Cluster-based Haldane state in edge-shared tetrahedral spin-cluster chain: Fedotovite KCuO(SO)
arXiv:1709.06405 · doi:10.1103/PhysRevLett.120.077201
Abstract
Fedotovite KCuO(SO) is a candidate of new quantum spin systems, in which the edge-shared tetrahedral (EST) spin-clusters consisting of Cu are connected by weak inter-cluster couplings to from one-dimensional array. Comprehensive experimental studies by magnetic susceptibility, magnetization, heat capacity, and inelastic neutron scattering measurements reveal the presence of an effective = 1 Haldane state below K. Rigorous theoretical studies provide an insight into the magnetic state of KCuO(SO): an EST cluster makes a triplet in the ground state and one-dimensional chain of the EST induces a cluster-based Haldane state. We predict that the cluster-based Haldene state emerges whenever the number of tetrahedra in the EST is .
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Cited by in corpus (13)
- Quantum Magnetism in Minerals
- Magnetic hexamers interacting in layers in the (Na,K)CuO(SO minerals
- Spin Triplet Ground-State in the Copper Hexamer Compounds A2Cu3O(SO4)3 (A=Na,K)
- Cluster-based Haldane phases, bound magnon crystals and quantum spin liquids of a mixed spin-1 and spin-1/2 Heisenberg octahedral chain
- Spin-Coupling Topology in the Copper Hexamer Compounds ACuO(SO) (A=Na, K)
- Cluster-Based Haldane States in Spin-1/2 Cluster Chains
- Magnetization curves and low-temperature thermodynamics of two spin-1/2 Heisenberg edge-shared tetrahedra
- Insights into nature of magnetization plateaus of a nickel complex [Ni4(CO3)2(aetpy)8](ClO4)4 from a spin-1 Heisenberg diamond cluster
- Imbalanced spin couplings in the copper hexameter compounds A2Cu3O(SO4)3 (A2=Na2, NaK, K2)
- Long range 3D magnetic structures of the spin =1 hexamer cluster fedotovite-like ACuO(SO) (A=K, NaK, Na): a neutron diffraction study
- Quasi-fractionalization of spin in a cluster-based Haldane state supported by chirality of a triangular spin tube
- High-field NMR study of the spin correlations in the spin-cluster mineral NaCuO(SO)
- Parity-dependent phase diagrams in spin-cluster two-leg ladders