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RESEARCH PRODUCT

Topological electronic structure and Weyl points in nonsymmorphic hexagonal materials

Bernardo UribeErick TuiranRafael González-hernándezRafael González-hernández

subject

Materials scienceSymmetry operationPhysics and Astronomy (miscellaneous)FOS: Physical sciences02 engineering and technologyAlgebraic topologyTopology01 natural sciencesDispersion relationMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesFOS: MathematicsAlgebraic Topology (math.AT)General Materials ScienceMathematics - Algebraic Topology010306 general physicsTopological quantum numberCondensed Matter - Materials ScienceCondensed Matter - Mesoscale and Nanoscale PhysicsMaterials Science (cond-mat.mtrl-sci)Charge (physics)021001 nanoscience & nanotechnologyCoupling (probability)Berry connection and curvature0210 nano-technologyGroup theory

description

Using topological band theory analysis we show that the nonsymmorphic symmetry operations in hexagonal lattices enforce Weyl points at the screw-invariant high-symmetry lines of the band structure. The corepresentation theory and connectivity group theory show that Weyl points are generated by band crossings in accordion-like and hourglass-like dispersion relations. These Weyl points are stable against weak perturbations and are protected by the screw rotation symmetry. Based on first-principles calculations we found a complete agreement between the topological predicted energy dispersion relations and real hexagonal materials. Topological charge (chirality) and Berry curvature calculations show the simultaneous formation of Weyl points and nodal-lines in 4d transition-metal trifluorides such as AgF3 and AuF3. Furthermore, a large intrinsic spin-Hall conductivity was found due to the combined strong spin-orbit coupling and multiple Weyl-point crossings in the electronic structure. These materials could be used to the spin/charge conversion in more energy-efficient spintronic devices.

10.1103/physrevmaterials.4.124203https://hdl.handle.net/21.11116/0000-0008-BA87-E21.11116/0000-0008-BA89-C21.11116/0000-0008-BA8A-B