Abstract
We have investigated effects of a finite band width on the electron-spin-fluctuation coupling constant λsf and the electron-phonon coupling constant λph in the Hubbard Hamiltonian system. We have found that both λph and λsf are reduced a lot in overall magnitudes by an effect of the finite band width. From the phonon self-energy, we have obtained the renormalized phonon frequency, which becomes hardened with increasing the Coulomb correlation. In particular, λph becomes larger than λsf for a system with a nearly filled band, which indicates that a phonon mediated BCS superconductivity may be possible in correlated systems.
| Original language | English |
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| Pages (from-to) | S75-S79 |
| Journal | Journal of the Korean Physical Society |
| Volume | 29 |
| Issue number | SUPPL. Part 1 |
| State | Published - 1996 |