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Abstract
Magnetic topological semimetals allow for an effective control of the topological electronic states by tuning the spin configuration. Among them, Weyl nodal line semimetals are thought to have the greatest tunability, yet they are the least studied experimentally due to the scarcity of material candidates. Here, using a combination of angle-resolved photoemission spectroscopy and quantum oscillation measurements, together with density functional theory calculations, we identify the square-net compound EuGa4 as a magnetic Weyl nodal ring semimetal, in which the line nodes form closed rings near the Fermi level. The Weyl nodal ring states show distinct Landau quantization with clear spin splitting upon application of a magnetic field. At 2 K in a field of 14 T, the transverse magnetoresistance of EuGa4 exceeds 200,000%, which is more than two orders of magnitude larger than that of other known magnetic topological semimetals. Our theoretical model suggests that the non-saturating magnetoresistance up to 40 T arises as a consequence of the nodal ring state.
The tunability of electronic properties is a central goal of research into topological semimetals. Here, the authors report Weyl nodal ring states in the magnetic semimetal EuGa4 and link the nodal ring state to the observed large non-saturating magnetoresistance.
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1 Rice University, Department of Physics and Astronomy, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278); Rice University, Rice Center for Quantum Materials, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278)
2 Rice University, Department of Physics and Astronomy, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278); Rice University, Rice Center for Quantum Materials, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278); Rice University, Applied Physics Graduate Program, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278)
3 National High Magnetic Field Laboratory, Tallahase, USA (GRID:grid.481548.4) (ISNI:0000 0001 2292 2549)
4 Rice University, Department of Physics and Astronomy, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278); Rice University, Rice Center for Quantum Materials, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278); University of California, Department of Physics, Berkeley, USA (GRID:grid.47840.3f) (ISNI:0000 0001 2181 7878)
5 SLAC National Accelerator Laboratory, Stanford Synchrotron Radiation Lightsource, Menlo Park, USA (GRID:grid.445003.6) (ISNI:0000 0001 0725 7771)
6 Lawrence Berkeley National Laboratory, Advanced Light Source, Berkeley, USA (GRID:grid.184769.5) (ISNI:0000 0001 2231 4551)
7 National High Magnetic Field Laboratory, Tallahase, USA (GRID:grid.481548.4) (ISNI:0000 0001 2292 2549); Florida State University, Department of Physics, Tallahassee, USA (GRID:grid.255986.5) (ISNI:0000 0004 0472 0419)
8 University of California, Department of Physics, Berkeley, USA (GRID:grid.47840.3f) (ISNI:0000 0001 2181 7878); Lawrence Berkeley National Laboratory, Materials Science Division, Berkeley, USA (GRID:grid.184769.5) (ISNI:0000 0001 2231 4551)
9 Institute of Metal Research, Chinese Academy of Sciences, Shenyang National Laboratory for Materials Science, Shenyang, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309)