TY - JOUR
T1 - Study of the superconductivity of the 132 K Sb-doped Bi-system oxide superconductor
AU - Yuheng, Zhang
AU - Chenggao, Fan
AU - Guien, Zhou
AU - Li, Yang
AU - Tingzhu, Cheng
AU - Zhiqiang, Mao
PY - 1991
Y1 - 1991
N2 - According to powder X-ray diffraction analyses and electron diffraction for the 132 K Sb-doped Bi-system oxide superconductor it can be found that a new phase exists in this system; the new phase belongs to the monoclinic system with cell dimensions a=22.10 AA, b=5.90 AA, c=19.91 AA and beta =99.6 degrees and is not superconducting itself. Furthermore, there exists intergrowth between the monoclinic phase and 2:2:2:3 (=Bi:Sr:Ca:Cu) phase, and for this reason crystals of the 2:2:2:3 phase are distorted. The superconductivity at 132 K may be caused by the distorted 2:2:2:3 phase. After thermal cycles, this kind of intergrowth phenomenon disappears so that only superconductivity at 110 K occurs as usual. All this can explain why the 132 K phase is not stable. In addition, how and why the measurement current influences Tc is also discussed.
AB - According to powder X-ray diffraction analyses and electron diffraction for the 132 K Sb-doped Bi-system oxide superconductor it can be found that a new phase exists in this system; the new phase belongs to the monoclinic system with cell dimensions a=22.10 AA, b=5.90 AA, c=19.91 AA and beta =99.6 degrees and is not superconducting itself. Furthermore, there exists intergrowth between the monoclinic phase and 2:2:2:3 (=Bi:Sr:Ca:Cu) phase, and for this reason crystals of the 2:2:2:3 phase are distorted. The superconductivity at 132 K may be caused by the distorted 2:2:2:3 phase. After thermal cycles, this kind of intergrowth phenomenon disappears so that only superconductivity at 110 K occurs as usual. All this can explain why the 132 K phase is not stable. In addition, how and why the measurement current influences Tc is also discussed.
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U2 - 10.1088/0953-8984/3/33/020
DO - 10.1088/0953-8984/3/33/020
M3 - Article
AN - SCOPUS:36149035478
SN - 0953-8984
VL - 3
SP - 6433
EP - 6437
JO - Journal of Physics: Condensed Matter
JF - Journal of Physics: Condensed Matter
IS - 33
M1 - 020
ER -