Measurements of critical magnetic fields and resistance for a phase Mo-Re

https://doi.org/10.1016/0022-5088(80)90293-3Get rights and content

Abstract

Measurements of the critical magnetic fields and the electrical resistance for σ phase alloys of the Mo1−xReitx (0.55 ⩽ x ⩽ 0.7) system are reported. The variation of Tc lies within 0.5 K for various compositions and heat treatments. The extrapolated upper critical magnetic fields Hc2(0) are between 22.6 and 36.0 kG. A splat-quenched alloy of composition Mo-62at.%Re has an Hc2(0) value of 27.1 kG. Thus atomic disorder does not influence Hc2(0) significantly. The Hc2(0) values agree in general with the calculated Hc2∗∗(0) values where paramagnetic effects have been included. The resistance ratio varies as T3 in the low temperature region, then has a negative curvature (50 – 150K) and the curve is less than linear in T at temperatures above 150 K. This behaviour is similar to that of many other d and f band superconductors and can be explained by a modified s-d model.

References (14)

  • K. Maki

    Physics

    (1964)
  • H.R. Khan et al.

    Phys. Status Solidi B

    (1976)
    H.R. Khan et al.

    Phys. Status Solidi B

    (1977)
    H.R. Khan et al.

    Appl. Phys.

    (1977)
    H.R. Khan et al.

    Appl. Phys.

    (1978)
    H.R. Khan et al.

    Appl. Phys.

    (1979)
  • R.D. Blaugher et al.

    IBM J. Res. Dev.

    (1962)
  • E. Bucher et al.

    Phys. Kondens. Mater.

    (1964)
  • C.C. Koch et al.

    Phys. Rev., Sect. B

    (1971)
  • L.R. Testardi et al.

    Solid State Commun.

    (1971)
  • J.R. Gavaler et al.
There are more references available in the full text version of this article.

Cited by (11)

  • Magnetic irreversibility and pinning force density in the Mo<inf>100-x</inf>Re<inf>x</inf> alloy superconductors

    2015, Physica C: Superconductivity and its Applications
    Citation Excerpt :

    Narrow isothermal M(H)-hysteresis curves similar to the present alloys have been observed both in the polycrystalline [15] and single crystal MgB2 samples [16]. In these materials, the narrow width of the hysteresis, is thought to be arising due to weak pinning [15] and the lack of defects (flux line pinning centers) [16]. In such a case, the M− curve lies close to the equilibrium magnetization (MEq) and thus exhibits negative values.

  • Superconductivity in the Nb-Ru-Ge σ phase

    2017, Physical Review Materials
View all citing articles on Scopus
View full text