Tailoring tricolor structure of magnetic topological insulator for robust axion insulator

Gigantic magnetoresistance is shown in a Cr- and V-doped topological insulator multilayer, assuring robust axion insulator. Exploration of novel electromagnetic phenomena is a subject of great interest in topological quantum materials. One of the unprecedented effects to be experimentally verified is the topological magnetoelectric (TME) effect originating from an unusual coupling of electric and magnetic fields in materials. A magnetic heterostructure of topological insulator (TI) hosts such exotic magnetoelectric coupling and can be expected to realize the TME effect as an axion insulator. We designed a magnetic TI with a tricolor structure where a nonmagnetic layer of (Bi, Sb)2Te3 is sandwiched by a soft ferromagnetic Cr-doped (Bi, Sb)2Te3 and a hard ferromagnetic V-doped (Bi, Sb)2Te3. Accompanied by the quantum anomalous Hall (QAH) effect, we observe zero Hall conductivity plateaus, which are a hallmark of the axion insulator state, in a wide range of magnetic fields between the coercive fields of Cr- and V-doped layers. The resistance of the axion insulator state reaches as high as 109 ohms, leading to a gigantic magnetoresistance ratio exceeding 10,000,000% upon the transition from the QAH state. The tricolor structure of the TI may not only be an ideal arena for the topologically distinct phenomena but can also provide magnetoresistive applications for advancing dissipation-less topological electronics.

[1]  D. Awschalom,et al.  Local optical control of ferromagnetism and chemical potential in a topological insulator , 2017, Proceedings of the National Academy of Sciences.

[2]  Y. Tokura,et al.  A magnetic heterostructure of topological insulators as a candidate for an axion insulator. , 2017, Nature materials.

[3]  Y. Tokura,et al.  Current-Nonlinear Hall Effect and Spin-Orbit Torque Magnetization Switching in a Magnetic Topological Insulator. , 2016, Physical review letters.

[4]  G. V. Astakhov,et al.  Observation of the universal magnetoelectric effect in a 3D topological insulator , 2016, Nature Communications.

[5]  Y. Tokura,et al.  Terahertz spectroscopy on Faraday and Kerr rotations in a quantum anomalous Hall state , 2016, Nature Communications.

[6]  N. P. Armitage,et al.  Quantized Faraday and Kerr rotation and axion electrodynamics of a 3D topological insulator , 2016, Science.

[7]  Y. Tokura,et al.  Magnetic modulation doping in topological insulators toward higher-temperature quantum anomalous Hall effect , 2015, 1511.01724.

[8]  X. Qi,et al.  Quantized topological magnetoelectric effect of the zero-plateau quantum anomalous Hall state , 2015, 1506.03141.

[9]  T. Morimoto,et al.  Topological magnetoelectric effects in thin films of topological insulators , 2015, 1505.06285.

[10]  C. Felser,et al.  Extremely large magnetoresistance and ultrahigh mobility in the topological Weyl semimetal candidate NbP , 2015, Nature Physics.

[11]  Don Heiman,et al.  High-precision realization of robust quantum anomalous Hall state in a hard ferromagnetic topological insulator. , 2014, Nature materials.

[12]  Q. Gibson,et al.  Large, non-saturating magnetoresistance in WTe2 , 2014, Nature.

[13]  Y. Tokura,et al.  Trajectory of the anomalous Hall effect towards the quantized state in a ferromagnetic topological insulator , 2014, Nature Physics.

[14]  Kang L. Wang,et al.  Scale-invariant quantum anomalous Hall effect in magnetic topological insulators beyond the two-dimensional limit. , 2014, Physical review letters.

[15]  Kang L. Wang,et al.  Magnetization switching through giant spin-orbit torque in a magnetically doped topological insulator heterostructure. , 2014, Nature materials.

[16]  Q. Xue,et al.  Experimental Observation of the Quantum Anomalous Hall Effect in a Magnetic Topological Insulator , 2013, Science.

[17]  A. Vishwanath,et al.  Computational design of axion insulators based on 5d spinel compounds. , 2011, Physical review letters.

[18]  Ashvin Vishwanath,et al.  Subject Areas : Strongly Correlated Materials A Viewpoint on : Topological semimetal and Fermi-arc surface states in the electronic structure of pyrochlore iridates , 2011 .

[19]  X. Qi,et al.  Topological insulators and superconductors , 2010, 1008.2026.

[20]  Xiao-Liang Qi,et al.  Topological quantization in units of the fine structure constant. , 2010, Physical review letters.

[21]  Wang-Kong Tse,et al.  Giant magneto-optical Kerr effect and universal Faraday effect in thin-film topological insulators. , 2010, Physical review letters.

[22]  C. Kane,et al.  Topological Insulators , 2019, Electromagnetic Anisotropy and Bianisotropy.

[23]  Wei Zhang,et al.  Quantized Anomalous Hall Effect in Magnetic Topological Insulators , 2010, Science.

[24]  Xi Dai,et al.  Oscillatory crossover from two-dimensional to three-dimensional topological insulators , 2009, 0908.3654.

[25]  Jing Wang,et al.  Dynamical axion field in topological magnetic insulators , 2009, 0908.1537.

[26]  Xi Dai,et al.  Crossover of the three-dimensional topological insulator Bi 2 Se 3 to the two-dimensional limit , 2010 .

[27]  J. Rivera A short review of the magnetoelectric effect and related experimental techniques on single phase (multi-) ferroics , 2009 .

[28]  D. Vanderbilt,et al.  Magnetoelectric polarizability and axion electrodynamics in crystalline insulators. , 2008, Physical review letters.

[29]  Xiao-Liang Qi,et al.  Topological field theory of time-reversal invariant insulators , 2008, 0802.3537.

[30]  M. Fiebig Revival of the magnetoelectric effect , 2005 .

[31]  F. Wilczek,et al.  Two applications of axion electrodynamics. , 1987, Physical review letters.

[32]  R. Peccei,et al.  CP Conservation in the Presence of Pseudoparticles , 1977 .