APS March Meeting 2015
Volume 60, Number 1
Monday–Friday, March 2–6, 2015;
San Antonio, Texas
Session G7: Focus Session: Novel Topological Materials
11:15 AM–2:15 PM,
Tuesday, March 3, 2015
Room: 006B
Sponsoring
Units:
DMP DCMP
Chair: Yong Chen, Purdue University
Abstract ID: BAPS.2015.MAR.G7.4
Abstract: G7.00004 : Quantum Anomalous Hall Effect in Magnetic Semiconductors
11:51 AM–12:27 PM
Preview Abstract
Abstract
Author:
Chaoxing Liu
(The Department of Physics, Pennsylvania State University)
In the quantum anomalous Hall effect, dissipationless charge currents are
carried by chiral edge states and the Hall conductance is quantized, similar
to the quantum Hall effect. Different from the conventional quantum Hall
effect that requires strong magnetic fields, the quantum anomalous Hall
effect is induced by strong exchange coupling between electron spin and
magnetic moments in magnetic materials, so it can be realized at zero
magnetic field, enabling the potential application of electronic devices
with low energy consumption. Recent experiments on Cr or V doped BiSbTe thin
films has observed the quantized Hall conductance at zero magnetic field and
confirmed this novel effect.
In this talk, I would like to discuss our recent work on the quantum
anomalous Hall effect in magnetic semiconductors. I will first introduce two
key ingredients, inverted band structures and ferromagnetic insulators, for
the quantum anomalous Hall effect in realistic magnetic materials. Then,
based on these two ingredients, I will discuss different classes of
materials for the quantum anomalous Hall effect, focusing on magnetically
doped InAs/GaSb quantum wells and magnetically doped LaOSbSe2 films. For
magnetically doped InAs/GaSb quantum wells, we will show how band edge
singularity can enhance spin susceptibility and lead to the quantum
anomalous Hall state at a relatively high critical temperature. For
magnetically doped LaOSbSe2 films, we find the quantum anomalous Hall effect
can be tuned electrically by a gate voltage and identify layer dependent
spin texture as the underlying physical reason. Finally, we will also
discuss disordered transport and anisotropic magnetoresistance in the
quantum anomalous Hall regime.\\[4pt]
[1] Quantum Anomalous Hall Effect in Hg$_{\mathrm{1-y}}$Mn$_{\mathrm{y}}$Te
Quantum Wells, Chao-Xing Liu, Xiao-Liang Qi, Xi Dai, Zhong Fang, Shou-Cheng
Zhang, Phys. Rev. Lett. 101, 146802 (2008). \\[0pt]
[2] In-plane Magnetization Induced Quantum Anomalous Hall Effect, Xin Liu,
Hsiu-Chuan Hsu, Chao-Xing Liu, Phys. Rev. Lett. 111, 086802 (2013). \\[0pt]
[3] Quantum Anomalous Hall Effect in Magnetically Doped InAs/GaSb Quantum
Wells, Qingze Wang, Xin Liu, Hai-Jun Zhang, Nitin Samarth, Shou-Cheng Zhang,
Chao-Xing Liu, Phys. Rev. Lett. 113, 147201 (2014). \\[0pt]
[4] Electrically tunable multiple Dirac cones in thin films of
(LaO)$_{2}$(SbSe$_{2})_{2}$ family of
materials, Xiao-Yu Dong, Jian-Feng Wang, Rui-Xing Zhang, Wen-Hui Duan,
Bang-Fen Zhu, Jorge Sofo and Chao-Xing Liu, arXiv:cond-mat/1409.3641 (2014).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.MAR.G7.4