Vortex phase diagram and transition in (Bi1.6Pb0.4Sr2Ca2Cu3O10-δ)1-x(SnO2)x superconductors

•Superconductivity of SnO2-added Bi1.6Pb0.4Sr2Ca2Cu3O10+δ ceramics was investigated using resistivity measurements under magnetic fields.•Analysis of excess conductivity using Aslamazov–Larkin and Lawrence–Doniach models revealed optimized c-axis coherence length and interlayer coupling strength.•Th...

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Veröffentlicht in:Results in physics 2024-08, Vol.63, p.107887, Article 107887
Hauptverfasser: Pham, An T., Le, Tien, Thi Anh Hong, Vuong, Lee, Hanoh, Park, T., Duy Thien, Nguyen, Thi Kim Anh, Do, Hoang Nam, Nguyen, Thanh Binh, Nguyen, Man, Nguyen K., Ngoc Thao, Pham, Hop, Dang T.B., Miyanaga, T., Nghi Pham, Q., Tran, Duc H.
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Sprache:eng
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Zusammenfassung:•Superconductivity of SnO2-added Bi1.6Pb0.4Sr2Ca2Cu3O10+δ ceramics was investigated using resistivity measurements under magnetic fields.•Analysis of excess conductivity using Aslamazov–Larkin and Lawrence–Doniach models revealed optimized c-axis coherence length and interlayer coupling strength.•The activation energy (U0) and upper critical field (Bc2) were significantly enhanced for the x  = 0.002 sample, indicating improved flux pinning properties.•Vortex phase (B-T) diagrams showed extended pinning regimes for the x  = 0.002 sample, highlighting superior flux pinning characteristics. The superconducting vortex phase diagram of (Bi1.6Pb0.4Sr2Ca2Cu3O10-δ)1-x(SnO2)x ceramics, where x  = 0, 0.002, 0.004, 0.006, 0.008, and 0.010, was investigated using resistivity measurement under magnetic fields. If the value of the offset critical temperature (Tc,offset) monotonously decreased on the SnO2-added samples, then the mean-field critical temperature (Tmf) would slightly improve on the x  = 0.002 sample. The excess conductivity of all samples was analyzed based on the Aslamazov–Larkin and Lawrence–Doniach models. The c-axis coherence length at 0 K (ξc(0)) and the interlayer coupling strength were optimized on the x  = 0.002 sample. The activation energy (U0) calculated using the Arrhenius model was also increased, and the maximum for the x  = 0.002 sample was reached. The upper critical field (Bc2) deduced using the Werthamer–Helfand–Hohenberg model was also enhanced for the x  = 0.002 sample. The small bundle field (Bsb), large bundle field (Blb), irreversibility field (Birr), and Bc2 were combined for the vortex phase (B-T) diagram of the x  = 0.000 and x  = 0.002 samples. All pinning regimes of the x  = 0.002 sample were extended, clearly revealing the improvements in the flux pinning properties in that sample.
ISSN:2211-3797
2211-3797
DOI:10.1016/j.rinp.2024.107887