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Bulk Upper Critical Field of Clean Type-II Superconductors: V and Nb

S. J. Williamson*

  • Science Center, North American Rockwell Corporation, Thousand Oaks, California 91360

  • *Present address: Department of Physics, University of California, Santa Barbara, Calif. 93106.

Phys. Rev. B 2, 3545 – Published 1 November, 1970

DOI: https://doi.org/10.1103/PhysRevB.2.3545

Abstract

The bulk upper critical field Hc2 of single crystals of Nb and V has been measured for various crystallographic orientations within the temperature range between the respective critical temperature and T0.06 °K. The normalized critical field averaged over all crystallographic directions h(t)=Hc2(t)(dHc2dt)t=1, where t=TTc, and the relative anisotropy of Hc2 for the two metals are found to be similar. The measurements support predictions of the Hohenberg-Werthamer calculation that attributes the observed anisotropy of Hc2 to the effects of an anisotropic Fermi surface. Some differences in the behavior of Hc2(t) for the present samples can be understood qualitatively to arise from the effects of a shorter electron-collision time τ for the less pure V specimen. At very low temperatures, Hc2(0)Hc2(t) for V does not follow a t2ln(t) temperature dependence, previously observed for Nb, but can be characterized by an empirical formula t2ln(t+α) in which the constant α is conjectured to be inversely proportional to τ.

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