Superconductivity in the ferromagnetic phase of polycrystalline HoMo6S8 films
J. Maps, D. D. Berkley, J. H. Kang, A. M. Goldman
DOI 10.1103/PhysRevB.35.38 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
Films of HoMo6S8 have been found to exhibit zero resistance at low temperatures in the ferromagnetic phase. Measurements of the temperature and magnetic field dependences of the electrical resistance, critical field, magnetization, and critical current have been carried out. Zero resistance in the ferromagnetic phase is a consequence of the superconductivity on either domain walls within crystallites or domain walls associated with grain boundaries. In either instance there must be significant supercurrent flow through ferromagnetic material.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| HoMo6S8 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 1.3 | Pressure not reported | midpoint |
| ErRh4B4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Coexistence of ferromagnetism and superconductivity in ErRh4B4 single crystals probed by dynamic magnetic susceptibility
similarity 0.92R. Prozorov et al.
Source status unknown — claims are unverified
Influence of spin-orbit scattering on the coexistence phase of the ferromagnetic superconductors ErRh4B4 and HoMo6S8
similarity 0.90L. N. Bulaevskii et al.
Source status unknown — claims are unverified
Possible Topological Superconducting Phases of MoS2
similarity 0.90Noah F. Q. Yuan et al.
Source status unknown — claims are unverified
Vortex Breaking and Cutting in Type II Superconductors
similarity 0.89A. Palau et al.
Source status unknown — claims are unverified
Normal state charge dynamics of Fe1.06Te0.88S0.14 superconductor probed with infrared spectroscopy
similarity 0.89N. Stojilovic et al.
Source status unknown — claims are unverified
Discrete Superconducting Phases in FeSe-Derived Superconductors
similarity 0.89T. P. Ying et al.
Source status unknown — claims are unverified