TY - JOUR
T1 - Superconductivity in (N H3)y N axFeS e0.5 T e0.5
AU - Zheng, Lu
AU - Sakai, Yusuke
AU - Miao, Xiao
AU - Nishiyama, Saki
AU - Terao, Takahiro
AU - Eguchi, Ritsuko
AU - Goto, Hidenori
AU - Kubozono, Yoshihiro
N1 - Funding Information:
The authors thank Professor Yoshihiro Iwasa of the University of Tokyo for kindly permitting us to use the XRD equipment in his laboratory. This study was partly supported by a grant-in-aid (Grants No. 22244045, No. 24654305, and No. 26105004) from Ministry of Education, Culture, Sports, Science, and Technology (MEXT), Japan, the LEMSUPER project (JST-EU Superconductor Project), the JST-ACTC project of the Japan Science and Technology Agency (JST), and the MEXT Program for Promoting the Enhancement of Research Universities. Furthermore, this study was supported by the JSPS Program for Advancing Strategic International Networks to Accelerate the Circulation of Talented Researchers.
Publisher Copyright:
© 2016 American Physical Society.
PY - 2016
Y1 - 2016
N2 - Na-intercalated FeSe0.5Te0.5 was prepared using the liquid NH3 technique, and a superconducting phase exhibiting a superconducting transition temperature (Tc) as high as 27 K was discovered. This can be called the high-Tc phase since a 21 K superconducting phase was previously obtained in (NH3)yNaxFeSe0.5Te0.5. The chemical composition of the high-Tc phase was determined to be (NH3)0.61(4)Na0.63(5)Fe0.85Se0.55(3)Te0.44(2). The x-ray diffraction patterns of both phases show that a larger lattice constant c (i.e., FeSe0.5Te0.5 plane spacing) produces a higher Tc. This behavior is the same as that of metal-doped FeSe, suggesting that improved Fermi-surface nesting produces the higher Tc. The high-Tc phase converted to the low-Tc phase within several days, indicating that it is a metastable phase. The temperature dependence of resistance for both phases was recorded at different magnetic fields, and the critical fields were determined for both phases. Finally, the Tc versus c phase diagram was prepared for the metal-doped FeSe0.5Te0.5, which is similar to that of metal-doped FeSe, although the Tc is lower.
AB - Na-intercalated FeSe0.5Te0.5 was prepared using the liquid NH3 technique, and a superconducting phase exhibiting a superconducting transition temperature (Tc) as high as 27 K was discovered. This can be called the high-Tc phase since a 21 K superconducting phase was previously obtained in (NH3)yNaxFeSe0.5Te0.5. The chemical composition of the high-Tc phase was determined to be (NH3)0.61(4)Na0.63(5)Fe0.85Se0.55(3)Te0.44(2). The x-ray diffraction patterns of both phases show that a larger lattice constant c (i.e., FeSe0.5Te0.5 plane spacing) produces a higher Tc. This behavior is the same as that of metal-doped FeSe, suggesting that improved Fermi-surface nesting produces the higher Tc. The high-Tc phase converted to the low-Tc phase within several days, indicating that it is a metastable phase. The temperature dependence of resistance for both phases was recorded at different magnetic fields, and the critical fields were determined for both phases. Finally, the Tc versus c phase diagram was prepared for the metal-doped FeSe0.5Te0.5, which is similar to that of metal-doped FeSe, although the Tc is lower.
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U2 - 10.1103/PhysRevB.94.174505
DO - 10.1103/PhysRevB.94.174505
M3 - Article
AN - SCOPUS:84995478992
SN - 2469-9950
VL - 94
JO - Physical Review B
JF - Physical Review B
IS - 17
M1 - 174505
ER -