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A. KebedeCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122C. S. JeeCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122J. SchweglerCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122J. E. CrowCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122T. MihalisinCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122G. H. MyerCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122R. E. SalomonCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122P. SchlottmannCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122M. V. KuricCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122S. H. BloomCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122R. P. GuertinCenter for Materials Research, Temple University, Philadelphia, Pennsylvania 19122
1989lv
ABI

Abstract

An extensive study of magnetic, thermal, transport, and structural properties of the alloy ${\mathrm{Y}}_{1\mathrm{\ensuremath{-}}\mathit{x}}$${\mathrm{Pr}}_{\mathit{x}}$${\mathrm{Ba}}_{2}$${\mathrm{Cu}}_{3}$${\mathrm{O}}_{7\mathrm{\ensuremath{-}}\mathit{y}}$ is presented. The endpoints of the alloy series are a high-temperature superconductor Y-Ba-Cu-O and an antiferromagnetic semiconductor (Pr-Ba-Cu-O, ${T}_{N}$=17 K). The superconducting transition temperature is reduced with increasing Pr concentration following the Abrikosov-Gorkov pair-breaking curve with critical concentration ${x}_{\mathrm{cr}=0.62}$. Alloying also reduces the N\'eel temperature approximately linearly with the Y content, and there is a concentration region (0.4&lt;x&lt;0.6) where antiferromagnetism and superconductivity is suggested to coexist. The specific heat, the susceptibility, the magnetic ordering, and the metal-to-semiconductor transition seen in the resistivity are consistent with the picture that ${\mathrm{Y}}^{3+}$ is replaced by ${\mathrm{Pr}}^{4+}$ with some degree of valence admixture of the ${\mathrm{Pr}}^{3+}$ configuration.

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