Quantum Hall effect in a bulk antiferromagnet EuMnBi2 with magnetically confined two-dimensional Dirac fermions.
Quantum Hall effect in a bulk antiferromagnet EuMnBi2 with magnetically confined two-dimensional Dirac fermions.
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DOI:
10.1126/sciadv.1501117
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发表时间:
2016-01
期刊:
影响因子:
13.6
通讯作者:
Ishiwata S
中科院分区:
文献类型:
--
作者:
Masuda H;Sakai H;Tokunaga M;Yamasaki Y;Miyake A;Shiogai J;Nakamura S;Awaji S;Tsukazaki A;Nakao H;Murakami Y;Arima TH;Tokura Y;Ishiwata S
Quantum transport of quasi–two-dimensional Dirac fermions is largely controlled by magnetic order in a layered magnet. For the innovation of spintronic technologies, Dirac materials, in which low-energy excitation is described as relativistic Dirac fermions, are one of the most promising systems because of the fascinating magnetotransport associated with extremely high mobility. To incorporate Dirac fermions into spintronic applications, their quantum transport phenomena are desired to be manipulated to a large extent by magnetic order in a solid. We report a bulk half-integer quantum Hall effect in a layered antiferromagnet EuMnBi2, in which field-controllable Eu magnetic order significantly suppresses the interlayer coupling between the Bi layers with Dirac fermions. In addition to the high mobility of more than 10,000 cm2/V s, Landau level splittings presumably due to the lifting of spin and valley degeneracy are noticeable even in a bulk magnet. These results will pave a route to the engineering of magnetically functionalized Dirac materials.