Magnetic Susceptibility of Superconductors and Other Spin Systems 1991
DOI: 10.1007/978-1-4899-2379-0_3
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Alternating-Field Susceptometry and Magnetic Susceptibility of Superconductors

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Cited by 113 publications
(98 citation statements)
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References 153 publications
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“…According to the single-phase description, both the 2212 and the 2223 phase should contribute with a highly superconducting grain component and with a poorly superconducting matrix component, but in the investigated temperature range both the 2212 phase components are in the normal non-diamagnetic state. On the other hand, as far as the 2223 phase is concerned, it has been shown for systems similar to ours [29,30] that at about the applied ®eld of H 200 A/m the superconductivity of the 2223 phase matrix component is strongly suppressed at least for T > 90 K. Therefore, in order to apply the two component model to our samples, it is necessary to identify the spherical grains with the 2223 phase highly superconducting grain component, while the embedding medium consists of the 2223 phase poorly superconducting matrix component, both the 2212 phase components (matrix and grains) plus, obviously, the detected impurities and voids. The request for the embedding medium to be non magnetic is full®lled by the fact that these superconducting components are in the normal state.…”
Section: Resultssupporting
confidence: 66%
“…According to the single-phase description, both the 2212 and the 2223 phase should contribute with a highly superconducting grain component and with a poorly superconducting matrix component, but in the investigated temperature range both the 2212 phase components are in the normal non-diamagnetic state. On the other hand, as far as the 2223 phase is concerned, it has been shown for systems similar to ours [29,30] that at about the applied ®eld of H 200 A/m the superconductivity of the 2223 phase matrix component is strongly suppressed at least for T > 90 K. Therefore, in order to apply the two component model to our samples, it is necessary to identify the spherical grains with the 2223 phase highly superconducting grain component, while the embedding medium consists of the 2223 phase poorly superconducting matrix component, both the 2212 phase components (matrix and grains) plus, obviously, the detected impurities and voids. The request for the embedding medium to be non magnetic is full®lled by the fact that these superconducting components are in the normal state.…”
Section: Resultssupporting
confidence: 66%
“…To relate the two geometries we briefly discuss demagnetization effects. 80,81 As a model sample of finite dimensions, we consider an oblate ellipsoid of revolution about the z axis for which the demagnetizing factor is 81…”
Section: B H M and Demagnetization In Oblate Ellipsoids And Fmentioning
confidence: 99%
“…j c (B) is constant (Bean, 1964). Analytical solutions for magnetization loops are known for an infinitely long slab or cylinder in a parallel field (Goldfarb, 1991) and thin disk (Clem & Sanchez, 1994;Mikheenko & Kuzovlev, 1993) or strip (Brandt, 1993) in a perpendicular field. In these cases the 3D partial differential equation (PDE) Eq.…”
Section: Bean Critical Statementioning
confidence: 99%