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Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles

The major limitations of the Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor are weak flux pinning capability and weak inter-grains coupling that lead to a low critical current density and low critical magnetic field which impedes the suppleness of this material towards practical applications. T...

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Autores principales: Aftabi, Ali, Mozaffari, Morteza
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7900248/
https://www.ncbi.nlm.nih.gov/pubmed/33619318
http://dx.doi.org/10.1038/s41598-021-83218-9
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author Aftabi, Ali
Mozaffari, Morteza
author_facet Aftabi, Ali
Mozaffari, Morteza
author_sort Aftabi, Ali
collection PubMed
description The major limitations of the Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor are weak flux pinning capability and weak inter-grains coupling that lead to a low critical current density and low critical magnetic field which impedes the suppleness of this material towards practical applications. The addition of nanoscales impurities can create artificial pining centers that may improve flux pinning capability and intergranular coupling. In this work, the influences of ZnO nanoparticles on the superconducting parameters and pseudogap properties of the Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor are investigated using fluctuation induced conductivity analyses. Results demonstrate that the ZnO nanoparticles addition improves the formation of the Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) phase significantly. Various superconducting parameters include coherence length along c-axis (ξ(c)(0)), penetration depth (λ(pd)(0)), Fermi velocity (v(F)), Fermi energy (E(F)), lower and upper critical magnetic fields (B(c1)(0) and B(c2)(0) respectively) and critical current density (J(c)(0)), are estimated for samples with different amounts of ZnO nanoparticles. It is found that the values of the B(c1)(0), B(c2)(0), and J(c)(0) are improved significantly in the 0.2 wt% ZnO added sample in comparison to the ZnO-free sample. The magnitude and temperature dependence of the pseudogap Δ*(T) is calculated using the local pairs model. The obtained values of T(pair), the temperature at which local pairs are transformed from strongly coupled bosons into the fluctuating Cooper pairs, increases as the added ZnO nanoparticles concentration enhances up to 0.2 wt%. Also, the estimated values for the superconducting gap at T = 0 K (Δ(0)) are decreased from about 26 meV in ZnO-free sample to about 22 meV in 0.2 wt% ZnO added sample and then increases for higher values of additive.
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spelling pubmed-79002482021-02-24 Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles Aftabi, Ali Mozaffari, Morteza Sci Rep Article The major limitations of the Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor are weak flux pinning capability and weak inter-grains coupling that lead to a low critical current density and low critical magnetic field which impedes the suppleness of this material towards practical applications. The addition of nanoscales impurities can create artificial pining centers that may improve flux pinning capability and intergranular coupling. In this work, the influences of ZnO nanoparticles on the superconducting parameters and pseudogap properties of the Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor are investigated using fluctuation induced conductivity analyses. Results demonstrate that the ZnO nanoparticles addition improves the formation of the Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) phase significantly. Various superconducting parameters include coherence length along c-axis (ξ(c)(0)), penetration depth (λ(pd)(0)), Fermi velocity (v(F)), Fermi energy (E(F)), lower and upper critical magnetic fields (B(c1)(0) and B(c2)(0) respectively) and critical current density (J(c)(0)), are estimated for samples with different amounts of ZnO nanoparticles. It is found that the values of the B(c1)(0), B(c2)(0), and J(c)(0) are improved significantly in the 0.2 wt% ZnO added sample in comparison to the ZnO-free sample. The magnitude and temperature dependence of the pseudogap Δ*(T) is calculated using the local pairs model. The obtained values of T(pair), the temperature at which local pairs are transformed from strongly coupled bosons into the fluctuating Cooper pairs, increases as the added ZnO nanoparticles concentration enhances up to 0.2 wt%. Also, the estimated values for the superconducting gap at T = 0 K (Δ(0)) are decreased from about 26 meV in ZnO-free sample to about 22 meV in 0.2 wt% ZnO added sample and then increases for higher values of additive. Nature Publishing Group UK 2021-02-22 /pmc/articles/PMC7900248/ /pubmed/33619318 http://dx.doi.org/10.1038/s41598-021-83218-9 Text en © The Author(s) 2021 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons licence, and indicate if changes were made. The images or other third party material in this article are included in the article's Creative Commons licence, unless indicated otherwise in a credit line to the material. If material is not included in the article's Creative Commons licence and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Aftabi, Ali
Mozaffari, Morteza
Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles
title Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles
title_full Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles
title_fullStr Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles
title_full_unstemmed Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles
title_short Fluctuation induced conductivity and pseudogap state studies of Bi(1.6)Pb(0.4)Sr(2)Ca(2)Cu(3)O(10+δ) superconductor added with ZnO nanoparticles
title_sort fluctuation induced conductivity and pseudogap state studies of bi(1.6)pb(0.4)sr(2)ca(2)cu(3)o(10+δ) superconductor added with zno nanoparticles
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7900248/
https://www.ncbi.nlm.nih.gov/pubmed/33619318
http://dx.doi.org/10.1038/s41598-021-83218-9
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