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|a 9780306482168
|9 978-0-306-48216-8
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|a 10.1007/0-306-48216-9
|2 doi
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|a QC173.45-173.458
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|a 530.41
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|a Theory of High Temperature Superconductivity
|h [electronic resource] /
|c edited by Shigeji Fujita, Salvador Godoy.
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|a Dordrecht :
|b Springer Netherlands,
|c 2001.
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|a XIX, 374 p.
|b online resource.
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|a text
|b txt
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|a computer
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|a Fundamental Theories of Physics, An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application ;
|v 121
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|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.
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|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 “electron” and “hole” kinetic energies and a pairing interaction with the phonon variables eliminated. These “electrons” and “holes” were introduced formally in terms of a free-electron model, which we consider unsatisfactory. We define “electrons” and “holes” in terms of the cur- tures of the Fermi surface. “Electrons” (1) and “holes” (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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|a Physics.
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|a Physical chemistry.
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|a Condensed matter.
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|a Statistical physics.
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|a Dynamical systems.
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|a Physics.
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|a Condensed Matter Physics.
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|a Physical Chemistry.
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|a Statistical Physics, Dynamical Systems and Complexity.
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|a Fujita, Shigeji.
|e editor.
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|a Godoy, Salvador.
|e editor.
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|a SpringerLink (Online service)
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|t Springer eBooks
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|i Printed edition:
|z 9781402001499
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|a Fundamental Theories of Physics, An International Book Series on The Fundamental Theories of Physics: Their Clarification, Development and Application ;
|v 121
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|u http://dx.doi.org/10.1007/0-306-48216-9
|z Full Text via HEAL-Link
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|a ZDB-2-PHA
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|a ZDB-2-BAE
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|a Physics and Astronomy (Springer-11651)
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