Calculation of the phase of hidden rotating antiferromagnetic order

Abstract

The phase of the rotating order parameter in rotating antiferromagnetism is calculated using a combination of mean-field theory and Heisenberg equation. This phase shows a linear time dependence, which allows us to interpret rotating antiferromagnetism as a synchronized Larmor-like precession of all the spins in the system or as an unusual $\mathbf{q}=(\pi ,\pi )$ spin-wave around a zero local magnetization. We discuss implications for the pseudogap state of high-$T_C$ superconducting materials. Rotating antiferromagnetism has been proposed to model the pseudogap state in these materials.

References in corpus (4)

• From a single-band metal to a high-temperature superconductor via two thermal phase transitions
• From a single-band metal to a high-temperature superconductor via two thermal phase transitions (Supporting Material)
• Enhancement of the Nernst effect by stripe order in a high-Tc superconductor
• Nernst and Seebeck Coefficients of the Cuprate SuperconductorYBa${}_2$Cu${}_3$O${}_{6.67}$: A Study of Fermi Surface Reconstruction

Cited by in corpus (2)

• Theory of the Magnetic Resonance for the High-$T_C$ Copper-Oxide Superconductors
• Effect of the Fermi surface reconstruction on the self-energy of the copper-oxide superconductors