparticle peaks in angle-resolved photoemission spectroscopy with an intensity determined by their internal structure. For a non-zero hole concentration, the fermions form hole pockets with qualitatively the same location, shape, and intensity variation in the Brillouin zone as the so-called Fermi arcs observed in the pseudogap phase. Such agreement is remarkable since the Fermi arcs arise from the delicate interplay between the symmetry of the QSL and the internal structure of the emerging fermions in a minimal single band model with no extra degrees of freedom added. Our results, therefore, provide a microscopic mechanism for the conjectured fractionalized Fermi liquid and open up new pathways for exploring the pseudogap phase and high temperature superconductivity as arising from a QSL.