FeTe0.55Se0.45: A multiband superconductor in the clean and dirty limit
C. C. Homes, Y. M. Dai, J. S. Wen, Z. J. Xu, G. D. Gu
DOI 10.1103/PhysRevB.91.144503 · 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 detailed optical properties of the multiband iron-chalcogenide superconductor FeTe0.55Se0.45 have been reexamined for a large number of temperatures above and below the critical temperature Tc=14K for light polarized in the a−b planes. Instead of the simple Drude model that assumes a single band, above Tc the normal-state optical properties are best described by the two-Drude model that considers two separate electronic subsystems; we observe a weak response (ωp,D;1≃3000cm−1) where the scattering rate has a strong temperature dependence (1/τD,1≃32cm−1 for T≳Tc), and a strong response (ωp,D;2≃14500cm−1) with a large scattering rate (1/τD,2≃1720cm−1) that is essentially temperature independent. The multiband nature of this material precludes the use of the popular generalized-Drude approach commonly applied to single-band materials, implying that any structure observed in the frequency-dependent scattering rate 1/τ(ω) is spurious and it cannot be used as the foundation for optical inversion techniques to determine an electron-boson spectral function α2F(ω). Below Tc the optical conductivity is best described using two superconducting optical gaps of 2Δ1≃45 and 2Δ2≃90cm−1 applied to the strong and weak responses, respectively. The scattering rates for these two bands are vastly different at low temperature, placing this material simultaneously in both clean and dirty limit. Interestingly, this material falls on the universal scaling line initially observed for the cuprate superconductors.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| FeTe0.55Se0.45 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 14 | Pressure unresolved | unknown |
| FeTe0.55Se0.45 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 14 | Pressure unresolved | unknown |
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 8 | Pressure unresolved | unknown |
| FeSe Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 37 | Pressure not reported | unknown |
Similar papers
Unusual Relationship between Magnetism and Superconductivity in FeTe0.5Se0.5
similarity 0.96H. A. Mook et al.
Source status unknown — claims are unverified
FeTeSe: a multiband superconductor in the clean and dirty limit
similarity 0.95C. C. Homes et al. · 2015 · arXiv:1502.07604
Source status unknown — claims are unverified
Superconductivity at Tc∼14 K in single-crystalline FeTe0.61Se0.39
similarity 0.95T. Taen et al.
Source status unknown — claims are unverified
Effect of impurity substitution on band structure and mass renormalization of the correlated FeTe0.5Se0.5 superconductor
similarity 0.95S. Thirupathaiah et al.
Source status unknown — claims are unverified
Spin fluctuations and superconductivity in powders of Fe1+xTe0.7Se0.3 as a function of interstitial iron concentration
similarity 0.95C. Stock et al.
Source status unknown — claims are unverified
Calorimetric evidence of strong-coupling multiband superconductivity in Fe(Te0.57Se0.43) single crystal
similarity 0.94J. Hu et al.
Source status unknown — claims are unverified