Superconducting and structural properties of the noncentrosymmetric Re6Hf superconductor under high pressure
Sathiskumar Mariappan, Manikandan Krishnan, Dilip Bhoi, Hanming Ma, Jun Gouchi, Kapil Motla, R. P. Singh, Ponniah Vajeeston, Arumugam Sonachalam, Yoshiya Uwatoko
DOI 10.1103/PhysRevB.105.224505 · Physical Review B
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Abstract
We report the effect of high pressure on the superconducting, vortex pinning, and structural properties of a polycrystalline, noncentrosymmetric superconductor Re6Hf. The superconducting transition temperature,Tc, reveals a modest decrease as pressure (P) increases with a slope of −0.046 K/GPa (−0.065 K/GPa) estimated from resistivity measurements up to 8 GPa (magnetization measurement ∼1.1 GPa). Structural analysis up to ∼18 GPa reveals monotonic decreases of lattice constant without undergoing any structural transition and a high value of bulk modulus B0≈333.63 GPa, indicating the stability of the structure. Furthermore, the upper critical field and lower critical field at absolute temperature [Hc2(0) and Hc1(0)] decrease slightly from the ambient pressure value as pressure increases up to 2.5 GPa. In addition, analysis of ρ(T,H) up to P∼ 2.5 GPa using thermally activated flux flow of vortices revealed a double linearity field dependence of activation energy of vortices [Uo(H)], confirming the coexistence of single and collective pinning vortex states. Moreover, analysis of critical current density using the collective pinning theory showed the transformation of δTc to δl pinning as pressure increases, possibly due to migration of grain boundaries. Besides, the band structure calculations using density functional theory show that density of states decreases modestly with pressure, which may be a possible reason for such a small decrease in Tc by pressure.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Re6Hf Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.96 | Pressure unresolved | onset |
| Re6Hf Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.56 | Pressure unresolved | zero_resistance |
| Re6Hf Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.59 | 8 GPa | onset |
| Re6Hf Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.95 | Pressure unresolved | onset |
| Re6Hf Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 5.88 | 1.2 GPa | onset |
| LaNiC2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2.8 | Pressure not reported | unknown |
| BiPd Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.8 | Pressure not reported | unknown |
| SrPtAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 2.4 | Pressure not reported | unknown |
| Re3Ta Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 4.68 | Pressure not reported | unknown |
| Re24Ti5 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6 | Pressure not reported | unknown |
| Re0.82Nb0.18 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8.8 | Pressure not reported | unknown |
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