Hydrogen in layered iron arsenide: indirect electron doping to induce superconductivity
arXiv:1103.1177 · doi:10.1103/PhysRevB.84.024521
Abstract
Utilizing the high stability of calcium and rare earth hydrides, CaFeAsF1-xHx (x = 0.0-1.0) and SmFeAsO1-xHx (x = 0.0-0.47) have been first synthesized using high pressure to form hydrogen-substituted 1111 type iron-arsenide superconductors. Neutron diffraction and density functional calculations have demonstrated that the hydrogens are incorporated as H- ions occupying F- sites in the blocking layer of CaFeAsF. The resulting CaFeAsF1-xHx is non-superconducting, whereas SmFeAsO1-xHx is a superconductor, with an optimal Tc = 55 K at x 0.2. It was found that up to 40% of the O2- ions can be replaced by H- ions, with electrons being supplied into the FeAs-layer to maintain neutrality (O2- = H-+ e-). When x exceeded 0.2, Tc was reduced corresponding to an electron over-doped region.
14 pages, 4 figures
References in corpus (19)
- Superconductivity at 38 K in the iron arsenide (Ba1-xKx)Fe2As2
- Superconductivity at 43 K in Samarium-arsenide Oxides
- Superconductivity at 41 K and its competition with spin-density-wave instability in layered CeOFFeAs
- The superconductivity at 18 K in LiFeAs system
- Superconductivity and Phase Diagram in the Iron-based Arsenic-oxides ReFeAsO1-delta (Re = rare earth metal) without F-Doping
- Superconductivity in iron-based F-doped layered quaternary compound Nd[O1-xFx]FeAs
- Superconductivity at 52 K in iron-based F-doped layered quaternary compound Pr[O1-xFx]FeAs
- Superconductivity in Co-doped LaFeAsO
- Crystallographic Phase Transition and High-Tc Superconductivity in LaFeAsO:F
- Superconductivity at 17 K in (Fe2P2)(Sr4Sc2O6): a new superconducting layered pnictide oxide with a thick perovskite oxide layer
- Effect of Co doping on superconductivity and transport properties in SmFeCoAsO
- Superconductivity induced by cobalt doping in iron-based oxyarsenides
- Different resistivity response to spin density wave and superconductivity at 20 K in
- Superconductivity above 50K in LnFeAsO1-y (Ln= Nd, Sm, Gd, Tb and Dy) Synthesized by High-pressure Technique
- Narrow superconducting window in Ni-doped LaFeAsO
- Effect of 3d Transition Metal Doping on the Superconductivity in Quaternary Fluoroarsenide CaFeAsF
- Absence of an appreciable iron isotope effect on the transition temperature of the optimally doped SmFeAsO_{1-y} superconductor
- WDX-Analysis of the New Superconductors RO(1-x)F(x)FeAs and Its Consequences on the Electronic Phase Diagram
- Mechanism of phase transitions and the electronic density of states in (La,Sm)FeAsOF from ab initio calculations