Stoichiometry, Spin Fluctuations, and Superconductivity in LaNiPO
arXiv:0904.4237 · doi:10.1103/PhysRevB.79.172502
Abstract
Superconductivity in LaNiPO is disrupted by small (~5%) amounts of non-stoichiometry on the lanthanum site, even though the electronic contribution to the heat capacity increases with increasing non-stoichiometry. All samples also exhibit specific heat anomalies consistent with the presence of ferromagnetic spin fluctuations (Tsf ~ 14 K). Comparison of layered nickel phosphide and nickel borocarbide superconductors reveals different structure-property correlations in the two families.
Submitted to Phys. Rev. B
References in corpus (12)
- Superconductivity at 38 K in the iron arsenide (Ba1-xKx)Fe2As2
- Structural and magnetic phase diagram of CeFeAsO1-xFx and its relationship to high-temperature superconductivity
- Superconductivity up to 37 K in (A1-xSrx)Fe2As2 with A=K and Cs
- LiFeAs: An Intrinsic FeAs-based Superconductor with Tc = 18K
- Superconductivity at 52 K in iron-based F-doped layered quaternary compound Pr[O1-xFx]FeAs
- First Order Phase Transition and Superconductivity in BaNi2As2 Single Crystals
- Nickel-based phosphide superconductor with infinite-layer structure, BaNi2P2
- Intrinsic Properties of Stoichiometric LaOFeP
- Strong-coupling superconductivity in layered nickel-based LaOFNiAs
- Superconductivity and the Effects of Pressure and Structure in Single Crystalline SrNiP
- Electron Phonon Superconductivity in LaNiOP
- Electronic structure and Fermi surface character of LaONiP from first principles