Effect of Y3+ substitution for Ca on the superconducting and the normal state properties of Bi(2223) system (Bi1.7Pb0.3Ca2-xYxSr2Cu3Oy)

K. Nanda Kishore; S. Satyavathi; M. Muralidhar; O. Pena; V. Hari Babu

doi:10.1016/0921-4534(94)91985-2

Effect of Y³⁺ substitution for Ca on the superconducting and the normal state properties of Bi(2223) system (Bi_1.7Pb_0.3Ca_2-xY_xSr₂Cu₃O_y)

K. Nanda Kishore, S. Satyavathi, M. Muralidhar, O. Pena, V. Hari Babu

Research output: Contribution to journal › Article › peer-review

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Abstract

The superconducting properties of the Bi_1.7Pb_0.3Ca_2-xY_xSr₂Cu₃O_y system have been investigated by X-ray diffraction, SEM, DC electrical resistivity, AC susceptibility and Thermo Electric Power measurements. With increasing Y concentration the volume fraction of the high T_c (2223) phase decreased and that of the low T_c (2212) phase increased and also T_c (0)'s and T_c(onset)'s have decreased. The AC susceptibility measurements have shown the granular nature of the superconductivity. The thermoelectric power measurements have shown that the charge carrier concentration decreases with increasing Y concentration.

Original language	English
Pages (from-to)	1521-1522
Number of pages	2
Journal	Physica C: Superconductivity and its applications
Volume	235-240
Issue number	PART 2
DOIs	https://doi.org/10.1016/0921-4534(94)91985-2
Publication status	Published - 1994 Dec
Externally published	Yes

ASJC Scopus subject areas

Electronic, Optical and Magnetic Materials
Condensed Matter Physics
Energy Engineering and Power Technology
Electrical and Electronic Engineering

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10.1016/0921-4534(94)91985-2

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Effect of Y³⁺ substitution for Ca on the superconducting and the normal state properties of Bi(2223) system (Bi_1.7Pb_0.3Ca_2-xY_xSr₂Cu₃O_y). / Nanda Kishore, K.; Satyavathi, S.; Muralidhar, M.; Pena, O.; Hari Babu, V.

In: Physica C: Superconductivity and its applications, Vol. 235-240, No. PART 2, 12.1994, p. 1521-1522.

Research output: Contribution to journal › Article › peer-review

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abstract = "The superconducting properties of the Bi1.7Pb0.3Ca2-xYxSr2Cu3Oy system have been investigated by X-ray diffraction, SEM, DC electrical resistivity, AC susceptibility and Thermo Electric Power measurements. With increasing Y concentration the volume fraction of the high Tc (2223) phase decreased and that of the low Tc (2212) phase increased and also Tc (0)'s and Tc(onset)'s have decreased. The AC susceptibility measurements have shown the granular nature of the superconductivity. The thermoelectric power measurements have shown that the charge carrier concentration decreases with increasing Y concentration.",

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AU - Satyavathi, S.

AU - Muralidhar, M.

AU - Pena, O.

AU - Hari Babu, V.

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N2 - The superconducting properties of the Bi1.7Pb0.3Ca2-xYxSr2Cu3Oy system have been investigated by X-ray diffraction, SEM, DC electrical resistivity, AC susceptibility and Thermo Electric Power measurements. With increasing Y concentration the volume fraction of the high Tc (2223) phase decreased and that of the low Tc (2212) phase increased and also Tc (0)'s and Tc(onset)'s have decreased. The AC susceptibility measurements have shown the granular nature of the superconductivity. The thermoelectric power measurements have shown that the charge carrier concentration decreases with increasing Y concentration.

AB - The superconducting properties of the Bi1.7Pb0.3Ca2-xYxSr2Cu3Oy system have been investigated by X-ray diffraction, SEM, DC electrical resistivity, AC susceptibility and Thermo Electric Power measurements. With increasing Y concentration the volume fraction of the high Tc (2223) phase decreased and that of the low Tc (2212) phase increased and also Tc (0)'s and Tc(onset)'s have decreased. The AC susceptibility measurements have shown the granular nature of the superconductivity. The thermoelectric power measurements have shown that the charge carrier concentration decreases with increasing Y concentration.

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Effect of Y³⁺ substitution for Ca on the superconducting and the normal state properties of Bi(2223) system (Bi_1.7Pb_0.3Ca_2-xY_xSr₂Cu₃O_y)

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