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Abstract
The hypothetical Weyl particles in high-energy physics have been discovered in three-dimensional crystals as collective quasiparticle excitations near two-fold degenerate Weyl points. Such momentum-space Weyl particles carry quantised chiral charges, which can be measured by counting the number of Fermi arcs emanating from the corresponding Weyl points. It is known that merging unit-charged Weyl particles can create new ones with more charges. However, only very recently has it been realised that there is an upper limit — the maximal charge number that a two-fold Weyl point can host is four — achievable only in crystals without spin-orbit coupling. Here, we report the experimental realisation of such a maximally charged Weyl point in a three-dimensional photonic crystal. The four charges support quadruple-helicoid Fermi arcs, forming an unprecedented topology of two non-contractible loops in the surface Brillouin zone. The helicoid Fermi arcs also exhibit the long-pursued type-II van Hove singularities that can reside at arbitrary momenta. This discovery reveals a type of maximally charged Weyl particles beyond conventional topological particles in crystals.
Here the authors experimentally demonstrate a maximally charged Weyl point in a three dimensional photonic crystal, with topological charge of four — the maximal charge number that a two-fold Weyl point can host, which supports quadruple-helicoid Fermi arcs
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1 Zhejiang University, Interdisciplinary Centre for Quantum Information, State Key Laboratory of Modern Optical Instrumentation, ZJU-Hangzhou Global Scientific and Technological Innovation Centre, Hangzhou, China (GRID:grid.13402.34) (ISNI:0000 0004 1759 700X); The Electromagnetics Academy at Zhejiang University, Zhejiang University, International Joint Innovation Centre, Key Lab. of Advanced Micro/Nano Electronic Devices & Smart Systems of Zhejiang, Haining, China (GRID:grid.13402.34) (ISNI:0000 0004 1759 700X); Jinhua Institute of Zhejiang University, Zhejiang University, Jinhua, China (GRID:grid.13402.34) (ISNI:0000 0004 1759 700X)
2 Beijing Institute of Technology, Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246); Beijing Institute of Technology, Beijing Key Laboratory of Nanophotonics and Ultrafine Optoelectronic Systems, School of Physics, Beijing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246)
3 Southern University of Science and Technology, Department of Electrical and Electronic Engineering, Shenzhen, China (GRID:grid.263817.9) (ISNI:0000 0004 1773 1790)
4 Singapore University of Technology and Design, Research Laboratory for Quantum Materials, Singapore, Singapore (GRID:grid.263662.5) (ISNI:0000 0004 0500 7631)
5 Nanyang Technological University, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Singapore, Singapore (GRID:grid.59025.3b) (ISNI:0000 0001 2224 0361); Nanyang Technological University, Centre for Disruptive Photonic Technologies, The Photonics Institute, Singapore, Singapore (GRID:grid.59025.3b) (ISNI:0000 0001 2224 0361)