Abstract

The temperature T dependence of the upper critical magnetic field ${\mathit{H}}_{\mathit{c}2}$ of the heavy-electron superconductors ${\mathrm{U}}_{1\mathrm{\ensuremath{-}}\mathit{x}}$${\mathrm{Th}}_{\mathit{x}}$${\mathrm{Be}}_{13}$ (x=0 and 2.9%) doped with various concentrations of Gd has been determined from low-frequency ac magnetic susceptibility measurements in magnetic fields up to 60 kOe. The ${\mathit{H}}_{\mathit{c}2}$(T) curves for ${\mathrm{U}}_{1\mathrm{\ensuremath{-}}\mathit{x}}$${\mathrm{Gd}}_{\mathit{x}}$${\mathrm{Be}}_{13}$ samples deviate from the ${\mathit{H}}_{\mathit{c}2}$(T) curves of ${\mathrm{UBe}}_{13}$ near ${\mathit{T}}_{\mathit{c}}$, which is consistant with the depairing of superconducting electrons via the Zeeman interaction between the spins of the superconducting electrons and the exchange field associated with the Gd spins. This suggests that ${\mathrm{UBe}}_{13}$ exhibits singlet superconductivity. In contrast, the ${\mathit{H}}_{\mathit{c}2}$(T) curves for (${\mathrm{U}}_{0.97}$${\mathrm{Th}}_{0.03}$)${\mathrm{Be}}_{13}$ doped with Gd scale with ${\mathit{H}}_{\mathit{c}2}$(T) of pure (${\mathrm{U}}_{0.97}$${\mathrm{Th}}_{0.03}$)${\mathrm{Be}}_{13}$ and do not reflect superconducting depairing by the Gd ions. These results are consistent with either strong spin-orbit scattering due to the presence of Th in ${\mathrm{UBe}}_{13}$, or to a qualitatively different type of superconductivity involving triplet spin pairing in (${\mathrm{U}}_{0.97}$${\mathrm{Th}}_{0.03}$)${\mathrm{Be}}_{13}$. Measurements of the temperature dependence of ${\mathit{H}}_{\mathit{c}2}$ for ${\mathrm{U}}_{1\mathrm{\ensuremath{-}}\mathit{x}}$${\mathit{R}}_{\mathit{x}}$${\mathrm{Be}}_{13}$ compounds where R=La, Lu, and Ce for various compositions x as well as ${\mathrm{U}}_{0.985}$${\mathit{R}}_{0.015}$${\mathrm{Be}}_{13}$ compounds for R=Tb, Dy, Ho, and Er are also presented and compared with the Gd-doped ${\mathrm{UBe}}_{13}$ system. The results of low-temperature specific-heat measurements of ${\mathrm{UBe}}_{13}$ doped with various concentrations of Gd are also discussed.

Highlights

  • The upper critical magnetic field H, 2(T) of the heavyelectron superconductor UBe&3 (T, 8 1 K) is characterized by several peculiarities

  • The temperature T dependence of the upper critical magnetic field H, 2 of the heavy-electron superconductors U& Th Be» (x=0 and 2.9%) doped with various concentrations of Gd has been determined from low-frequency ac magnetic susceptibility measurements in magnetic fields up to 60

  • The arc-melted polycrystalline samples used in this investigation were prepared in a manner described previously. ' The upper critical magnetic field H, 2(T) was g„, determined from the ac magnetic susceptibility measured on bulk specimens by means of a standard mutual inductance technique at a frequency of 16 Hz in a He-He dilution refrigerator

Read more

Summary

JANUARY 1991

Upper(xc=rit0icaalndm2ag.9n%eti)c field doped of the heavy-electron superconductors Ui with paramagnetic Gd and other rare-earth. The temperature T dependence of the upper critical magnetic field H, 2 of the heavy-electron superconductors U& Th Be» (x=0 and 2.9%) doped with various concentrations of Gd has been determined from low-frequency ac magnetic susceptibility measurements in magnetic fields up to 60. KOe. The H, 2(T) curves for U, „Gd Be» samples deviate from the H, 2(T) curves of UBe» near T„which is consistant with the depairing of superconducting electrons via the Zeeman interaction between the spins of the superconducting electrons and the exchange field associated with the Gd spins. The H, 2(T) curves for (Uo»Tho o3)Be» doped with Gd scale with H„(T) of pure (Uo»Tho O3)Be» and do not reflect superconducting depairing by the Gd ions These results are consistent with either strong spin-orbit scattering due to the presence of Th in UBe», or to a qualitatively diferent type of superconductivity involving triplet spin pairing in (Uo 9pThp 03)Be». The results of low-temperature specific-heat measurements of UBe» doped with various concentrations of Gd are discussed

INTRODUCTION
RESULTS
CONCLUSIONS
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.