AC susceptibility and electrical properties of rare-earth- and alkali metal-substituted (Tl0.7M0.3)Sr2CaCu2O7 with M = Er, Gd, La, Na, K and Rb

The effects of rare-earth elements M = Er, Gd and La, and alkali metals M = Na, K and Rb substitution on (Tl 0.7 M 0.3 )Sr 2 CaCu 2 O 7 (Tl-1212) are reported. The rare-earth elements were chosen by considering the ionic radius, i.e., from the smallest (Er +3 ) to the largest (La +3 ) ion. The sampl...

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Veröffentlicht in:Applied physics. A, Materials science & processing Materials science & processing, 2019, Vol.125 (1), p.1-7, Article 21
Hauptverfasser: Bakar, Ilhamsyah Putra Abu, Muhammad-Aizat, K., Nur-Akasyah, J., Mohd-Syahmi, M. S., Mohd Suib, Nurul Raihan, Chiu, W. S., Abd-Shukor, R.
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Sprache:eng
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Zusammenfassung:The effects of rare-earth elements M = Er, Gd and La, and alkali metals M = Na, K and Rb substitution on (Tl 0.7 M 0.3 )Sr 2 CaCu 2 O 7 (Tl-1212) are reported. The rare-earth elements were chosen by considering the ionic radius, i.e., from the smallest (Er +3 ) to the largest (La +3 ) ion. The samples were prepared via the solid-state reaction method. X-ray diffraction patterns showed the presence of major Tl-1212 and minor Tl-1201 and Ca 0.3 Sr 0.7 CuO 2 phase in almost all samples. The resistance versus temperature curves for the rare-earth-substituted samples showed onset temperature between 87 and 90 K and zero resistance temperature between 69 and 81 K. Alkali metal substitutions exhibited Tl-1212 phase but showed no superconducting transition although the electrical resistivity was much lower than the rare-earth-substituted samples. AC susceptibility measurement showed superconducting transition T cχ , between 59 and 80 K for the rare-earth element-substituted samples. The average grain size, the transition temperature, T cχ and the peak temperature T p of the imaginary part of the susceptibility χ″ decreased as the ionic radius of the rare earths was reduced.
ISSN:0947-8396
1432-0630
DOI:10.1007/s00339-018-2316-8