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the Youth Innovation Promotion Association of the Chinese Academy of Sciences(Grant,No.,2015187)
the National Natural Science Foundation of China(Grant,Nos.,11204338,11574338,51572165)
the “Strategic Priority Research Program(B)
National Key R&D Program(Grant,No.,2016YFF0101701)
and the Science and Technology Commission of Shanghai Municipality(Grant,Nos.,16521108400,16DZ0504300,14521102800)
This work was supported by the Youth Innovation Promotion Association of the Chinese Academy of Sciences (Grant No. 2015187), the National Natural Science Foundation of China (Grant Nos. 11204338, 11574338, and 51572165), the “Strategic Priority Research Program (B)” of the Chinese Academy of Sciences (Grant No. XDB04040300), the National Key R&D Program (Grant No. 2016YFF0101701), and the Science and Technology Commission of Shanghai Municipality (Grant Nos. 16521108400, 16DZ0504300, and 14521102800).
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Figure 1
(Color online) (a) Schematic of the crystal structure of BaFe2S3. (b) Powder X-ray diffraction patterns for two samples under quenching and annealing treatments. The powdered samples were obtained by crushing the crystals. (c) An enlarged view of the PXRD patterns near (350) peak.
Figure 2
(Color online) (a) Temperature dependence of the magnetic susceptibility
Figure 3
(Color online) (a) Temperature dependence of the normalized resistivity for the quenched and annealed samples. (b)-(d) Plot with log(
(1) | (2) | (3) | (4) | |
Sample | Lattice constant | Neel temperature | FM component | Resistivity behavior |
Quenched | small | low | high | 2D VRH |
Annealed | large | high | low | 1D VRH |
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