Large Theory of Superconducting Fluctuations in a Magnetic Field and its Application to Iron-Pnictides
arXiv:1004.5277 · doi:10.1103/PhysRevLett.105.037006
Abstract
A Ginzburg-Landau approach to fluctuations of a layered superconductor in a magnetic field is used to show that the interlayer coupling can be incorporated within an interacting self-consistent theory of a single layer, in the limit of a large number of neighboring layers. The theory exhibits two phase transitions -- a vortex liquid-to-solid transition is followed by a Bose-Einstein condensation into the Abrikosov lattice -- illustrating the essential role of interlayer coupling. Using this theory, explicit expressions for magnetization, specific heat, and fluctuation conductivity are derived. We compare our results with recent experimental data on the iron-pnictide superconductors.
5 pages, 3 figures. Published version. Streamlined presentation; typos corrected in Eqs. (14, 20) and elsewhere; improved Figs. (1, 3); additional references
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Cited by in corpus (5)
- Measurements of the superconducting fluctuations in optimally-doped BaFeNiAs under high magnetic fields: Probing the 3D anisotropic Ginzburg-Landau approach
- As NMR of Ba(FeCo)As in High Magnetic Field
- Vortex-lattice melting and paramagnetic depairing in the nematic superconductor FeSe
- Measurements of the fluctuation-induced in-plane magnetoconductivity at high reduced temperatures and magnetic fields in the iron arsenide BaFe(2-x)NixAs2
- Large increase of the anisotropy factor in the overdoped region of Ba(FeNi)As as probed by fluctuation spectroscopy