TY - JOUR
T1 - Substitution of vanadium for copper in the (Bi, Pb)2Sr2Ca2Cu3O10+σ system
AU - Lu, Y. F.
AU - Wu, X. Z.
AU - Dong, Q. J.
AU - Qiu, X. L.
AU - Zhou, L.
PY - 1994/1/16
Y1 - 1994/1/16
N2 - X‐ray powder diffraction, ac magnetic susceptibility, electrical resistivity measurements, and scanning electron microscopy are used to investigate the effect of V substitution in the Bi1.6Pb0.4Sr2Ca2‐Cu3–xVxOy system for different values of V concentration x (0 ≦ x ≦ 0.5). The addition of V is found to lower the melting point of the system. The samples become multiphasic compounds including the 2223 phase, the 2212 phase, the 2201 phase, and other non‐superconducting phases with increasing x. The lattice parameter c of the 2223 phase decreases from 3.676 to 3.672 nm. There exists an extra step of diamagnetic transition in ac susceptibility curves at lower temperatures (above 77 K) for the samples, which is mainly caused by weak links consisting of non‐superconducting phases and higher‐angle boundaries between the superconducting grains. The transition temperature of the 2223 phase monotonously decreases by 3.4 K with the substitution of V for Cu. The suppression of Tc may be related to a decrease of the hole concentration, which can be caused by Cu vacancies in the CuO2 planes.
AB - X‐ray powder diffraction, ac magnetic susceptibility, electrical resistivity measurements, and scanning electron microscopy are used to investigate the effect of V substitution in the Bi1.6Pb0.4Sr2Ca2‐Cu3–xVxOy system for different values of V concentration x (0 ≦ x ≦ 0.5). The addition of V is found to lower the melting point of the system. The samples become multiphasic compounds including the 2223 phase, the 2212 phase, the 2201 phase, and other non‐superconducting phases with increasing x. The lattice parameter c of the 2223 phase decreases from 3.676 to 3.672 nm. There exists an extra step of diamagnetic transition in ac susceptibility curves at lower temperatures (above 77 K) for the samples, which is mainly caused by weak links consisting of non‐superconducting phases and higher‐angle boundaries between the superconducting grains. The transition temperature of the 2223 phase monotonously decreases by 3.4 K with the substitution of V for Cu. The suppression of Tc may be related to a decrease of the hole concentration, which can be caused by Cu vacancies in the CuO2 planes.
UR - http://www.scopus.com/inward/record.url?scp=10944264035&partnerID=8YFLogxK
U2 - 10.1002/pssa.2211410117
DO - 10.1002/pssa.2211410117
M3 - 文章
AN - SCOPUS:10944264035
SN - 0031-8965
VL - 141
SP - 175
EP - 182
JO - Physica Status Solidi (A) Applied Research
JF - Physica Status Solidi (A) Applied Research
IS - 1
ER -