4.3 Article

Normal and Superconducting Properties of Bi1.7Pb0.30Sr2Ca1-xLaxCu2OySuperconductor with 0.00 ≤ x ≤ 0.30

Journal

JOURNAL OF SUPERCONDUCTIVITY AND NOVEL MAGNETISM
Volume 33, Issue 11, Pages 3349-3359

Publisher

SPRINGER
DOI: 10.1007/s10948-020-05587-y

Keywords

2212 phase; Resistivity; Hardness; DTA and surface energy

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We report here normal and superconducting properties of Bi(1.7)Pb(0.30)Sr(2)Ca(1-x)La(x)Cu(2)O(y)superconductor with variousxvalues (0.00 <= x <= 0.30). It is found that the replacement of Ca(2+)by La(3+)does not influence the phase purity of the samples, while the orthorhombic distortion, excess oxygen, effective Cu valance, and hole carriers/Cu ions are affected. Further, the doping distance and crystal geometry factor are decreased by La, but the distance between neighboring Cu atoms and the density of excess doping are increased. Furthermore, the DTA graphs show strong endothermic peaks at a temperature of 844.1, 848.03, 850.10, and 857.41 degrees C for pure and La-doped samples, respectively. The thermogravimetric analysis diagrams displayed a sharp mass loss started at about 800 degrees C and extended up to 1000 degrees C for all samples. Although the critical temperatureT(c)of the samples is decreased by La from 94 K to 83, 63, and 51 K, the critical concentration for quenching superconductivity can be extended above 0.30. Moreover, an inverse linear relation betweenT(m)andT(c), given byT(c)(K) = - 2.544T(m)(degrees C) + 2272.1, is also estimated. On the other hand, the Vickers hardnessH(v)is increased by La up to 0.30 (H-v alpha T-m,H-v alpha (1/T-c)), but it is decreased by the applied loadF. TheH(v)-Fcharacters are divided according to the applied load into two parts: the first at lower loads (0.00-1.962 N) and the second at higher loads (2.942-4.904 N). It is noted that the surface energy, elastic indentation, and resistance pressure are increased by La, but their values at higher loads are generally more than that of lower loads. Our results are discussed in terms of the balance between the hole carriers lost by La(3+)with that introduced by excess oxygen in the Cu-O(2)planes, which alters the quenching of superconductivity by La(3+)and highlights the present work.

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