TY - JOUR
T1 - Flux patterns of monofilamentary Bi2Sr2Ca2Cu3O10+δ tapes at various temperatures
AU - Koblischka, M. R.
AU - Johansen, T. H.
AU - Bratsberg, H.
AU - Vase, P.
PY - 1999/3/1
Y1 - 1999/3/1
N2 - By means of magneto-optic imaging, flux patterns of monofilamentary, silver-sheathed Bi2Sr2Ca2Cu3O10+δ (Bi-2223) tapes are obtained at various temperatures between 12 K and 77 K. Above 50 K, the flux distributions are found to be nearly homogeneous, implying a uniform current flow. On decreasing the temperature, the observed flux patterns develop indications of granularity. This effect is most pronounced at the lowest temperature investigated. From these observations we can deduce the temperature dependence of the transport current density, jtrans, and of the current density of the grains, jgrain. We show that the appearance of granularity in the flux patterns at low temperatures can be explained by assuming a very steep temperature dependence of the intragranular current density, being large at low T and decreasing rapidly with increasing T until at about 50 K, jgrain ≈ jtrans. The absence of granularity above 50 K shows that the current flow is here dominated by the transport currents.
AB - By means of magneto-optic imaging, flux patterns of monofilamentary, silver-sheathed Bi2Sr2Ca2Cu3O10+δ (Bi-2223) tapes are obtained at various temperatures between 12 K and 77 K. Above 50 K, the flux distributions are found to be nearly homogeneous, implying a uniform current flow. On decreasing the temperature, the observed flux patterns develop indications of granularity. This effect is most pronounced at the lowest temperature investigated. From these observations we can deduce the temperature dependence of the transport current density, jtrans, and of the current density of the grains, jgrain. We show that the appearance of granularity in the flux patterns at low temperatures can be explained by assuming a very steep temperature dependence of the intragranular current density, being large at low T and decreasing rapidly with increasing T until at about 50 K, jgrain ≈ jtrans. The absence of granularity above 50 K shows that the current flow is here dominated by the transport currents.
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U2 - 10.1088/0953-2048/12/3/002
DO - 10.1088/0953-2048/12/3/002
M3 - Article
AN - SCOPUS:0032649279
SN - 0953-2048
VL - 12
SP - 113
EP - 119
JO - Superconductor Science and Technology
JF - Superconductor Science and Technology
IS - 3
ER -