Interplay of electron–phonon interaction and strong correlations: the possible way to high-temperature superconductivity

2000 ◽  
Vol 338 (1-2) ◽  
pp. 1-264 ◽  
Author(s):  
Miodrag L. Kulić
1990 ◽  
Vol 04 (05) ◽  
pp. 325-331
Author(s):  
SURESH V. VETTOOR ◽  
V. M. NANDAKUMARAN

Electron-phonon interaction is considered within the framework of the fluctuating valence of Cu atoms. Anderson's lattice Hamiltonian is suitably modified to take this into account. Using Green's function technique the possible quasiparticle excitations are determined. The quantity 2∆k(0)/k B T c is calculated for T c = 40 K . The calculated values are in good agreement with the experimental results.


2014 ◽  
Vol 2014 ◽  
pp. 1-7 ◽  
Author(s):  
S. Orozco ◽  
R. M. Méndez-Moreno ◽  
M. A. Ortiz

The relation between thed-wave superconducting gapΔ0and the specific heat obtained with the Volovik effect is used to determine the upper critical fieldHc2as doping function, for high-temperature superconductors. A two-components model withd-wave symmetry, within the BCS framework, is introduced to describe the superconducting state. Generalized Fermi surface topologies are used in order to increase the density of states at the Fermi level, allowing the high-Tcvalues observed. The electron-phonon interaction is considered the most relevant mechanism for the high-Tccuprates, where the available phonon energy is provided by the half-breathing modes. The energy gap valuesΔ0calculated with this model are introduced to describe the variation of the upper critical fieldHc2as function of doping, forLa2-xSrxCuO4.


2008 ◽  
Vol 101 (10) ◽  
Author(s):  
O. Delaire ◽  
M. S. Lucas ◽  
J. A. Muñoz ◽  
M. Kresch ◽  
B. Fultz

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