TY - JOUR
T1 - Microstructures in high‐Tc Bi(Pb)‐family 2212 superconductors as revealed by scanning and transmission electron microscopy
AU - Horiuchi, Shigeo
AU - Hirasaka, Masao
AU - Tsutsumi, Masayuki
AU - Kosuda, Kosuke
AU - Szerer, M. Y.
AU - Ben‐Dor, Lina
PY - 1995/2/15
Y1 - 1995/2/15
N2 - Microstructures of Bi(Pb)‐family 2212 superconductors, which were prepared by a sol‐gel method with three different compositions, were examined mainly by scanning and transmission electron microscopy. The magnetization of the specimens strongly depends on the ratio between Bi and Pb content, while Tc is almost constant. In specimen 1, prepared with the nominal composition of Bi/Pb = 9/1, small grains of 2212 phase are formed with a minor fraction of some impurity phases. In specimen 2, with Bi/Pb = 17/3, which is optimum from the viewpoint of magnetization, large grains of the 2212 phase are formed during heating at 800°C, also with the impurity phases. In specimen 3, with Bi/Pb = 8/2, the 2212 grains are divided by layers of (Bi0.86, Pb0.14) (Ca0.7, Sr0.3)Ox. Moreover, plate‐like 2212 crystals are severely bent so that small cracks appear often with an inclusion of amorphous substance being rich in Ca and Pb. These layers and cracks must degrade the magnetization. A modulated structure of Bi‐type is formed in the 2212 grains of specimens 1 and 2, while not only Bi‐type but also Pb‐type are formed in specimen 3. The wavelength of Bi‐type is different for each specimen. © 1995 Wiley‐Liss, Inc.
AB - Microstructures of Bi(Pb)‐family 2212 superconductors, which were prepared by a sol‐gel method with three different compositions, were examined mainly by scanning and transmission electron microscopy. The magnetization of the specimens strongly depends on the ratio between Bi and Pb content, while Tc is almost constant. In specimen 1, prepared with the nominal composition of Bi/Pb = 9/1, small grains of 2212 phase are formed with a minor fraction of some impurity phases. In specimen 2, with Bi/Pb = 17/3, which is optimum from the viewpoint of magnetization, large grains of the 2212 phase are formed during heating at 800°C, also with the impurity phases. In specimen 3, with Bi/Pb = 8/2, the 2212 grains are divided by layers of (Bi0.86, Pb0.14) (Ca0.7, Sr0.3)Ox. Moreover, plate‐like 2212 crystals are severely bent so that small cracks appear often with an inclusion of amorphous substance being rich in Ca and Pb. These layers and cracks must degrade the magnetization. A modulated structure of Bi‐type is formed in the 2212 grains of specimens 1 and 2, while not only Bi‐type but also Pb‐type are formed in specimen 3. The wavelength of Bi‐type is different for each specimen. © 1995 Wiley‐Liss, Inc.
KW - Amorphous substance
KW - Crack
KW - EPMA
KW - High‐Tc Bi(Pb)‐2212 superconductor
KW - Magnetization
KW - Microstructure
KW - Modulated structure
KW - Powder XRD
KW - SEM
KW - Sol‐gel method
KW - TEM
UR - http://www.scopus.com/inward/record.url?scp=0028950979&partnerID=8YFLogxK
U2 - 10.1002/jemt.1070300307
DO - 10.1002/jemt.1070300307
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C2 - 7718919
AN - SCOPUS:0028950979
SN - 1059-910X
VL - 30
SP - 258
EP - 264
JO - Microscopy Research and Technique
JF - Microscopy Research and Technique
IS - 3
ER -