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Abstract
The interplay between magnetism and electronic band topology enriches topological phases and has promising applications. However, the role of topology in magnetic fluctuations has been elusive. Here, we report evidence for topology stabilized magnetism above the magnetic transition temperature in magnetic Weyl semimetal candidate CeAlGe. Electrical transport, thermal transport, resonant elastic X-ray scattering, and dilatometry consistently indicate the presence of locally correlated magnetism within a narrow temperature window well above the thermodynamic magnetic transition temperature. The wavevector of this short-range order is consistent with the nesting condition of topological Weyl nodes, suggesting that it arises from the interaction between magnetic fluctuations and the emergent Weyl fermions. Effective field theory shows that this topology stabilized order is wavevector dependent and can be stabilized when the interband Weyl fermion scattering is dominant. Our work highlights the role of electronic band topology in stabilizing magnetic order even in the classically disordered regime.
Recently, rich condensed matter physics has emerged from the interplay between band topology and magnetic order. Here, the authors characterize the magnetic Weyl semimetal CeAlGe and find evidence for the role of Weyl fermions in stabilizing the magnetic order above the local transition temperature.
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1 MIT, Quantum Measurement Group, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786); Harvard University, John A. Paulson School of Engineering and Applied Sciences, Cambridge, USA (GRID:grid.38142.3c) (ISNI:0000 0004 1936 754X)
2 MIT, Quantum Measurement Group, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786); MIT, Department of Nuclear Science and Engineering, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
3 MIT, Quantum Measurement Group, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786); MIT, Department of Physics, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
4 University of Shanghai for Science and Technology, College of Science, Shanghai, China (GRID:grid.267139.8) (ISNI:0000 0000 9188 055X)
5 Argonne National Laboratory, Lemont, USA (GRID:grid.187073.a) (ISNI:0000 0001 1939 4845)
6 Hunan Normal University, School of Physics and Electronics, Changsha, China (GRID:grid.411427.5) (ISNI:0000 0001 0089 3695)
7 MIT, Department of Nuclear Science and Engineering, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
8 MIT, Department of Physics, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
9 SLAC National Accelerator Laboratory, Menlo Park, USA (GRID:grid.445003.6) (ISNI:0000 0001 0725 7771)
10 Oak Ridge National Laboratory, Neutron Scattering Division, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)
11 Brookhaven National Laboratory, National Synchrotron Light Source II, Upton, USA (GRID:grid.202665.5) (ISNI:0000 0001 2188 4229)
12 Argonne National Laboratory, Advanced Photon Source, Lemont, USA (GRID:grid.187073.a) (ISNI:0000 0001 1939 4845)
13 Quantum Design, Inc., San Diego, USA (GRID:grid.456047.4) (ISNI:0000 0004 6050 194X)
14 Oak Ridge National Laboratory, Center for Nanophase Materials Sciences, Oak Ridge, USA (GRID:grid.135519.a) (ISNI:0000 0004 0446 2659)
15 Rice University, Department of Electrical Engineering, Houston, USA (GRID:grid.21940.3e) (ISNI:0000 0004 1936 8278)
16 Fudan University, Department of Physics and State Key Laboratory of Surface Physics, Shanghai, China (GRID:grid.8547.e) (ISNI:0000 0001 0125 2443)