The effects of hydrostatic pressure and partial Na substitution on the normal-state properties and the superconducting transition temperature (T-c) of K1-xNaxFe2As2 single crystals were investigated. It was found that a partial Na substitution leads to a deviation from the standard T-2 Fermi-liquid behavior in the temperature dependence of the normal-state resistivity. It was demonstrated that non-Fermi-liquid like behavior of the resistivity for K1-xNaxFe2As2 and some KFe2As2 samples can be explained by a disorder effect in the multiband system with rather different quasiparticle effective masses. Concerning the superconducting state our data support the presence of a shallow minimum around 2 GPa in the pressure dependence of T-c for stoichiometric KFe2As2. The analysis of T-c in K1-xNaxFe2As2 at pressures below 1.5 GPa showed that the reduction of T-c with Na substitution follows the Abrikosov-Gor'kov law with the critical temperature T-c0 of the clean system (without pair breaking), which linearly depends on the pressure. Our observations also suggest that T-c of K1-xNaxFe2As2 is nearly independent of the lattice compression produced by the Na substitution. Further, we theoretically analyzed the behavior of the band structure under pressure within the generalized gradient approximation (GGA). A qualitative agreement between the calculated and the recently measured-in de Haas-van Alphen experiments [T. Terashima et al., Phys. Rev. B 89, 134520 (2014)]-pressure dependencies of the Fermi-surface cross sections has been found. These calculations also indicate that the observed minimum around 2 GPa in the pressure dependence of T-c may occur without a change of the pairing symmetry.
Superconducting properties of K1-xNaxFe2As2 under pressure
Profeta G
2014
Abstract
The effects of hydrostatic pressure and partial Na substitution on the normal-state properties and the superconducting transition temperature (T-c) of K1-xNaxFe2As2 single crystals were investigated. It was found that a partial Na substitution leads to a deviation from the standard T-2 Fermi-liquid behavior in the temperature dependence of the normal-state resistivity. It was demonstrated that non-Fermi-liquid like behavior of the resistivity for K1-xNaxFe2As2 and some KFe2As2 samples can be explained by a disorder effect in the multiband system with rather different quasiparticle effective masses. Concerning the superconducting state our data support the presence of a shallow minimum around 2 GPa in the pressure dependence of T-c for stoichiometric KFe2As2. The analysis of T-c in K1-xNaxFe2As2 at pressures below 1.5 GPa showed that the reduction of T-c with Na substitution follows the Abrikosov-Gor'kov law with the critical temperature T-c0 of the clean system (without pair breaking), which linearly depends on the pressure. Our observations also suggest that T-c of K1-xNaxFe2As2 is nearly independent of the lattice compression produced by the Na substitution. Further, we theoretically analyzed the behavior of the band structure under pressure within the generalized gradient approximation (GGA). A qualitative agreement between the calculated and the recently measured-in de Haas-van Alphen experiments [T. Terashima et al., Phys. Rev. B 89, 134520 (2014)]-pressure dependencies of the Fermi-surface cross sections has been found. These calculations also indicate that the observed minimum around 2 GPa in the pressure dependence of T-c may occur without a change of the pairing symmetry.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
