Upper critical field, critical current density and thermally activated flux flow in CaFFe0.9Co0.1As superconductor

Details Upper critical field, critical current density and thermally activated flux flow in CaFFe0.9Co0.1As superconductor Upper critical field, critical current density and thermally activated flux flow in CaFFe0.9Co0.1As superconductor

2012-02-07

arxiv.org/abs/1202.1473v2

Supercond. Sci. Technol. 25 (2012) 045004

Physics

Condensed Matter

Superconductivity

10 pages, 10 figures, to be published in Supercond. Sci. Technol

Scientific paper

10.1088/0953-2048/25/4/045004

In this paper, we report the synthesis, structure, transition temperature, upper critical field, critical current density and thermally activated flux flow in CaFFe0.9Co0.1As superconductor. Superconductivity arises at 23 K by Co substitution at the site of Fe atoms and upper critical field is estimated 102 T by using the Werthamer-Helfand-Hohenberg formula. The flux-flow activation energy (U0/kB) varies from 3230 K and 4190 K in the field of 1 T and 9 T respectively. At 2K, the Jc is found to be approximately 4x10^3A/cm^2 and 0.3x10^3 A/cm&^2 in zero and 6T field, respectively. Transmission electron microscopy analysis shows an amorphous region surrounding around most of the grains which is likely to be present in the form of amorphous and weak link grain boundaries in this compound. It seems that most of the current is hindered by miss aligned grains, amorphous grain boundaries and impurities, which are invariably found between the grains. Presence of the weakly linked granules and their weakly pinned intergranular Josephson vortices are responsible for both low Jc and the Arrhenius temperature dependence of resistivity

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