R. Zeyher et Ml. Kulic, RENORMALIZATION OF THE ELECTRON-PHONON INTERACTION BY STRONG ELECTRONIC CORRELATIONS IN HIGH-T-C SUPERCONDUCTORS, Physical review. B, Condensed matter, 53(5), 1996, pp. 2850-2862
The renormalization of the electron-phonon interaction by strong elect
ronic correlations is studied using a one-band Hubbard model with infi
nite repulsion and nearest (t model) and nearest and second-nearest (t
t' model) neighbor hopping terms and an on-site electron-phonon coupli
ng. Using Hubbard's X operators and an extension from 2 to N degrees o
f freedom for the electrons the leading contributions for the electron
self-energy and the vertex function in 1/N and the electron-phonon co
upling constant are given and numerically evaluated for a square latti
ce. We find that the momentum dependence of the vertex function depend
s strongly on doping: For large dopings it is rather weak, with decrea
sing doping it becomes more and more pronounced leading to a strong re
duction of the vertex at larger momentum transfers until, for very sma
ll dopings, the vertex essentially consists of a forward scattering pe
ak with a width proportional to the doping. This behavior occurs both
in the t and the tt' models and also in one dimension where analytic e
xpressions are derived. Correlation effects also change alpha(2)F in g
eneral: The full-symmetric component alpha(2)F(1) is in the t model so
mewhat, in the tt' model rather strongly suppressed, especially near h
alf-filling; the other symmetry components alpha(2)F(i) with i=2,...,5
increase strongly with decreasing doping and are of similar magnitude
as alpha(2)F(1) near half-filling. Including also direct Coulomb repu
lsion nontrivial symmetries such as d wave become more stable than the
s-wave order parameter below a critical value for the doping even for
the considered phonon-mediated superconductivity. Most dramatic, howe
ver, is the quenching of the resistivity due to electron-phonon scatte
ring both in the t and the tt' models at intermediate and small doping
s. This result may explain the absence of phonon features in the exper
imental transport coefficients of high-T-c compounds.