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Physica C Superconductivity

Spin-charge separation in an extended Hubbard model: a large D study

J.Lleweilun Smith, Qimiao Si A

Published Nov 1, 2000• 1 citation
Publisher
DOI
10.1016/s0921-4534(00)00418-4

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We propose an effective model called the ``charge model,'' for the half-filled one-dimensional Hubbard and extended Hubbard models. In this model, spin-charge separation, which has been justified from an infinite on-site repulsion (UUU) in the strict sense, is compatible with charge fluctuations. Our analyses based on the many-body Wannier functions succeeded in determining the optical conductivity spectra in large systems. The obtained spectra reproduce the spectra for the original models well even in the intermediate UUU region of U=5U=5U=5--10T10T10T, with TTT being the nearest-neighbor electron hopping energy. These results indicate that the spin-charge separation works fairly well in this intermediate UUU region against the usual expectation and that the charge model is an effective model that applies to actual quasi-one-dimensional materials classified as strongly correlated electron systems.
I summarize recent work on non-Fermi liquids within a certain generalized Anderson impurity model as well as in the large-dimensionality (D) limit of the two-band extended Hubbard model. The competition between local charge and spin fluctuations leads either to a Fermi liquid with renormalized quasiparticle excitations, or to non-Fermi liquids with spin - charge separation. These results provide new insights into the phenomenological similarities and differences between different correlated metals. While presenting these results, I outline a general strategy of local approach to non-Fermi liquids in correlated electron systems.