Abstract
The one-dimensional Hubbard model with arbitrary degeneracy N (N = 2S + 1, where S is the spin) is integrable if site-occupations of more than two electrons are excluded. The Bethe-ansatz equations are analyzed in the thermodynamic limit in the absence of external fields. In the large N limit they reduce to those of a hard core Bose gas. The 1/N-correction to the leading order result vanishes identically, so that the first corrections are contributions of the order 1/N2.
| Original language | English |
|---|---|
| Pages (from-to) | 398-400 |
| Number of pages | 3 |
| Journal | Physica B: Condensed Matter |
| Volume | 163 |
| Issue number | 1-3 |
| DOIs | |
| State | Published - Apr 1990 |
Bibliographical note
Funding Information:We would like to acknowledge the support by US Department of Energy under the grant DE-FGOZ 87ER45333.