2015
DOI: 10.1007/s10948-015-3238-8
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Field-dependent Behavior of AC Susceptibility in [Y 0.8 Ca 0.2](Ba 0.5 Sr 0.5)2 Cu 3 O 7−δ

Abstract: The AC susceptibility of [Y 0.8 Ca 0.2 ](Ba 0.5 Sr 0.5 ) 2 Cu 3 O 7−δ was investigated as a function of frequency and amplitude of AC magnetic field. The susceptibilities of the sample display the field amplitude dependence. The peak temperature (T p ) of its imaginary part shows not frequency dependence but field amplitude dependence. The frequency effect on AC susceptibility was negligible. As the field amplitude increases, T p shifts to lower temperature.

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Cited by 2 publications
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“…The pinning losses are strongly dependent on amplitude of applied AC field, while flux losses depend on frequency of applied magnetic field [28]. In this case, AC susceptibility strongly depends on amplitude and and not on frequency, therefore one can say that in Nb 2 PdS 5 sample mostly the pinning losses occursand the granular coupling is rather strong [28,29]. To be brave enough one can conjecture that Nb 2 PdS 5 is a well coupled heavily pinned superconductor.…”
Section: Resultsmentioning
confidence: 99%
“…The pinning losses are strongly dependent on amplitude of applied AC field, while flux losses depend on frequency of applied magnetic field [28]. In this case, AC susceptibility strongly depends on amplitude and and not on frequency, therefore one can say that in Nb 2 PdS 5 sample mostly the pinning losses occursand the granular coupling is rather strong [28,29]. To be brave enough one can conjecture that Nb 2 PdS 5 is a well coupled heavily pinned superconductor.…”
Section: Resultsmentioning
confidence: 99%