Thin Films of Magnetically Doped Topological Insulator with Carrier-Independent Long-Range Ferromagnetic Order
Thin Films of Magnetically Doped Topological Insulator with Carrier-Independent Long-Range Ferromagnetic Order
复制标题
具有载流子无关长程铁磁序的磁掺杂拓扑绝缘体薄膜
DOI:
10.1002/adma.201203493
复制
发表时间:
2013-02-20
影响因子:
29.4
通讯作者:
Xue, Qi-Kun
中科院分区:
文献类型:
--
作者:
Chang, Cui-Zu;Zhang, Jinsong;Xue, Qi-Kun
In recent years, topological insulators (TIs), as a class of new concept quantum materials, have received substantial research interests from not only condensed matter physics but also material science.[1, 2] A TI has its bulk band gapped at Fermi level, the same as usual insulators, but hosts gapless, Diractype, and spin-split surface states at all of its surfaces which are protected by the time reversal symmetry (TRS). The special kind of surface states is expected to exhibit various unique quantum phenomena which may bring revolutionary developments in low power electronics and topological quantum computation.[1, 2] A large portion of the quantum phenomena results from breaking of the TRS of TIs by, say, introducing ferromagnetism in them.[3–6] For example, a thin film of a ferromagnetic TI, no matter three-dimensional (3D) or two-dimensional (2D) one, with perpendicular magnetic anisotropy is predicted to show quantum Hall (QH) effect without needing external magnetic field, very high quality of samples, and even low temperature, because the special QH effect does not depend on the formation of well-defined Landau levels.[3–6] This kind of easy access QH effect, known as quantized anomalous Hall (QAH) effect, has been sought after for decades since its realization would open the possibility of applying the novel QH effect into real devices.[7–10]