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Superconducting and electrical properties of amorphous zirconium-transition metal binary alloys
Authors:A Inoue  K Matsuzaki  T Masumoto  H S Chen
Affiliation:(1) The Research Institute for Iron, Steel and Other Metals, Tohoku University, 980 Sendai, Japan;(2) ATT Bell Laboratories, 600 Mountain Avenue, 07974 Murray Hill, New Jersey, USA
Abstract:In order to clarify the compositional effect on the superconductivity of zirconium-transition metal (M) binary amorphous alloys, the superconducting properties and electrical resistance of the alloys were examined as functions of the concentration, group number and periodicity of the M elements.T c for Zr75M25 alloys rises in the order Ru > Rh > Ir > Co > Os > Ni > Pt > Cu > Pd > Fe > Au, i.e. as the group number decreases when the periodicity belongs to the 5th period, and with decreasing M content for Zr100–X M X alloys. The highT c attained in the present work is 4.55 K for Zr80Rh20, 4.38 K for Zr75Rh25 and 4.47 K for Zr75Ru25. The temperature gradient of the upper critical magnetic field (H c2) near the transition temperature (T C) tends to increase with increasing zirconium content, and the resistive state due to the flux flow phenomena appears in a wide sweeping field. Following the sharp and large decrease of the flux flow resistance due to a peak effect, the resistance recovers sharply nearH c2. The peak effect was found to occur more distinctly for the alloys containing a magnetic element of iron or cobalt, probably because of the suppression of the pair-breaking effect due to magnetic scattering by the application of the high field nearH c2. The dominating factor for the compositional effect onT C is inferred to originate from the variation oflambda throughohgr for Zr100–x M X alloys and from that of lambda through N(Ef) for Zr75M25 alloys. Additionally, it has been found for the Zr-M amorphous alloys that the electrical resistivityrgr(T) exhibits a maximum value at temperature ranging from 2T C to 3T C, suggesting that the hump phenomenon in rgr(T) appeared through the generation of the superconducting fluctuations. The temperature coefficient of resistivity (tcr) defined by 1/R250(dR/dT) shows negative values ranging from 1.05×10–4 to 1.75×10–4 K –1 andT C was found to rise through the increase inlambda with the increase in the negative value of the tcr.
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