AVS 59th Annual International Symposium and Exhibition
    Magnetic Interfaces and Nanostructures Wednesday Sessions
       Session MI-WeM

Paper MI-WeM2
Scanning Tunneling Spectroscopy of Topological Insulators’ Electrically Tunable Electronic Structure

Wednesday, October 31, 2012, 8:20 am, Room 006

Session: Topological Insulators and Rashba
Presenter: J. Ha, Center for Nanoscale Sci. and Tech. / NIST and Seoul National Univ., Korea
Authors: N. Levy, Center for Nanoscale Sci. and Tech. / NIST
T. Zhang, Center for Nanoscale Sci. and Tech. / NIST and Maryland NanoCenter / Univ. of Maryland
J. Ha, Center for Nanoscale Sci. and Tech. / NIST and Seoul National Univ., Korea
Y. Kuk, Seoul National Univ., Republic of Korea
J.A. Stroscio, Center for Nanoscale Sci. and Tech. / NIST
Correspondent: Click to Email

Three-dimensional (3D) topological insulators (TI) are a new state of matter with a bulk band gap but topologically protected gapless surface states. These protected surface states are massless helical Dirac fermions which are predicted to host many striking quantum phenomena [1]. Angle resolved photoemission spectroscopy (ARPES) and scanning tunneling microscopy (STM) measurements confirmed the existence of these surface states and their helical spin structure [1]. All the 3D TI materials to date have an initial doping level which places the Dirac point away from the Fermi level. Initial studies used chemical doping to align the surface states within the bulk band gap. A preferable method to realize the host of new phenomena in TI materials is to electrically tune the carrier density using the field effect from a gate electrode, as demonstrated in three terminal transport experiments [2]. However, the combination of local probe studies with samples containing low defect concentrations and a tunable carrier density remains a challenge, due to the chemical reactivity of the TI surfaces which precludes ex-situ fabrication and processing of the unprotected films.

In this talk we present new results on atomically flat Bi2Se3 and Sb2Te3 films grown on SrTiO3 substrates using Molecular Beam Epitaxy (MBE). SrTiO3 has a very large dielectric constant of ~104 at 4 K [3], allowing tuning of the TI Dirac point and carrier density even with a relatively thick dielectric of 100 μm. The SrTiO3 substrates were pre-patterned with platinum electrodes and mounted in specially designed sample holders, allowing us to in-situ control the carrier density with a back gate on in-situ grown films, avoiding any ex-situ post processing of the samples. As a result, we are able to continuously change the carrier density and observe the local electronic structure of pristine grown TI films. Initial measurements at 5 K are focused on very thin films of 2 to 10 quintuple layers. Scanning tunneling spectroscopy measurements of the thin film’s surface electronic structure allow us to study the gate's efficiency vs. local film thickness in a single sample. We find that the efficiency of gating the top surface state’s electronic structure depends on the film thickness, with a decreasing efficiency for thicker films. In addition, we observe substantial differences in gating between Bi2Se3 and Sb2Te3.We will discuss these results and models of the gating of carriers in the bottom and top surface states through the bulk films at different bulk carrier densities.

[1] Rev. Mod. Phys. 82 3045 (2010)

[2] Nano Lett., 10 (12), 5032 (2010)

[3] Phys. Rev. B 19, 3593–3602 (1979)