Magnetism and superconductivity in (Er0.16Ho0.84)Rh4B4
O. A. Pringle, H. A. Mook, S. E. Lambert, M. B. Maple
DOI 10.1103/PhysRevB.38.8724 · Physical Review B
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Abstract
The superconducting and ferromagnetic phase boundaries in the (Er1−xHox)Rh4B4 mixed ternary alloy system meet in a multicritical point at xcr≊0.9. For x<xcr, the compounds first become superconducting as the temperature is lowered, and then lose superconductivity in a transition to ferromagnetism. The coexistence of superconductivity and ferromagnetism for alloys near the erbium-rich end of the phase diagram is well established. It has also been suggested that ferromagnetism and superconductivity coexist in alloys with x just below xcr. We have carried out neutron-diffraction, ac magnetic susceptibility, and heat-capacity measurements on a sample of (Er0.16Ho0.84)Rh4B4 to investigate the possibility of coexistence of ferromagnetism and superconductivity for x≊xcr. We find that there are minor discrepancies in the superconducting and magnetic transition temperatures reported for different samples of (Er0.16Ho0.84)Rh4B4, but that ferromagnetism and superconductivity do occur simultaneously over a narrow temperature range in this sample. We suggest that an inhomogeneous state occurs, consisting of separate ferromagnetic and superconducting regions, rather than microscopic coexistence.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| (Er0.16Ho0.84)Rh4B4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.95 | Pressure not reported | onset |
| (Er0.16Ho0.84)Rh4B4 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.33 | Pressure not reported | unknown |