Weyl spin liquids
arXiv:1411.7379 · doi:10.1103/PhysRevLett.114.157202
Abstract
The fractionalization of quantum numbers in interacting quantum-many body systems is a central motif in condensed matter physics with prominent examples including the fractionalization of the electron in quantum Hall liquids or the emergence of magnetic monopoles in spin-ice materials. Here we discuss the fractionalization of magnetic moments in three-dimensional Kitaev models into Majorana fermions (and a gauge field) and their emergent collective behavior. We analytically demonstrate that the Majorana fermions form a Weyl superconductor for the Kitaev model on the recently synthesized hyperhoneycomb structure of -LiIrO when applying a magnetic field. We characterize the topologically protected bulk and surface features of this state, which we dub a Weyl spin liquid, including thermodynamic and transport signatures.
published version
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Cited by in corpus (7)
- Line of Dirac Nodes in Hyper-Honeycomb Lattices
- Tunable magnon Weyl points in ferromagnetic pyrochlores
- Spin-orbit physics of j=1/2 Mott insulators on the triangular lattice
- Raman spectroscopic signature of fractionalized excitations in the harmonic-honeycomb iridates - and -LiIrO
- Kitaev materials beyond iridates: order by quantum disorder and Weyl magnons in rare-earth double perovskites
- Fractionalized Metals and Superconductors in Three Dimensions
- From chiral d-wave to nodal line superconductivity in the harmonic honeycomb lattices