The Collinear Magnetic Phases of the Geometrically-Frustrated Antiferromagnet CuFeO: The Importance of Stacking
arXiv:0807.3948 · doi:10.1103/PhysRevB.78.140407
Abstract
The correct stacking of hexagonal layers is used to obtain accurate estimates for the exchange and anisotropy parameters of the geometrically-frustrated antiferromagnet CuFeO. Those parameters are highly constrained by the stability of a collinear metamagnetic phase between fields of 13.5 and 20 T. Constrained fits of the spin-wave frequencies of the collinear $\uudd $ phase below 7 T are used to identify the magnetic unit cell of the metamagnetic $\uuudd $ phase, which contains two hexagonal layers and 10 Fe spins.
arXiv comment3 Figures
References in corpus (5)
- Inversion symmetry breaking in noncollinear magnetic phase of a triangular lattice antiferromagnet CuFeO2
- Impurity-doping induced ferroelectricity in frustrated antiferromagnet CuFeO2
- Magnetic Interaction in the Geometrically Frustrated Triangular Lattice Antiferromagnet
- Spin phonon induced colinear order and magnetization plateaus in triangular and kagome antiferromagnets. Applications to CuFeO_2
- Long-range magnetic order and spin-lattice coupling in the delafossite CuFeO2
Cited by in corpus (11)
- Quantum Magnetism in Minerals
- Magnetic excitations in the geometric frustrated multiferroic CuCrO
- Mapping the B,T phase diagram of frustrated metamagnet CuFeO2
- Magnons and electromagnons in a spin-lattice-coupled frustrated magnet CuFeO2 as seen via inelastic neutron scattering
- High-field recovery of the undistorted triangular lattice in the frustrated metamagnet CuFeO2
- Non-Collinear Magnetic Phases of a Triangular-Lattice Antiferromagnet and Doped CuFeO
- Spin-Wave Instabilities and Non-Collinear Magnetic Phases of a Geometrically-Frustrated Triangular-Lattice Antiferromagnet
- Partially disordered state and spin-lattice coupling in an S=3/2 triangular lattice antiferromagnet Ag2CrO2
- Low-temperature heat transport of CuFeGaO ( 0--0.12) single crystals
- Critical Anisotropies of a Geometrically-Frustrated Triangular-Lattice Antiferromagnet
- Spin-Driven Bond Order in a 1/5-Magnetization Plateau Phase in a Triangular Lattice Antiferromagnet CuFeO2