Continuum excitations in a spin-supersolid on a triangular lattice
arXiv:2401.16581 · doi:10.1103/PhysRevLett.133.186704
Abstract
Magnetic, thermodynamic, neutron diffraction and inelastic neutron scattering are used to study spin correlations in the easy-axis XXZ triangular lattice magnet K2Co(SeO3)2. Despite the presence of quasi-2D "supersolid" magnetic order, the low-energy excitation spectrum contains no sharp modes and is instead a broad and structured multi-particle continuum. Applying a weak magnetic field drives the system into an m = 1/3 fractional magnetization plateau phase and restores sharp spin wave modes. To some extent, the behavior at zero field can be understood in terms of spin wave decay. However, the presence of clear excitation minima at the M-points of the Brillouin zone suggest that the spinon language may provide a more adequate description, and signals a possible proximity to a Dirac spin liquid state.
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Cited by in corpus (24)
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- Supersolidity in Rydberg tweezer arrays
- Easy-axis Heisenberg model on the triangular lattice: from supersolid to gapped solid
- From continuum excitations to sharp magnons via transverse magnetic field in the spin-1/2 Ising-like triangular lattice antiferromagnet Na2BaCo(PO4)2
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- Modified large- approach to gapless spin liquids, magnetic orders, and dynamics: Application to triangular lattice antiferromagnets
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- NMR evidence of spin supersolid and Pomeranchuk effect behaviors in the triangular-lattice antiferromagnet RbNi(SeO)
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- Dynamics and thermodynamics of the S = 5/2 almost Heisenberg triangular lattice antiferromagnet K2Mn(SeO3)2
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