Fully gapped superconducting state in interstitial-carbon-doped Zr5Pt3
T. Shang, J. Philippe, X. Y. Zhu, H. Zhang, B. C. Yu, Z. X. Zhen, H.-R. Ott, J. Kitagawa, T. Shiroka
DOI 10.1103/PhysRevB.106.014507 · Physical Review B
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Abstract
We report a comprehensive study of the Zr5Pt3Cx superconductors, with interstitial carbon between 0 and 0.3. At a macroscopic level, their superconductivity, with Tc ranging from 4.5 to 6.3 K, was investigated via electrical-resistivity, magnetic-susceptibility, and specific-heat measurements. The upper critical fields μ0Hc2∼7 T were determined mostly from measurements of the electrical resistivity in applied magnetic field. The microscopic electronic properties were investigated by means of muon-spin rotation and relaxation (μSR) and nuclear magnetic resonance (NMR) techniques. In the normal state, NMR relaxation data indicate an almost ideal metallic behavior, confirmed by band-structure calculations, which suggest a relatively high electronic density of states at the Fermi level, dominated by the Zr 4d orbitals. The low-temperature superfluid density, obtained via transverse-field μSR, suggests a fully gapped superconducting state in Zr5Pt3 and Zr5Pt3C0.3, with zero-temperature gap Δ0=1.20 and 0.60 meV and magnetic penetration depth λ0 = 333 and 493 nm, respectively. The exponential dependence of the NMR relaxation rates below Tc further supports nodeless superconductivity. The absence of spontaneous magnetic fields below the onset of superconductivity, as determined from zero-field μSR measurements, confirms the preserved time-reversal symmetry in the superconducting state of Zr5Pt3Cx. In contrast to a previous study, our μSR and NMR results suggest conventional superconductivity in the Zr5Pt3Cx family, independent of the C content.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Zr5Pt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 7.2 | Pressure not reported | onset |
| Zr5Pt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.8 | Pressure not reported | midpoint |
| Zr5Pt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.1 | Pressure not reported | zero_resistance |
| Zr5Pt3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.3 | Pressure not reported | onset |
| Zr5Pt3C0.3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.2 | Pressure not reported | onset |
| Zr5Pt3C0.3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.9 | Pressure not reported | midpoint |
| Zr5Pt3C0.3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.4 | Pressure not reported | zero_resistance |
| Zr5Pt3C0.3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.5 | Pressure not reported | onset |
| Zr5Pt3C0.05 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Zr5Pt3C0.15 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Mo5PB2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 9.2 | Pressure not reported | unknown |
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