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Abstract
Pressure-induced magnetic phase transitions are attracting interest as a means to detect superconducting behaviour at high pressures in diamond anvil cells, but determining the local magnetic properties of samples is a challenge due to the small volumes of sample chambers. Optically detected magnetic resonance of nitrogen vacancy centres in diamond has recently been used for the in situ detection of pressure-induced phase transitions. However, owing to their four orientation axes and temperature-dependent zero-field splitting, interpreting these optically detected magnetic resonance spectra remains challenging. Here we study the optical and spin properties of implanted silicon vacancy defects in 4H-silicon carbide that exhibit single-axis and temperature-independent zero-field splitting. Using this technique, we observe the magnetic phase transition of Nd2Fe14B at about 7 GPa and map the critical temperature–pressure phase diagram of the superconductor YBa2Cu3O6.6. These results highlight the potential of silicon vacancy-based quantum sensors for in situ magnetic detection at high pressures.
Optically detected magnetic resonance of nitrogen vacancy centres in diamond enables the detection of pressure-induced phase transitions, but interpreting their magnetic resonance spectra remains challenging. Here the authors propose implanted silicon vacancy defects in 4H-SiC for in situ magnetic phase detection at high pressures.
Details
; Li, Qiang 4 ; Cui, Jin-Ming 5 ; Zhou, Di-Fan 6 ; Zhou, Ji-Yang 4 ; Wei, Yu 7 ; Xu, Hai-An 3 ; Xu, Wan 3 ; Lin, Wu-Xi 5 ; Yan, Jin-Wei 3 ; He, Zhen-Xuan 4 ; Liu, Zheng-Hao 4
; Hao, Zhi-He 4 ; Li, Hai-Ou 5
; Liu, Wen 7 ; Xu, Jin-Shi 5
; Gregoryanz, Eugene 8
; Li, Chuan-Feng 5
; Guo, Guang-Can 5 1 University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639); Sichuan University, College of Physics, Chengdu, China (GRID:grid.13291.38) (ISNI:0000 0001 0807 1581)
2 University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639); Chinese Academy of Sciences, Key Laboratory of Materials Physics, Institute of Solid State Physics, HFIPS, Hefei, China (GRID:grid.9227.e) (ISNI:0000000119573309)
3 Chinese Academy of Sciences, Key Laboratory of Materials Physics, Institute of Solid State Physics, HFIPS, Hefei, China (GRID:grid.9227.e) (ISNI:0000000119573309)
4 University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639); University of Science and Technology of China, CAS Center for Excellence in Quantum Information and Quantum Physics, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
5 University of Science and Technology of China, CAS Key Laboratory of Quantum Information, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639); University of Science and Technology of China, CAS Center for Excellence in Quantum Information and Quantum Physics, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639); University of Science and Technology of China, Hefei National Laboratory, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
6 Shanghai University, Physics Department, Shanghai Key Laboratory of High Temperature Superconductors, Shanghai, China (GRID:grid.39436.3b) (ISNI:0000 0001 2323 5732)
7 University of Science and Technology of China, Center for Micro- and Nanoscale Research and Fabrication, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
8 Chinese Academy of Sciences, Key Laboratory of Materials Physics, Institute of Solid State Physics, HFIPS, Hefei, China (GRID:grid.9227.e) (ISNI:0000000119573309); University of Edinburgh, Centre for Science at Extreme Conditions and School of Physics and Astronomy, Edinburgh, UK (GRID:grid.4305.2) (ISNI:0000 0004 1936 7988); Center for High Pressure Science and Technology Advanced Research (HPSTAR), Shanghai, China (GRID:grid.410733.2)





