Volume-wise destruction of the antiferromagnetic Mott insulating state through quantum tuning.
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Frandsen BA
Department of Physics, Columbia University, New York, New York 10027, USA.
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Liu L
Department of Physics, Columbia University, New York, New York 10027, USA.
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Cheung SC
Department of Physics, Columbia University, New York, New York 10027, USA.
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Guguchia Z
Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
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Khasanov R
Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
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Morenzoni E
Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
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Munsie TJ
Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
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Hallas AM
Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
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Wilson MN
Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
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Cai Y
Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
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Luke GM
Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
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Chen B
Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
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Li W
Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
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Jin C
Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
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Ding C
Department of Physics, Zhejiang University, Hangzhou 310027, China.
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Guo S
Department of Physics, Zhejiang University, Hangzhou 310027, China.
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Ning F
Department of Physics, Zhejiang University, Hangzhou 310027, China.
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Ito TU
Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan.
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Higemoto W
Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan.
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Billinge SJ
Department of Applied Physics and Applied Mathematics, Columbia University, New York, New York 10027, USA.
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Sakamoto S
Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan.
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Fujimori A
Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan.
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Murakami T
Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510, Japan.
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Kageyama H
Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510, Japan.
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Alonso JA
Instituto de Ciencia de Materiales de Madrid (ICMM), CSIC, Madrid E-28049, Spain.
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Kotliar G
Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
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Imada M
Department of Applied Physics, University of Tokyo, 7-3-1 Hongo, Tokyo 113-8656, Japan.
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Uemura YJ
Department of Physics, Columbia University, New York, New York 10027, USA.
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Published in:
- Nature communications. - 2016
English
RENiO3 (RE=rare-earth element) and V2O3 are archetypal Mott insulator systems. When tuned by chemical substitution (RENiO3) or pressure (V2O3), they exhibit a quantum phase transition (QPT) between an antiferromagnetic Mott insulating state and a paramagnetic metallic state. Because novel physics often appears near a Mott QPT, the details of this transition, such as whether it is first or second order, are important. Here, we demonstrate through muon spin relaxation/rotation (μSR) experiments that the QPT in RENiO3 and V2O3 is first order: the magnetically ordered volume fraction decreases to zero at the QPT, resulting in a broad region of intrinsic phase separation, while the ordered magnetic moment retains its full value until it is suddenly destroyed at the QPT. These findings bring to light a surprising universality of the pressure-driven Mott transition, revealing the importance of phase separation and calling for further investigation into the nature of quantum fluctuations underlying the transition.
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gold
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https://fredi.hepvs.ch/global/documents/25152
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