journal article·2019-12-02Open access

Giant Rashba system on a semiconductor substrate with tunable Fermi level: Bi/GaSb(110)–(2×1)

Takuto Nakamura, Yoshiyuki Ohtsubo, Naoki Tokumasu, Patrick Le Fèvre, François Bertran, Shin-ichiro Ideta, Kiyohisa Tanaka, Kenta Kuroda, Koichiro Yaji, Ayumi Harasawa, Shik Shin, Fumio Komori, Shin-ichi Kimura

Physical Review Materials· Volume 3· Issue 12

Abstract

We fabricated spin-polarized surface electronic states with tunable Fermi levels from a semiconductor to low-dimensional metal in the Bi/GaSb(110)-$(2\ifmmode\times\else\texttimes\fi{}1)$ surface using angle-resolved photoelectron spectroscopy (ARPES) and spin-resolved ARPES. The spin-polarized surface band of Bi/GaSb(110) exhibits quasi-one-dimensional character with the Rashba parameter ${\ensuremath{\alpha}}_{\mathrm{R}}$ of 4.1 and 2.6 eV\AA{} at the $\overline{\mathrm{\ensuremath{\Gamma}}}$ and $\overline{\mathrm{Y}}$ points of the surface Brillouin zone, respectively. The Fermi level of the surface electronic state is tuned in situ by element-selective Ar-ion sputtering on the GaSb substrate. The giant Rashba-type spin splitting with switchable metallic/semiconducting character on a semiconductor substrate makes this system a promising candidate for future research in low-dimensional spintronic phenomena.
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Research context

OpenAlex topics: Topological Materials and Phenomena · Advanced Condensed Matter Physics · Electronic and Structural Properties of Oxides

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References (33)

Show source-provided references
1. 10.1103/RevModPhys.82.304510.1103/RevModPhys.82.3045 ↗
2. 10.1038/nmat436010.1038/nmat4360 ↗
3. 10.1038/s41535-018-0100-910.1038/s41535-018-0100-9 ↗
4. 10.1103/PhysRevLett.120.20720710.1103/PhysRevLett.120.207207 ↗
5. E. I. Rashba · Sov. Phys.-Solid State · 1960 · 2 · 1109
6. 10.1103/PhysRevLett.103.04680310.1103/PhysRevLett.103.046803 ↗
7. 10.1038/ncomms101610.1038/ncomms1016 ↗
8. 10.1103/PhysRevB.98.07543110.1103/PhysRevB.98.075431 ↗
9. 10.1103/PhysRevB.75.15540910.1103/PhysRevB.75.155409 ↗
10. 10.1103/PhysRevLett.98.18680710.1103/PhysRevLett.98.186807 ↗
11. 10.1038/nmat305110.1038/nmat3051 ↗
12. 10.1088/1367-2630/16/6/06501610.1088/1367-2630/16/6/065016 ↗
13. 10.1002/adma.20150345910.1002/adma.201503459 ↗
14. 10.1103/PhysRevB.77.08140710.1103/PhysRevB.77.081407 ↗
15. 10.1103/PhysRevB.80.23541910.1103/PhysRevB.80.235419 ↗
16. 10.1088/0953-8984/24/9/09200110.1088/0953-8984/24/9/092001 ↗
17. 10.1038/ncomms307310.1038/ncomms3073 ↗
18. 10.1088/0953-8984/25/4/04500710.1088/0953-8984/25/4/045007 ↗
19. 10.1103/PhysRevB.57.374910.1103/PhysRevB.57.3749 ↗
20. 10.1063/1.494873810.1063/1.4948738 ↗
21. 10.1103/PhysRevB.59.1576010.1103/PhysRevB.59.15760 ↗
22. 10.1103/PhysRevLett.110.03680110.1103/PhysRevLett.110.036801 ↗
23. 10.1103/PhysRevLett.114.06640210.1103/PhysRevLett.114.066402 ↗
24. 10.1142/S0218625X9800141910.1142/S0218625X98001419 ↗
25. 10.1103/PhysRevB.61.268810.1103/PhysRevB.61.2688 ↗
26. 10.1103/RevModPhys.42.31710.1103/RevModPhys.42.317 ↗
27. 10.1088/0953-8984/21/6/06423910.1088/0953-8984/21/6/064239 ↗
28. 10.1103/PhysRevB.90.23542210.1103/PhysRevB.90.235422 ↗
29. 10.1002/sia.584710.1002/sia.5847 ↗
30. 10.1103/PhysRevLett.45.65610.1103/PhysRevLett.45.656 ↗
31. 10.1016/0039-6028(95)00327-410.1016/0039-6028(95)00327-4 ↗
32. 10.1016/S0039-6028(97)00456-110.1016/S0039-6028(97)00456-1 ↗
33. 10.1103/PhysRevB.52.1408610.1103/PhysRevB.52.14086 ↗