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論文

Magnetic-impurity-induced modifications to ultrafast carrier dynamics in the ferromagnetic topological insulators Sb$$_{2-x}$$V$$_{x}$$Te$$_{3}$$

角田 一樹*; 鹿子木 将明*; Reimann, J.*; Nurmamat, M.*; 後藤 伸一*; 竹田 幸治; 斎藤 祐児; Kokh, K. A.*; Tereshchenko, O. E.*; G$"u$dde, J.*; et al.

New Journal of Physics (Internet), 21(9), p.093006_1 - 093006_8, 2019/09

 被引用回数:1 パーセンタイル:65.14(Physics, Multidisciplinary)

We systematically investigate the magnetic, structural and electronic properties and the ultrafast carrier dynamics in a series of V-doped Sb$$_{2}$$Te$$_{3}$$ samples of composition Sb$$_{2-x}$$V$$_{x}$$Te$$_{3}$$ with x = 0, 0.015 and 0.03. Element specific X-ray magnetic circular dichroism signifies that the ferromagnetism of V-doped Sb$$_{2}$$Te$$_{3}$$ is governed by the p-d hybridization between the host carrier and the magnetic dopant. Time- and angle-resolved photoemission spectroscopy has revealed that the V impurity induced states underlying the topological surface state (TSS) add scattering channels that significantly shorten the duration of transient surface electrons down to 100 fs scale. This is in a sharp contrast to the prolonged duration reported for pristine samples though the TSS is located inside the bulk energy gap of the host in either magnetic or non-magnetic cases. It implies the presence of a mobility gap in the bulk energy gap region of the host material.

論文

Dirac gap opening and Dirac-fermion-mediated magnetic coupling in antiferromagnetic Gd-doped topological insulators and their manipulation by synchrotron radiation

Shikin, A. M.*; Estyunin, D. A.*; Surnin, Yu. I.*; Koroleva, A. V.*; Shevchenko, E. V.*; Kokh, K. A.*; Tereshchenko, O. E.*; Kumar, S.*; Schwier, E. F.*; 島田 賢也*; et al.

Scientific Reports (Internet), 9(1), p.4813_1 - 4813_17, 2019/03

 被引用回数:6 パーセンタイル:26.52(Multidisciplinary Sciences)

A new kind of magnetically-doped antiferromagnetic (AFM) topological insulators (TIs), Bi$$_{1.09}$$Gd$$_{0.06}$$Sb$$_{0.85}$$Te$$_{3}$$, has been studied by angle-resolved photoemission, superconducting magnetometry (SQUID) and X-ray magnetic circular dichroism (XMCD). It has been shown that this TI is characterized by the Dirac gap at the Fermi level. In the paramagnetic phase, a surface magnetic layer is supposed to develop, where the coupling between the Gd magnetic moments is mediated by the topological surface states (TSSs). This assumption can be confirmed by opening a gap at the Dirac point indicated by the surface-sensitive ARPES, a weak hysteresis loop measured by SQUID, the XMCD showing a surface magnetic moment and the temperature dependence of electrical resistance demonstrating a mid-gap semiconducting behavior, which correlates with the temperature dependence of the surface magnetization and confirms the conclusion that only TSSs are located at the Fermi level.

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