Author
Listed:
- Defen Kang
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Yazhou Zhou
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Wei Yi
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Chongli Yang
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Jing Guo
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Youguo Shi
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Shan Zhang
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Zhe Wang
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Chao Zhang
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Sheng Jiang
(Shanghai Synchrotron Radiation Facilities, Shanghai Institute of Applied Physics, Chinese Academy of Sciences)
- Aiguo Li
(Shanghai Synchrotron Radiation Facilities, Shanghai Institute of Applied Physics, Chinese Academy of Sciences)
- Ke Yang
(Shanghai Synchrotron Radiation Facilities, Shanghai Institute of Applied Physics, Chinese Academy of Sciences)
- Qi Wu
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences)
- Guangming Zhang
(State Key Laboratory for Low dimensional Quantum Physics, Tsinghua University
Collaborative Innovation Center of Quantum Matter)
- Liling Sun
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences
Collaborative Innovation Center of Quantum Matter)
- Zhongxian Zhao
(Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, Chinese Academy of Sciences
Collaborative Innovation Center of Quantum Matter)
Abstract
The recent discovery of large magnetoresistance in tungsten ditelluride provides a unique playground to find new phenomena and significant perspective for potential applications. The large magnetoresistance effect originates from a perfect balance of hole and electron carriers, which is sensitive to external pressure. Here we report the suppression of the large magnetoresistance and emergence of superconductivity in pressurized tungsten ditelluride via high-pressure synchrotron X-ray diffraction, electrical resistance, magnetoresistance and alternating current magnetic susceptibility measurements. Upon increasing pressure, the positive large magnetoresistance effect is gradually suppressed and turned off at a critical pressure of 10.5 GPa, where superconductivity accordingly emerges. No structural phase transition is observed under the pressure investigated. In situ high-pressure Hall coefficient measurements at low temperatures demonstrate that elevating pressure decreases the population of hole carriers but increases that of the electron ones. Significantly, at the critical pressure, a sign change of the Hall coefficient is observed.
Suggested Citation
Defen Kang & Yazhou Zhou & Wei Yi & Chongli Yang & Jing Guo & Youguo Shi & Shan Zhang & Zhe Wang & Chao Zhang & Sheng Jiang & Aiguo Li & Ke Yang & Qi Wu & Guangming Zhang & Liling Sun & Zhongxian Zhao, 2015.
"Superconductivity emerging from a suppressed large magnetoresistant state in tungsten ditelluride,"
Nature Communications, Nature, vol. 6(1), pages 1-6, November.
Handle:
RePEc:nat:natcom:v:6:y:2015:i:1:d:10.1038_ncomms8804
DOI: 10.1038/ncomms8804
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