Isotope effect due to the super-exchange interaction and van Hove singularity in high-Tc superconductors

2013 ◽  
Vol 114 (6) ◽  
pp. 063901
Author(s):  
A. Bechlaghem ◽  
D. Bourbie
1995 ◽  
Vol 09 (09) ◽  
pp. 1067-1080 ◽  
Author(s):  
M.L. HORBACH ◽  
H. KAJÜTER

Experimental indications for the role of the van Hove singularity (vHs) in the electronic density of states of high Tc superconductors are discussed. It is argued that (i) like the resistivity, the measured temperature and doping dependences of the normal state electronic specific heat of YBCO are consistent with the existence of a vHs and (ii) the doping dependence of Tc in the underdoped and optimally doped regimes may be accounted for mainly by a vHs. Further, we discuss the suppression of the quasiparticle scattering rate below Tc, and the coherence lengths in the hole-doped materials and NCCO. Assuming that the same mechanism for superconductivity operates in the electron-doped and the hole-doped cuprates, we argue that the bosonic mode that causes the superconductivity is strongly influenced by the doping in the overdoped regime. We further argue that this boson involves an energy scale larger than that of phonons and is only weakly coupled to the charge carriers.


2011 ◽  
Vol 25 (26) ◽  
pp. 2069-2078 ◽  
Author(s):  
A. BECHLAGHEM ◽  
D. BOURBIE

Analytical expressions for the superconducting transition temperature Tc and the isotope coefficient α have been obtained for the case where the Fermi level is close to the van Hove singularity. In this approach, we consider two interactions, the first related to the phonons and the second relevant to the magnetic excitations. Our result shows that the isotope coefficient α decreases with the superconducting transition temperature Tc in qualitative agreement with experimental data.


1987 ◽  
Vol 144 (2) ◽  
pp. K113-K117 ◽  
Author(s):  
S. L. Drechsler ◽  
N. M. Plakida

1999 ◽  
Vol 13 (32) ◽  
pp. 3915-3925 ◽  
Author(s):  
A. BECHLAGHEM ◽  
M. MOSTEFA ◽  
Y. ZANOUN

The model recently developed by Getino et al. to study the gap energy in the van Hove scenario in high-T c oxides is extended to study the isotope effect and the coherence length in these materials. We propose a more realistic model by: (1) adding a constant term to the singular logarithmic contribution, within the weak coupling BCS theory and a phonon mediated interaction; (2) assuming the Fermi level lies close to a van Hove singularity for optimal doping. The equations obtained from this approach, are applicable to low as well as high temperature superconductors successfully the superconducting temperature transition T c , the gap energy Δ, the isotope effect α and the coherence length ξ. For high-T c oxides, it is found that when the effective mass of carriers tends to be large, α and ξ tend to be small where T c and Δ became larges. We shown that when the effective mass of carriers is enclosed between 5 m e and 15 m e , the values obtained for these parameters are in agreement with experimental data.


1989 ◽  
Vol 03 (06) ◽  
pp. 897-908 ◽  
Author(s):  
T. GALBAATAR ◽  
R-J. RAKAUSKAS ◽  
J. SULSKUS

The results of a numerical simulation are presented for the oxygen isotope effect in the high-T c oxides by solving the Schrödinger equation for a local vibrational mode of oxygen ions in a double well anharmonic potential of the form −Ax2/2+Bx4/4. The features of the energy spectrum, eigenfunctions and the matrix elements of the dipole and quadrupole moments are discussed. The applicability region of a two-level approximation to describe the electron-phonon interaction is given. The constant of the isotope effect α is determined to be comparable to that of La 2−x Sr x CuO 4 but in disagreement with the up-to-date experimental observations for the YBaCuO system.


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