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Xiaoxiang Xi,1,2,3,* Xiangyan Bo,1,2 X. S. Xu,4 P. P. Kong,5 Z. Liu,6 X. G. Hong,7,8 C. Q. Jin,5 G. Cao,9 Xiangang Wan,1,2,† and G. L. Carr3 1National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China 2Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China 3Photon Sciences, Brookhaven National Laboratory, Upton, New York 11973, USA 4Department of Physics and Astronomy, University of Nebraska, Lincoln, Nebraska 68588, USA 5Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China 6Institute of Materials Science and Department of Civil and Environmental Engineering, The George Washington University, Washington D.C. 20052, USA 7Mineral Physics Institute, Stony Brook University, Stony Brook, New York 11794, USA 8Center for High Pressure Science and Technology Advanced Research, Beijing 100094, China 9Department of Physics, University of Colorado at Boulder, Boulder, Colorado 80309, USA

physical review. b./physical review. b

Honeycomb lattice <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi>Na</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>IrO</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math> at high pressures: A robust spin-orbit Mott insulator

Honeycomb lattice Na2IrO3 at high pressures: A robust spin-orbit Mott insulator