Pith. sign in

Spectral signatures of fractionalization in the frustrated Heisenberg model on the square lattice

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
abstract

We employ a variational Monte Carlo approach to efficiently obtain the dynamical structure factor for the spin-1/2 $J_1-J_2$ Heisenberg model on the square lattice. Upon increasing the frustrating ratio $J_2/J_1$, the ground state undergoes a continuous transition from a N\'eel antiferromagnet to a $\mathbb{Z}_{2}$ gapless spin liquid. We identify the characteristic spectral features in both phases and highlight the existence of a broad continuum of excitations in the proximity of the spin-liquid phase. The magnon branch, which dominates the spectrum of the unfrustrated Heisenberg model, gradually loses its spectral weight, thus releasing nearly-deconfined spinons, whose signatures are visible even in the magnetically ordered state. Our results show how free spinons emerge across a quantum critical point, providing evidence for the fractionalization of magnons into deconfined spinons.

citation-role summary

background 1

citation-polarity summary

years

2025 1

verdicts

UNVERDICTED 1

roles

background 1

polarities

support 1

representative citing papers

Fractionalized Fermi liquids and the cuprate phase diagram

cond-mat.str-el · 2025-08-27 · unverdicted · novelty 3.0

Reviews the FL* theory for cuprates using ancilla layer models and SU(2) gauge theories to explain pseudogap hole pockets of area p/8, Fermi arcs, and transitions to d-wave superconductivity and Fermi liquid behavior.

citing papers explorer

Showing 1 of 1 citing paper.

  • Fractionalized Fermi liquids and the cuprate phase diagram cond-mat.str-el · 2025-08-27 · unverdicted · none · ref 166 · internal anchor

    Reviews the FL* theory for cuprates using ancilla layer models and SU(2) gauge theories to explain pseudogap hole pockets of area p/8, Fermi arcs, and transitions to d-wave superconductivity and Fermi liquid behavior.