2014/11/30 by Maria Hermanns, Kevin O’Brien, Kevin O'Brien +1 · 99 citations
Physics and Astronomy · #Advanced Condensed Matter Physics #Condensed matter physics #Electron #Fermion #Fractionalization #Gauge theory #MAJORANA #Physics #Physics of Superconductivity and Magnetism #Quantum #Quantum mechanics #Quantum spin liquid #Quasiparticle #Spin polarization #State of matter #Superconductivity #Theoretical physics #Topological Materials and Phenomena #cond-mat.str-el
paper · pdf · doi:10.1103/physrevlett.114.157202
published in Physical Review Letters 114(15), 157202 (American Physical Society) · published version
arxiv created 2015/04/15 · openalex publication_date 2015/04/15 · arxiv updated 2015/04/16 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
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 Z2 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 β-Li2IrO3 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.