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      Topological Theory of Ceramic High Temperature Superconductors

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          Abstract

          Optimally doped ceramic superconductors (cuprates, pnictides, ...) exhibit transition temperatures Tc much larger than strongly coupled metallic superconductors like Pb (Tc= 7.2K, Eg/kTc = 4.5), and exhibit many universal features that appear to contradict the BCS theory of superconductivity based on attractive electron-phonon pairing interactions. Here I argue that this paradoxical simplicity is plausibly resolved within the framework of the Pauling-Phillips self-organized, hard-wired dopant network model of ceramic superconductors, which has previously explained many features of the normal-state transport properties of these materials and successfully predicted strict lowest upper bounds for Tc in the cuprate and pnictide families.

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          Electrodynamics of high-Tcsuperconductors

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            Beyond Eliashberg superconductivity in MgB2: anharmonicity, two-phonon scattering, and multiple gaps

            Density-functional calculations of the phonon spectrum and electron-phonon coupling in MgB\(_2\) are presented. The \(E_{2g}\) phonons, which involve in-plane B displacements, couple strongly to the \(p_{x,y}\) electronic bands. The isotropic electron-phonon coupling constant is calculated to be about 0.8. Allowing for different order parameters in different bands, the superconducting \(\lambda\) in the clean limit is calculated to be significantly larger. The \(E_{2g}\) phonons are strongly anharmonic, and the non-linear contribution to the coupling between the \(E_{2g}\) modes and the p\(_{x,y}\) bands is significant.
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              Electronic Phase Diagram of High-T_c Cuprate Superconductors from a Mapping of the In-Plane Resistivity Curvature

              We propose that Resistivity Curvature Mapping (RCM) based on the in-plane resistivity data is a useful way to objectively draw an electronic phase diagrams of high-T_c cuprates, where various crossovers are important. In particular, the pseudogap crossover line can be conveniently determined by RCM. We show experimental phase diagrams obtained by RCM for Bi_{2}Sr_{2-z}La_{z}CuO_{6+\delta}, La_{2-x}Sr_{x}CuO_{4}, and YBa_{2}Cu_{3}O_{y}, and demonstrate the universal nature of the pseudogap crossover. Intriguingly, the electronic crossover near optimum doping depicted by RCM appears to occur rather abruptly, suggesting that the quantum critical regime, if exists, must be very narrow.
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                Author and article information

                Journal
                30 April 2009
                2009-05-10
                Article
                0905.0023
                c411941e-e6f8-48af-ab4d-80736248827a

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                cond-mat.supr-con

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