Evidence from anisotropic penetration depth for a three-dimensional nodal superconducting gap in single-crystalline Ba(Fe1−xNix)2As2
C. Martin, H. Kim, R. T. Gordon, N. Ni, V. G. Kogan, S. L. Bud’ko, P. C. Canfield, M. A. Tanatar, R. Prozorov
DOI 10.1103/PhysRevB.81.060505 · 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 London penetration depth, λ, is directly related to the density, ns, of the Cooper pairs (λ2∝1/ns) and its variation with temperature provides valuable insight into the pairing mechanism. Here we study the evolution with doping of the temperature dependence of the in-plane (λab) and out-of-plane (λc) penetration depths in single crystals of electron-doped Ba(Fe1−xNix)2As2. As is the case for other pnictides, λ(T)∼Tn over the whole doping range and this behavior extends down to at least T=Tc/100, setting a very small upper limit on the gap minimum. Furthermore, in the overdoped regime: (1) the exponent n becomes substantially smaller than 2, which is incompatible with the models that explain power-law behavior to be due to scattering; (2) the exponent n becomes anisotropic, with λc(T) showing a clear T-linear behavior over a large temperature interval. These findings suggest that in the overdoped regime the superconducting gap in iron-based pnictide superconductors develops nodal structure, which unlike in the cuprates, cannot be understood within a two-dimensional picture.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| Ba(Fe1-xNix)2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 7.5 | Pressure not reported | unknown |
| Ba(Fe1-xNix)2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 6.5 | Pressure not reported | unknown |
| Ba(Fe1-xNix)2As2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 15 | 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 |
Similar papers
Competition between superconductivity and magnetic/nematic order as a source of anisotropic superconducting gap in underdoped Ba1−xKxFe2As2
similarity 0.96H. Kim et al.
Source status unknown — claims are unverified
Superconducting gap symmetry in the superconductor BaFe1.9Ni0.1As2
similarity 0.96T. E. Kuzmicheva et al.
Source status unknown — claims are unverified
Dependence of Carrier Doping on the Impurity Potential in Transition-Metal-Substituted FeAs-Based Superconductors
similarity 0.96S. Ideta et al.
Source status unknown — claims are unverified
Direct observation of in-plane anisotropy of the superconducting critical current density in Ba(Fe1−xCox)2As2 crystals
similarity 0.96J. Hecher et al.
Source status unknown — claims are unverified
Manipulation of Gap Nodes by Uniaxial Strain in Iron-Based Superconductors
similarity 0.96Jian Kang et al.
Source status unknown — claims are unverified
Electron-doping evolution of the low-energy spin excitations in the iron arsenide superconductor BaFe2−xNixAs2
similarity 0.96Miaoyin Wang et al.
Source status unknown — claims are unverified