APS March Meeting 2015 
Volume 60, Number 1
Monday–Friday, March 2–6, 2015;
San Antonio, Texas
Session A7: Focus Session: Magnetism & Topological Insulators
8:00 AM–11:00 AM, 
Monday, March 2, 2015
Room: 006B
Sponsoring
Units: 
DMP DCMP
Chair: Jagadeesh Moodera, Massachusetts Institute of Technology
Abstract ID: BAPS.2015.MAR.A7.1
Abstract: A7.00001 : Realization of high-precision and more robust quantum anomalous Hall state in a hard ferromagnetic topological insulator
8:00 AM–8:36 AM
Preview Abstract
  
Abstract   
Author:
Cui-Zu Chang
(Massachusetts Institute of Technology)
The discovery of the integer quantum Hall (QH)~effect in 1980 led to the 
realization of a topological electronic state with dissipationless currents 
circulating in one direction along the edge of a two dimensional electron 
layer under a strong magnetic field. The quantum 
anomalous Hall (QAH) effect shares a similar physical phenomenon as the QH 
effect, whereas its physical origin is a result of intrinsic spin-orbit 
coupling of the topological insulator (TI) and when it is in ferromagnetic 
state. Since the QAH effect does not require an 
external field and the associated Landau levels, it is believed that this 
effect has unique potential for applications in electronic devices with 
low-power consumption. In this talk, we shall describe the experimental 
observation of the QAH state in V-doped 
(Bi,Sb)$_{2}$Te$_{3}$ TI films. We find that in zero-field 
longitudinal resistance decreases to 0.00013 $\pm$ 0.00007 
$h/e^{2}$ $\sim$ 3.35 $\pm$ 1.76$\Omega )$, Hall 
conductance reaches 0.9998 $\pm$ 0.0006 $e^{2}/h$ and the 
Hall angle becoming as high as 89.993 $\pm$ 0.004$^{\circ}$ at 
$T=$25mK, thus realizing the anomalous Hall transport with negligible 
dissipation in the absence of any initial magnetic field. The advantage of 
this system comes from the fact that it is a hard ferromagnet with a large 
coercive field ($H_{c}$\textgreater 1.0T) and a relative high Curie 
temperature. These results were unexpected from the theoretical 
calculations. This high-precision realization of a more robust QAH state in 
hard FMTIs is a major step towards dissipationless electronic applications 
without external applied fields. 
\\[4pt]
Work done in collaboration with W. Zhao, D. Y. Kim, H. Zhang, B. A. Assaf, D. 
Heiman, S. C. Zhang, C. Liu, M. H. W. Chan, and J. S. Moodera.
\\[4pt]
Supported by funding from NSF (DMR-1207469), NSF (DMR-0907007), ONR 
(N00014-13-1-0301), NSF (DMR-0820404, Penn State MRSEC), and the STC Center 
for Integrated Quantum Materials under~NSF grant DMR-1231319.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.MAR.A7.1