2019
DOI: 10.1103/physrevlett.123.196604
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Magnetic-Field Control of Topological Electronic Response near Room Temperature in Correlated Kagome Magnets

Abstract: Strongly correlated Kagome magnets are promising candidates for achieving controllable topological devices owing to the rich interplay between inherent Dirac fermions and correlation-driven magnetism. Here we report tunable local magnetism and its intriguing control of topological electronic response near room temperature in the Kagome magnet Fe3Sn2 using small angle neutron scattering, muon spin rotation, and magnetoresistivity measurement techniques. The average bulk spin direction and magnetic domain textur… Show more

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Cited by 28 publications
(17 citation statements)
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“…Thus, materials containing kagome lattices are an exciting platform to explore the quantum level interplay between geometry, correlation, and topology. For instance, certain kagome magnets are found to exhibit electronic nematicity, giant spin-orbit tunability, and topological Chern quantum phases [3][4][5][6][7][8][9][10][11][12][13][14][15][16]. Kagome superconductors with competing orders have been identified for over 40 y [17][18][19], such as LaRu 3 Si 2 with T C of 7 K and a fundamental kagome band structure [20].…”
Section: Introductionmentioning
confidence: 99%
“…Thus, materials containing kagome lattices are an exciting platform to explore the quantum level interplay between geometry, correlation, and topology. For instance, certain kagome magnets are found to exhibit electronic nematicity, giant spin-orbit tunability, and topological Chern quantum phases [3][4][5][6][7][8][9][10][11][12][13][14][15][16]. Kagome superconductors with competing orders have been identified for over 40 y [17][18][19], such as LaRu 3 Si 2 with T C of 7 K and a fundamental kagome band structure [20].…”
Section: Introductionmentioning
confidence: 99%
“…The ratio F/m * is always close to E D /2eℏ, strongly supporting that the main quantum oscillation orbit α in transport is stemming from the Chern-gapped Dirac fermion. This is unlike the case of Fe 3 Sn 2 whose electron mass and gap size can be easily tuned by an external magnetic field 15,26,31 . The strong coupling between 4f and 3d electrons in TbMn 6 Sn 6 , which is absent in other transition-metal-bearing kagome magnets, guarantees a stable out-of-plane ferromagnetic Mn sublattice even in an extremely large external field and temperature range 30 .…”
Section: Resultsmentioning
confidence: 96%
“…The ratio F/m * is always close to E D /2eh, strongly supporting that the main quantum oscillation orbit α in transport is stemming from the Chern-gapped Dirac fermion. This is unlike the case of Fe 3 Sn 2 whose electron mass and gap size can be easily tuned by an external magnetic field 15,26,31 . The strong coupling between 4f and 3d electrons in TbMn 6 Sn 6 , which is absent in other transition-metal-bearing kagome magnets, guarantees a stable out-of-plane ferromagnetic Mn sublattice even in an extremely large external field and temperature range 30 .…”
mentioning
confidence: 96%