Large Gap Topological Insulator Bi2Te3 with a Single Dirac Cone on the Surface
| dc.creator | Chen, Y. L. | |
| dc.creator | Analytis, J. G. | |
| dc.creator | Chu, J. H. | |
| dc.creator | Liu, Z. K. | |
| dc.creator | Mo, S. K. | |
| dc.creator | Qi, X. L. | |
| dc.creator | Zhang, H. J. | |
| dc.creator | Lu, D. H. | |
| dc.creator | Dai, X. | |
| dc.creator | Fang, Z. | |
| dc.creator | Zhang, S. C. | |
| dc.creator | Fisher, I. R. | |
| dc.creator | Hussain, Z. | |
| dc.creator | Shen, Z. X. | |
| dc.date | 2009-04-12 | |
| dc.date.accessioned | 2026-07-07T13:03:18Z | |
| dc.date.available | 2026-07-07T13:03:18Z | |
| dc.description | We investigate the surface state of Bi$_2$Te$_3$ using angle resolved photoemission spectroscopy (ARPES) and transport measurements. By scanning over the entire Brillouin zone (BZ), we demonstrate that the surface state consists of a single non-degenerate Dirac cone centered at the $Γ$ point. Furthermore, with appropriate hole (Sn) doping to counteract intrinsic n-type doping from vacancy and anti-site defects, the Fermi level can be tuned to intersect only the surface states, indicating a full energy gap for the bulk states, consistent with a carrier sign change near this doping in transport properties. Our experimental results establish for the first time that Bi$_2$Te$_3$ is a three dimensional topological insulator with a single Dirac cone on the surface, as predicted by a recent theory. | |
| dc.description | Submitted for publication on March 03, 2009 | |
| dc.identifier | https://arxiv.org/abs/0904.1829 | |
| dc.identifier | http://arxiv.org/abs/0904.1829 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/226753 | |
| dc.subject | Materials Science | |
| dc.title | Large Gap Topological Insulator Bi2Te3 with a Single Dirac Cone on the Surface | |
| dc.type | text |