Coulomb phase diagnostics as function of temperature, interaction range and disorder
arXiv:1212.2112 · doi:10.1103/PhysRevLett.110.107202
Abstract
The emergent gauge field characteristic of the Coulomb phase of spin ice betrays its existence via pinch points in the spin structure factor in reciprocal space which takes the form of a transverse projector at low temperature: . We develop a theory which establishes the fate of the pinch points at low and high temperature, for hard and soft spins, for short- and long-ranged (dipolar) interactions, as well as in the presence of disorder. We find that their detailed shape can be used to read off the relative sizes of entropic and magnetic Coulomb interactions of monopoles in spin ice, and we resolve the question why pinch points have been experimentally observed for HoYTiO even at high temperature in the presence of strong disorder.
4+ pages, 2 eps figures, published version
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- Magnetic-Moment Fragmentation and Monopole Crystallization
- Refrustration and competing orders in the prototypical Dy2Ti2O7 spin ice material
- Fragmentation in Frustrated Magnets -- A review
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- Magnetic clustering, half-moons, and shadow pinch points as signals of a proximate Coulomb phase in frustrated Heisenberg magnets
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- Spin ice thin films: Large-N theory and Monte Carlo simulations
- Coulombic Charge Ice
- Rod motifs in neutron scattering in spin ice
- Charge and spin correlations in the Monopole Liquid
- Random Coulomb antiferromagnets: from diluted spin liquids to Euclidean random matrices
- Deviation from the dipole-ice model in the new spinel spin-ice candidate, MgErSe
- Seeing beyond the light: Vison and photon electrodynamics in quantum spin ice
- A cluster algorithm for Monte Carlo simulations of spin ice
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- The dipolar spin glass transition in three dimensions
- Spinor ice correlation in flat-band electronic states on kagome and pyrochlore lattices with spin-orbit coupling