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Abstract
Fractional quantum Hall (FQH) states are exotic quantum many-body phases whose elementary charged excitations are anyons obeying fractional braiding statistics. While most FQH states are believed to have Abelian anyons, the Moore–Read type states with even denominators – appearing at half filling of a Landau level (LL) – are predicted to possess non-Abelian excitations with appealing potential in topological quantum computation. These states, however, depend sensitively on the orbital contents of the single-particle LL wavefunctions and the LL mixing. Here we report magnetotransport measurements on Bernal-stacked trilayer graphene, whose multiband structure facilitates interlaced LL mixing, which can be controlled by external magnetic and displacement fields. We observe robust FQH states including even-denominator ones at filling factors ν = − 9/2, − 3/2, 3/2 and 9/2. In addition, we fine-tune the LL mixing and crossings to drive quantum phase transitions of these half-filling states and neighbouring odd-denominator ones, exhibiting related emerging and waning behaviour.
The fractional quantum Hall effect offers a potential platform to harness non-Abelian anyons. Here, the authors report fractional quantum Hall states in trilayer graphene and drive quantum phase transitions between neighbouring states.
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1 Nanjing University, National Laboratory of Solid-State Microstructures, School of Physics, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
2 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309); Hefei National Laboratory, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
3 High Magnetic Field Laboratory of the Chinese Academy of Science, Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, Hefei, China (GRID:grid.467854.c) (ISNI:0000 0004 5902 1885)
4 National Institute for Materials Science, Research Center for Electronic and Optical Materials, Tsukuba, Japan (GRID:grid.21941.3f) (ISNI:0000 0001 0789 6880)
5 National Institute for Materials Science, Research Center for Materials Nanoarchitectonics, Tsukuba, Japan (GRID:grid.21941.3f) (ISNI:0000 0001 0789 6880)
6 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309); Hefei National Laboratory, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639); Songshan Lake Materials Laboratory, Dongguan, China (GRID:grid.511002.7)
7 University of Chinese Academy of Sciences, Kavli Institute of Theoretical Sciences, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419)
8 University of Chinese Academy of Sciences, Kavli Institute of Theoretical Sciences, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419); University of Chinese Academy of Sciences, CAS Center for Excellence in Topological Quantum Computation, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419); Nanjing University, Collaborative Innovation Center of Advanced Microstructures, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)
9 Huazhong University of Science and Technology, School of Physics and Wuhan National High Magnetic Field Center, Wuhan, China (GRID:grid.33199.31) (ISNI:0000 0004 0368 7223)
10 Nanjing University, National Laboratory of Solid-State Microstructures, School of Physics, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X); Nanjing University, Collaborative Innovation Center of Advanced Microstructures, Nanjing, China (GRID:grid.41156.37) (ISNI:0000 0001 2314 964X)