TY - JOUR
T1 - Critical-state model with a secondary high-field peak
AU - Johansen, T.
AU - Koblischka, M.
AU - Bratsberg, H.
AU - Hetland, P.
PY - 1997
Y1 - 1997
N2 - A critical-state model capable of describing the experimentally observed secondary or fishtail peak in magnetization data for bulk high-(Formula presented) superconductors is introduced. As suggested by a recent understanding of the fishtail effect, the field dependence of the critical current density is taken as a sum of two terms; one giving rise to a low-field magnetization peak and another being responsible for the fishtail peak. The model, which extends the Kim model by adding a Lorentzian term in (Formula presented) allows analytical treatment. Expressions for internal flux-density profiles as well as the various branches of the magnetization loop are presented. It is shown that measured magnetization loops of (Formula presented) samples showing a very pronounced fishtail peak are well fitted by this model. Using our procedure, (Formula presented) can be determined without invoking the Bean model (with a constant (Formula presented)), and thus avoiding an inconsistency in the analysis.
AB - A critical-state model capable of describing the experimentally observed secondary or fishtail peak in magnetization data for bulk high-(Formula presented) superconductors is introduced. As suggested by a recent understanding of the fishtail effect, the field dependence of the critical current density is taken as a sum of two terms; one giving rise to a low-field magnetization peak and another being responsible for the fishtail peak. The model, which extends the Kim model by adding a Lorentzian term in (Formula presented) allows analytical treatment. Expressions for internal flux-density profiles as well as the various branches of the magnetization loop are presented. It is shown that measured magnetization loops of (Formula presented) samples showing a very pronounced fishtail peak are well fitted by this model. Using our procedure, (Formula presented) can be determined without invoking the Bean model (with a constant (Formula presented)), and thus avoiding an inconsistency in the analysis.
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U2 - 10.1103/PhysRevB.56.11273
DO - 10.1103/PhysRevB.56.11273
M3 - Article
AN - SCOPUS:0000123525
SN - 0163-1829
VL - 56
SP - 11273
EP - 11278
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 17
ER -