Theory of High Temperature Superconductivity

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 b...

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Bibliographic Details
Corporate Author: SpringerLink (Online service)
Other Authors: Fujita, Shigeji. (Editor), Godoy, Salvador. (Editor)
Format: Electronic
Language:English
Published: Dordrecht : Springer Netherlands, 2001.
Series:Fundamental Theories of Physics, An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application ; 121
Subjects:
Online Access:View fulltext via EzAccess
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490 1 # |a Fundamental Theories of Physics, An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application ;  |v 121 
505 0 # |a Superconducting Transition -- Bloch Electrons -- Phonon-Exchange Attraction -- Quantum Statistical Theory -- Cooper Pairs (Pairons) -- Superconductors at 0 K -- Quantum Statistics of Composites -- Bose-Einstein Condensation -- The Energy Gap Equations -- Pairon Energy Gaps. Heat Capacity -- Quantum Tunneling -- Flux Quantization -- Ginzburg-Landau Theory -- Josephson Effects -- Compound Superconductors -- Lattice Structures of Cuprates -- High-Tc Superconductors Below Tc -- Doping Dependence of Tc -- Transport Properties Above Tc -- Out-of-Plane Transport -- Seebeck Coefficient (Thermopower) -- Magnetic Susceptibility -- Infrared Hall Effect -- d-Wave Cooper Pairs -- Connection with Other Theories -- Summary and Remarks. 
520 # # |a 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 ỚSelectronỚ<U+00fd> and ỚSholeỚ<U+00fd> kinetic energies and a pairing interaction with the phonon variables eliminated. These ỚSelectronsỚ<U+00fd> and ỚSholesỚ<U+00fd> were introduced formally in terms of a free-electron model, which we consider unsatisfactory. We define ỚSelectronsỚ<U+00fd> and ỚSholesỚ<U+00fd> in terms of the cur- tures of the Fermi surface. ỚSElectronsỚ<U+00fd> (1) and ỚSholesỚ<U+00fd> (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. 
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650 # 0 |a Physical chemistry. 
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