Forward scattering peak in the electron-phonon interaction and impurity scattering of cuprate superconductors

2005 ◽  
Vol 242 (1) ◽  
pp. 151-178 ◽  
Author(s):  
M. L. Kulić ◽  
O. V. Dolgov
Keyword(s):  
Cuprate Superconductors ◽  
Impurity Scattering ◽  
Forward Scattering ◽  
Phonon Interaction ◽  
Electron Phonon Interaction

ELECTRONIC THEORY FOR ELECTRON-DOPED CUPRATE SUPERCONDUCTORS: d-WAVE SUPERCONDUCTIVITY AND THE PHASE DIAGRAM

2000 ◽  
Vol 14 (29n31) ◽  
pp. 3555-3560
Author(s):  
D. MANSKE ◽  
I. EREMIN ◽  
K. H. BENNEMANN
Keyword(s):  
Cuprate Superconductors ◽  
Narrow Range ◽  
Spin Fluctuation ◽  
Flat Band ◽  
Superconducting Transition ◽  
Phonon Interaction ◽  
Pairing Mechanism ◽  
Lattice Disorder ◽  
Electron Phonon Interaction ◽  
The One

Using the one-band Hubbard Hamiltonian we determine various basic properties of the electron-doped cuprate superconductor Nd 2-x Ce x CuO 4 for a spin-fluctuation-induced pairing mechanism. We find a narrow range of superconductivity and, most importantly, like for hole-doped cuprates dx2-y2 -symmetry for the superconducting order parameter. The superconducting transition temperatures Tc(x) for various electron doping concentrations x are calculated to be much smaller than for hole-doped cuprates due to the different energy dispersion and a flat band well below the Fermi level. We find that lattice disorder may sensitively distort the dx2-y2 -symmetry via electron-phonon interaction yielding a finite isotope exponent α0.

scholarly journals A COMPARISON OF THE RESISTIVITY BEHAVIOR OF MgB2, AlB2 AND AgB2 SYSTEMS

2006 ◽  
Vol 20 (16) ◽  
pp. 989-994 ◽  
Author(s):  
R. LAL ◽  
V. P. S. AWANA ◽  
K. P. SINGH ◽  
R. B. SAXENA ◽  
H. KISHAN ◽  
...  
Keyword(s):  
Phonon Scattering ◽  
Weak Localization ◽  
Impurity Scattering ◽  
Phonon Interaction ◽  
Electron Phonon Interaction ◽  
Maximum Minimum ◽  
Electron Phonon Scattering

Measurements have been performed on the resistivity of samples MgB 2, AlB 2 and AgB 2. The samples show presence of impurities. By analyzing the data in terms of impurity scattering, electron-phonon scattering, and weak localization, it has been found that the AlB 2 ( AgB 2) sample involves maximum (minimum) effect of the impurity, electron-phonon interaction and weak localization.

Impurity induced renormalized phonon spectrum of cuprate superconductors

2018 ◽  
Vol 32 (22) ◽  
pp. 1850237 ◽  
Author(s):  
Anushri Gupta ◽  
Sanjeev K. Verma ◽  
Anita Kumari ◽  
B. D. Indu
Keyword(s):  
Cuprate Superconductors ◽  
Potential Problem ◽  
High Temperature Superconductors ◽  
Many Body ◽  
Phonon Interaction ◽  
Electron Phonon Interaction ◽  
Many Body Theory ◽  
Anharmonic Lattice ◽  
The Many ◽  
Body Theory

The potential problem of anharmonic lattice vibrations in high-temperature superconductors (HTS) using the most suitable Born–Mayer–Huggins (BMH) potential has been taken up to investigate the renormalized phonon density of states (RPDOS). In order to develop the suitable results, the many body theory using quantum dynamical approach of Green’s function (GF) via an almost complete Hamiltonian (without using BCS type Hamiltonian) has been incorporated which includes harmonic electron and phonon Hamiltonian, electron–phonon interaction Hamiltonian, anharmonic and defect Hamiltonian. The derivation of anharmonic phonon GF for modified form of BMH potential enables to evaluate the renormalized and perturbed mode phonon frequencies of solids. The expressions obtained for the RPDOS can be resolved into diagonal and nondiagonal parts of which the nondiagonal part chiefly depends on impurities and disappears in pure crystals. A large number of new features are investigated in the light of this formulation followed by the numerical analysis for the energy spectrum of representative cuprate HTS YBa2Cu3O[Formula: see text]. The inclusion of defects, anharmonicities and electron–phonon interactions in the cuprate superconductors substantially modifies the scenario of RPDOS and reveals a large number of unexplained peaks in the spectrum.

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