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Physical Review B - Condensed Matter and Materials Physics

Volumn 78, Issue 10, 2008, Pages

Fermi-liquid effects in the gapless state of marginally thin superconducting films

(3) Catelani, G a Wu, X S b,c Adams, P W b

a RUTGERS UNIVERSITY (United States)

b LOUISIANA STATE UNIVERSITY (United States)

c GEORGIA INSTITUTE OF TECHNOLOGY (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 52949154340 PISSN: 10980121 EISSN: 1550235X Source Type: Journal
DOI: 10.1103/PhysRevB.78.104515 Document Type: Article

Times cited : (36)

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- This estimate of ξ is obtained using the value of the mean free path ℓ reported in Ref. via ξ ≃√ξ0ℓ, where ξ0 =hvF/pi;Δo and vF is the Fermi velocity. To further support this estimate we note that a separate measurement of the perpendicular critical field for a similarly prepared 6 nm thick film gives ξ≃56 nm (here we use Hc⊥ = φ0 /2π ξ2 with φ0 the flux quantum).
- This estimate of ξ is obtained using the value of the mean free path ℓ reported in Ref. via ξ ≃√ξ0ℓ, where ξ0 =hvF/pi;Δo and vF is the Fermi velocity. To further support this estimate we note that a separate measurement of the perpendicular critical field for a similarly prepared 6 nm thick film gives ξ≃56 nm (here we use Hc⊥ = φ0 /2π ξ2 with φ0 the flux quantum).

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- For example, no broadening is used in the upper panel curve-including it would slightly suppress the peaks' magnitude. Due to their interdependence, however, different values for c and Γ ≠ 0 could also satisfactorily fit the data.
- For example, no broadening is used in the upper panel curve-including it would slightly suppress the peaks' magnitude. Due to their interdependence, however, different values for c and Γ ≠ 0 could also satisfactorily fit the data.

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