Superconductivity in iron silicide Lu2Fe3Si5 probed by radiation-induced disordering
A. E. Karkin, M. R. Yangirov, Yu. N. Akshentsev, B. N. Goshchitskii
DOI 10.1103/PhysRevB.84.054541 · 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
Resistivity ρ(T), Hall coefficient RH(T), superconducting temperature Tc, and the slope of the upper critical field −dHc2/dT were studied in poly- and single-crystalline samples of the Fe-based superconductor Lu2Fe3Si5 irradiated by fast neutrons. Atomic disordering induced by the neutron irradiation leads to a fast suppression of Tc similarly to the case of doping of Lu2Fe3Si5 with magnetic (Dy) and nonmagnetic (Sc, Y) impurities. The same effect was observed in a novel FeAs-based superconductor La(O-F)FeAs after irradiation. Such behavior is accounted for by strong pair breaking that is traceable to scattering at nonmagnetic impurities or radiation defects in these unconventional superconductors. In such superconductors, the sign of the order parameter changes between the different Fermi sheets (s± model). Some relations that are specified for the properties of the normal and superconducting states in high-temperature superconductors are also observed in Lu2Fe3Si5. The first is the relationship −dHc2/dT ∼ Tc, which allows us to assign the compound Lu2Fe3Si5 to type II superconductors in the clean limit. The second is a correlation between the low-temperature linear coefficient a in the resistivity ρ = ρ0 + a1T, which appears presumably due to the scattering at magnetic fluctuations, and Tc, this correlation being an evidence of a tight relation between the superconductivity and magnetism. Data point to an unconventional (nonphononic) mechanism of superconductivity in Lu2Fe3Si5 and probably in some other Fe-based compounds, which can be fruitfully studied via the radiation-induced disordering.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Lu2Fe3Si5 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6 | Pressure not reported | unknown |
| La(O-F)FeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Nb3Sn Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| V3Si Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Mo3Si Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Mo3Ge Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| MgB2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| YBa2Cu3O7 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Ba(Fe1-xCox)2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Tl2Ba2CuO6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Nd(O-F)FeAs Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Observations of the effect of strong Pauli paramagnetism on the vortex lattice in superconducting CeCu2Si2
similarity 0.96E. Campillo et al.
Source status unknown — claims are unverified
Importance of structural instability to high-temperature superconductivity
similarity 0.96A. Bussmann-Holder et al.
Source status unknown — claims are unverified
Intrinsic and structural isotope effects in iron-based superconductors
similarity 0.96R. Khasanov et al.
Source status unknown — claims are unverified
Topological phase fluctuations, amplitude fluctuations, and criticality in extreme type-II superconductors
similarity 0.96A. K. Nguyen & A. Sudbø
Source status unknown — claims are unverified
Phenomenology of the superconducting state of a marginal Fermi liquid with BCS model interaction
similarity 0.96M. L. Horbach et al.
Source status unknown — claims are unverified
Unconventional isotope effects in superconductors
similarity 0.96Vladimir Z. Kresin et al.
Source status unknown — claims are unverified