Theory of High Temperature Superconductivity e-bog

Flux quantization experiments indicate that the carriers, Cooper pairs (pairons), in the supercurrent have charge magnitude 2e, and that they move independently. Josephson interference in a Superconducting Quantum Int- ference Device (SQUID) shows that the centers of masses (CM) of pairons move as bosons with a linear dispersion relation. Based on this evidence we develop a theory of superconductivity in conventional and mate- als from a unified point of view. Following Bardeen, Cooper and Schrieffer (BCS) we regard the phonon exchange attraction as the cause of superc- ductivity. For cuprate superconductors, however, we take account of both optical- and acoustic-phonon exchange. BCS started with a Hamiltonian containing "e;electron"e; and "e;hole"e; kinetic energies and a pairing interaction with the phonon variables eliminated. These "e;electrons"e; and "e;holes"e; were introduced formally in terms of a free-electron model, which we consider unsatisfactory. We define "e;electrons"e; and "e;holes"e; in terms of the cur- tures of the Fermi surface. "e;Electrons"e; (1) and "e;holes"e; (2) are different and so they are assigned with different effective masses: Blatt, Schafroth and Butler proposed to explain superconductivity in terms of a Bose-Einstein Condensation (BEC) of electron pairs, each having mass M and a size. The system of free massive bosons, having a quadratic dispersion relation: and moving in three dimensions (3D) undergoes a BEC transition at where is the pair density.