Type-I superconductivity in the noncentrosymmetric superconductor BeAu
D. Singh, A. D. Hillier, R. P. Singh
DOI 10.1103/PhysRevB.99.134509 · 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
The noncentrosymmetric superconductor BeAu has been investigated using magnetization, resistivity, specific heat, and muon-spin relaxation/rotation. BeAu crystallizes in a cubic FeSi-type B20 structure with a superconducting transition temperature Tc=3.2±0.1K. The low-temperature specific heat data, Cel(T), indicates a weakly-coupled fully gapped BCS superconductivity with an isotropic energy gap 2Δ(0)/kBTc=3.76, close to the BCS value of 3.52. Interestingly, type-I superconductivity is inferred from the μSR measurements, in contrast to the earlier reports of type-II superconductivity in BeAu. The Ginzburg-Landau parameter is κGL=0.4<1/2. The frequency domain transverse-field μSR spectra, depicting the internal magnetic field probability distribution, P(B), also confirms the absence of the mixed state in BeAu. The thermodynamic critical field, Hc, is calculated to be around 259 Oe. The zero-field μSR results indicate that time-reversal symmetry is preserved and supports a spin-singlet pairing in the superconducting ground state.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| BeAu Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.2 | Pressure not reported | midpoint |
| BeAu Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.2 | Pressure not reported | onset |
| BeAu Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.17 | Pressure not reported | unknown |
| BeAu Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.2 | Pressure not reported | unknown |
| CePt3Si Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Li2Pt3B Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| CeIrSi3 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| LaNiC2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Multiple-gap response of type-I noncentrosymmetric BeAu superconductor
similarity 0.96Rustem Khasanov et al.
Source status unknown — claims are unverified
Influence of pressure on the properties of the multigap type-I superconductor BeAu
similarity 0.96Rustem Khasanov et al.
Source status unknown — claims are unverified
Spin susceptibility of noncentrosymmetric superconductors
similarity 0.96K. V. Samokhin
Source status unknown — claims are unverified
Effects of impurities on superconductivity in noncentrosymmetric compounds
similarity 0.95V. P. Mineev & K. V. Samokhin
Source status unknown — claims are unverified
μSR and magnetometry study of the type-I superconductor BeAu
similarity 0.95J. Beare et al.
Source status unknown — claims are unverified
Pressure-Induced Superconductivity in Noncentrosymmetric Heavy-Fermion CeRhSi3
similarity 0.94N. Kimura et al.
Source status unknown — claims are unverified