TY - JOUR
T1 - Multiple Bi2Sr2-xBaxCuOy microstructures and the effect of element doping (Ba,La,Pb) on the 2:2:0:1 phase
AU - Zhiqiang, Mao
AU - Chenggao, Fan
AU - Lei, Shi
AU - Zhen, Yao
AU - Li, Yang
AU - Yu, Wang
AU - Yuheng, Zhang
PY - 1993
Y1 - 1993
N2 - The microstructure of Bi2Sr2-xBaxCuOy (0≤x≤0.5) was characterized by transmission-electron microscopy and x-ray diffraction. Electron-diffraction analyses reveal that in the Bi-Sr-Cu-O system there also exists a c=12.5 insulating phase with commensurate superstructure with the exception of the c=24 2:2:0:1 phase. However, with the partial substitution of Ba for Sr in this material, the c∼24 2:2:0:1 single phase is obtained, but Ba intercalation reduces the wavelength of modulation of the 2:2:0:1 phase along the b and c directions. Measurement of the superconductivity of the Bi2Sr2-xBaxCuOy samples shows that the appropriate substitution of Ba for Sr (x≤0.2) can raise the Tc of the 2:2:0:1 phase. Tc reaches 20 K for the x=0.2 sample, however, with excessive Ba substitution (x0.2) the metal-to-insulator transition for the 2:2:0:1 phase occurs and the superconductivity of the 2:2:0:1 phase disappears as x exceeds 0.3. In addition, the influence of La and Pb doping on the modulation structure of the 2:2:0:1 phase is also investigated in this article. We discuss the modulation structures of the three substituted systems and the origin of the incommensurate-modulation structure of the Bi-Sr-Cu-O system.
AB - The microstructure of Bi2Sr2-xBaxCuOy (0≤x≤0.5) was characterized by transmission-electron microscopy and x-ray diffraction. Electron-diffraction analyses reveal that in the Bi-Sr-Cu-O system there also exists a c=12.5 insulating phase with commensurate superstructure with the exception of the c=24 2:2:0:1 phase. However, with the partial substitution of Ba for Sr in this material, the c∼24 2:2:0:1 single phase is obtained, but Ba intercalation reduces the wavelength of modulation of the 2:2:0:1 phase along the b and c directions. Measurement of the superconductivity of the Bi2Sr2-xBaxCuOy samples shows that the appropriate substitution of Ba for Sr (x≤0.2) can raise the Tc of the 2:2:0:1 phase. Tc reaches 20 K for the x=0.2 sample, however, with excessive Ba substitution (x0.2) the metal-to-insulator transition for the 2:2:0:1 phase occurs and the superconductivity of the 2:2:0:1 phase disappears as x exceeds 0.3. In addition, the influence of La and Pb doping on the modulation structure of the 2:2:0:1 phase is also investigated in this article. We discuss the modulation structures of the three substituted systems and the origin of the incommensurate-modulation structure of the Bi-Sr-Cu-O system.
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U2 - 10.1103/PhysRevB.47.14467
DO - 10.1103/PhysRevB.47.14467
M3 - Article
AN - SCOPUS:0000886232
SN - 2469-9950
VL - 47
SP - 14467
EP - 14475
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 21
ER -