Ferromagnetic Coulomb phase in classical spin ice
arXiv:1412.1095 · doi:10.1103/PhysRevB.91.094431
Abstract
Spin ice is a frustrated magnetic system that at low temperatures exhibits a Coulomb phase, a classical spin liquid with topological order and deconfined excitations. This work establishes the presence of a Coulomb phase with coexisting ferromagnetic order in a microscopic model of classical spin ice subject to uniaxial lattice distortion. General theoretical arguments are presented for the presence of such a phase, and its existence is confirmed using Monte Carlo results. This example is used to illustrate generic properties of spin liquids with magnetic order, including deconfinement of monopoles, signatures in the neutron-scattering structure factor, and critical behavior at phase transitions. An analogous phase, a superfluid with spontaneously broken particle-hole symmetry, is demonstrated in a model of hard-core lattice bosons, related to spin ice through the quantum-classical correspondence.
12 pages, 16 figures; v2: new Fig. 9 showing effective potential between monopoles
References in corpus (24)
- Fractionalized excitations in the spin liquid state of a kagomé lattice antiferromagnet
- An RVB phase in the triangular lattice quantum dimer model
- The "Coulomb phase" in frustrated systems
- Spin Ice, Fractionalization and Topological Order
- Fractionalization in an Easy-axis Kagome Antiferromagnet
- Spin Correlations in HoTiO: a Dipolar Spin Ice System
- Coulombic Quantum Liquids in Spin-1/2 Pyrochlores
- Seeing the light : experimental signatures of emergent electromagnetism in a quantum spin ice
- Why spin ice obeys the ice rules
- Magnetic-Moment Fragmentation and Monopole Crystallization
- Critical Exponents of the 3D Ising Universality Class From Finite Size Scaling With Standard and Improved Actions
- Monte Carlo simulation of ice models
- A Three Dimensional Kasteleyn Transition: Spin Ice in a [100] Field
- Spin Liquid Regimes at Nonzero Temperature in Quantum Spin Ice
- Correlations and confinement in non-planar two-dimensional dimer models
- Topological Sector Fluctuations and Curie Law Crossover in Spin Ice
- Spin ice under pressure: symmetry enhancement and infinite order multicriticality
- SU(2)-invariant continuum theory for an unconventional phase transition in a three-dimensional classical dimer model
- Classical-Quantum Mappings for Geometrically Frustrated Systems: Spin Ice in a [100] Field
- Classical to quantum mapping for an unconventional phase transition in a three-dimensional classical dimer model
- Critical behavior in the cubic dimer model at nonzero monomer density
- Critical phenomena in a highly constrained classical spin system: Neel ordering from the Coulomb phase
- Confinement of monopoles and scaling theory near unconventional critical points
- Universal monopole scaling near transitions from the Coulomb phase
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- Angular momentum fluctuations in the convective helium shell of massive stars
- Topological aspects of symmetry breaking in triangular-lattice Ising antiferromagnets
- Generic nearest-neighbour kagome model: XYZ & Dzyaloshinskii-Moriya, and comparison to pyrochlore
- Monopole holes in a partially ordered spin liquid
- Modification of Spin Ice Physics in HoTiO Thin Films
- Tunable critical correlations in kagome ice
- Interplay of symmetry breaking and deconfinement in 3D quantum vertex models
- Symmetry, Superposition and Fragmentation in Classical Spin Liquids: A General Framework and Applications to Square Kagome Magnets
- Fractional Wannier Orbitals and Tight-Binding Gauge Fields for Kitaev Honeycomb Superlattices with Flat Majorana Bands
- Dynamic scaling near the Kasteleyn transition in spin ice: critical relaxation of monopoles and strings following a field quench