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Volume-wise destruction of the antiferromagnetic Mott insulating state through quantum tuning.
Frandsen, Benjamin A; Liu, Lian; Cheung, Sky C; Guguchia, Zurab; Khasanov, Rustem; Morenzoni, Elvezio; Munsie, Timothy J S; Hallas, Alannah M; Wilson, Murray N; Cai, Yipeng; Luke, Graeme M; Chen, Bijuan; Li, Wenmin; Jin, Changqing; Ding, Cui; Guo, Shengli; Ning, Fanlong; Ito, Takashi U; Higemoto, Wataru; Billinge, Simon J L; Sakamoto, Shoya; Fujimori, Atsushi; Murakami, Taito; Kageyama, Hiroshi; Alonso, Jose Antonio; Kotliar, Gabriel; Imada, Masatoshi; Uemura, Yasutomo J.
Afiliación
  • Frandsen BA; Department of Physics, Columbia University, New York, New York 10027, USA.
  • Liu L; Department of Physics, Columbia University, New York, New York 10027, USA.
  • Cheung SC; Department of Physics, Columbia University, New York, New York 10027, USA.
  • Guguchia Z; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Khasanov R; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Morenzoni E; Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen, Switzerland.
  • Munsie TJ; Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
  • Hallas AM; Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
  • Wilson MN; Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
  • Cai Y; Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
  • Luke GM; Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada L8S 4M1.
  • Chen B; Canadian Institute for Advanced Research, Toronto, Ontario, Canada L8S 4M1.
  • Li W; Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Jin C; Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Ding C; Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
  • Guo S; Department of Physics, Zhejiang University, Hangzhou 310027, China.
  • Ning F; Department of Physics, Zhejiang University, Hangzhou 310027, China.
  • Ito TU; Department of Physics, Zhejiang University, Hangzhou 310027, China.
  • Higemoto W; Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan.
  • Billinge SJ; Advanced Science Research Center, Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195, Japan.
  • Sakamoto S; Department of Applied Physics and Applied Mathematics, Columbia University, New York, New York 10027, USA.
  • Fujimori A; Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
  • Murakami T; Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan.
  • Kageyama H; Department of Physics, University of Tokyo, Bunkyo-ku, Tokyo 113-0033, Japan.
  • Alonso JA; Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510, Japan.
  • Kotliar G; Department of Energy and Hydrocarbon Chemistry, Graduate School of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510, Japan.
  • Imada M; Instituto de Ciencia de Materiales de Madrid (ICMM), CSIC, Madrid E-28049, Spain.
  • Uemura YJ; Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
Nat Commun ; 7: 12519, 2016 08 17.
Article en En | MEDLINE | ID: mdl-27531192
ABSTRACT
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.

Texto completo: 1 Bases de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2016 Tipo del documento: Article País de afiliación: Estados Unidos

Texto completo: 1 Bases de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2016 Tipo del documento: Article País de afiliación: Estados Unidos