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Nature Communications|July 8, 2015
Giant anisotropic magnetoresistance in a quantum anomalous Hall insulatorAbhinav Kandala, Anthony Richardella, Susan Kempinger, et al.Nano Letters|May 7, 2013
Surface-sensitive two-dimensional magneto-fingerprint in mesoscopic Bi2Se3 channelsAbhinav Kandala, Anthony Richardella, Duming Zhang, et al.Nature|July 28, 2006
Atom-by-atom substitution of Mn in GaAs and visualization of their hole-mediated interactionsDale Kitchen, Anthony Richardella, Jian-Ming Tang, et al.Science Advances|November 25, 2015
Persistent optical gating of a topological insulatorAndrew L Yeats, Yu Pan, Anthony Richardella, et al.Science (New York, N.Y.)|February 6, 2010
Visualizing critical correlations near the metal-insulator transition in Ga(1-x)Mn(x)AsAnthony Richardella, Pedram Roushan, Shawn Mack, et al.Proceedings of the National Academy of Sciences of the United States of America|September 14, 2017
Local optical control of ferromagnetism and chemical potential in a topological insulatorAndrew L Yeats, Peter J Mintun, Yu Pan, et al.ACS Applied Nano Materials|May 13, 2026
In Situ Composition and Thickness Monitoring during (Bi<sub>x</sub>In<sub>1‑x</sub>)<sub>2</sub>Se<sub>3</sub> Thin Film Growth: toward Automated Synthesis Control Using Spectroscopic Ellipsometry for Quantum and Spintronic DevicesMaria Hilse, Jackson Niedel, Qihua Zhang, et al.Physical Review Letters|August 27, 2016
Surface-State-Dominated Spin-Charge Current Conversion in Topological-Insulator-Ferromagnetic-Insulator HeterostructuresHailong Wang, James Kally, Joon Sue Lee, et al.Nature|August 12, 2009
Topological surface states protected from backscattering by chiral spin texturePedram Roushan, Jungpil Seo, Colin V Parker, et al.Scientific Reports|August 11, 2017
Proximity-effect-induced Superconducting Gap in Topological Surface States - A Point Contact Spectroscopy Study of NbSe<sub>2</sub>/Bi<sub>2</sub>Se<sub>3</sub> Superconductor-Topological Insulator HeterostructuresWenqing Dai, Anthony Richardella, Renzhong Du, et al.Pageof 2