TY - JOUR
T1 - Ambipolar field effect in the ternary topological insulator (BixSb1–x)2Te3 by composition tuning
AU - Kong, Desheng
AU - Chen, Yulin
AU - Cha, Judy J.
AU - Zhang, Qianfan
AU - Analytis, James G.
AU - Lai, Keji
AU - Liu, Zhongkai
AU - Hong, Seung Sae
AU - Koski, Kristie J.
AU - Mo, Sung-Kwan
AU - Hussain, Zahid
AU - Fisher, Ian R.
AU - Shen, Zhi-Xun
AU - Cui, Yi
N1 - KAUST Repository Item: Exported on 2020-10-01
Acknowledged KAUST grant number(s): KUS-l1-001-12, KUS-F1-033-02
Acknowledgements: Y.C. acknowledges support from the Keck Foundation, a DARPA MESO project (no. N66001-11-1-4105) and a King Abdullah University of Science and Technology (KAUST) Investigator Award (no. KUS-l1-001-12). Y.L.C. acknowledges support from a DARPA MESO project (no. N66001-11-1-4105). Z.K.L., Z.X.S., Y.L.C., J.G.A. and I. R. F. acknowledge support from Department of Energy, Office of Basic Energy Science (contract DE-AC02-76SF00515). K. L. acknowledges support from the KAUST Postdoctoral Fellowship (no. KUS-F1-033-02).
This publication acknowledges KAUST support, but has no KAUST affiliated authors.
PY - 2011/10/2
Y1 - 2011/10/2
N2 - Topological insulators exhibit a bulk energy gap and spin-polarized surface states that lead to unique electronic properties 1-9, with potential applications in spintronics and quantum information processing. However, transport measurements have typically been dominated by residual bulk charge carriers originating from crystal defects or environmental doping 10-12, and these mask the contribution of surface carriers to charge transport in these materials. Controlling bulk carriers in current topological insulator materials, such as the binary sesquichalcogenides Bi 2Te 3, Sb 2Te 3 and Bi 2Se 3, has been explored extensively by means of material doping 8,9,11 and electrical gating 13-16, but limited progress has been made to achieve nanostructures with low bulk conductivity for electronic device applications. Here we demonstrate that the ternary sesquichalcogenide (Bi xSb 1-x) 2Te 3 is a tunable topological insulator system. By tuning the ratio of bismuth to antimony, we are able to reduce the bulk carrier density by over two orders of magnitude, while maintaining the topological insulator properties. As a result, we observe a clear ambipolar gating effect in (Bi xSb 1-x) 2Te 3 nanoplate field-effect transistor devices, similar to that observed in graphene field-effect transistor devices 17. The manipulation of carrier type and density in topological insulator nanostructures demonstrated here paves the way for the implementation of topological insulators in nanoelectronics and spintronics. © 2011 Macmillan Publishers Limited. All rights reserved.
AB - Topological insulators exhibit a bulk energy gap and spin-polarized surface states that lead to unique electronic properties 1-9, with potential applications in spintronics and quantum information processing. However, transport measurements have typically been dominated by residual bulk charge carriers originating from crystal defects or environmental doping 10-12, and these mask the contribution of surface carriers to charge transport in these materials. Controlling bulk carriers in current topological insulator materials, such as the binary sesquichalcogenides Bi 2Te 3, Sb 2Te 3 and Bi 2Se 3, has been explored extensively by means of material doping 8,9,11 and electrical gating 13-16, but limited progress has been made to achieve nanostructures with low bulk conductivity for electronic device applications. Here we demonstrate that the ternary sesquichalcogenide (Bi xSb 1-x) 2Te 3 is a tunable topological insulator system. By tuning the ratio of bismuth to antimony, we are able to reduce the bulk carrier density by over two orders of magnitude, while maintaining the topological insulator properties. As a result, we observe a clear ambipolar gating effect in (Bi xSb 1-x) 2Te 3 nanoplate field-effect transistor devices, similar to that observed in graphene field-effect transistor devices 17. The manipulation of carrier type and density in topological insulator nanostructures demonstrated here paves the way for the implementation of topological insulators in nanoelectronics and spintronics. © 2011 Macmillan Publishers Limited. All rights reserved.
UR - http://hdl.handle.net/10754/597497
UR - http://www.nature.com/articles/nnano.2011.172
UR - http://www.scopus.com/inward/record.url?scp=80755132097&partnerID=8YFLogxK
U2 - 10.1038/NNANO.2011.172
DO - 10.1038/NNANO.2011.172
M3 - Article
C2 - 21963714
SN - 1748-3387
VL - 6
SP - 705
EP - 709
JO - Nature Nanotechnology
JF - Nature Nanotechnology
IS - 11
ER -