Magnetic transitions of superconducting thin films and foils. II. Tin
Magnetic transitions of superconducting thin films and foils. II. Tin
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超导薄膜和箔的磁转变。
DOI:
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发表时间:
1968
期刊:
影响因子:
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通讯作者:
G. Cody
中科院分区:
文献类型:
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作者:
R. Miller;G. Cody
The perpendicular and parallel magnetic transitions for pure Pb films and foils have been determined from transverse magnetization and ac susceptibility measurements as a function of thickness (400 AA{} to 35 ensuremath{mu}) and temperature (1.4 to 4.2ifmmode^circelse extdegreefi{}K). The perpendicular critical field (${H}_{ensuremath{perp}}$) for thicknesses less than a critical thickness, ${d}_{c}ensuremath{approx}15$ kAA{}, is in good agreement with the theory of Tinkham if it is assumed that the penetration depth is thickness-dependent. The data for thicknesses above ${d}_{c}$ follow a thickness dependence predicted from the effect of a positive surface energy on the free energy of the intermediate state. At ${d}_{c}$ there is a minimum in ${H}_{ensuremath{perp}}$. The parallel critical field (${H}_{ensuremath{parallel}}$) up to ${d}_{c}$ is in good agreement with the theory of Saint James and de Gennes for a second-order transition. Above ${d}_{c}$, ${H}_{ensuremath{parallel}}$ agrees with the bulk value of ${H}_{c3}$ for lead. In the vicinity of ${d}_{c}$ the magnetization curve starts to exhibit a reversible tail which persists to larger thicknesses and whose slope is in reasonable agreement with theory. From the data, the bulk values of $ensuremath{kappa}(T)$, $ensuremath{lambda}(T)$, ${ensuremath{lambda}}_{L}(0)$, and ${ensuremath{xi}}_{0}$, as well as the thickness dependence of these quantities, have been computed.