Metal to Insulator Transition in the 2-D Hubbard Model: A Slave Boson Approach

dc.creatorFresard, Raymond
dc.creatorDoll, Klaus
dc.date1996-03-18
dc.date.accessioned2026-07-07T03:08:26Z
dc.date.available2026-07-07T03:08:26Z
dc.descriptionWe use the Kotliar-Ruckenstein slave boson technique to treat the strong correlation of the Hubbard model. In a first part we discuss the metal to insulator transition that is occurring on the honeycomb lattice at half filling. We find the critical value for the interaction strength to be U/t=3.1. Above it a gap opens in the spectrum which behaves like (U-U_c) in the vicinity of the transition, and like U for strong coupling. In a second part we calculate the phase diagram of the Hubbard model on the square lattice at finite temperature. The Mermin-Wagner theorem is fulfilled in the largest part of the phase diagram. In the strong coupling regime, the uniform magnetic susceptibility shows a maximum in its doping dependence in agreement with numerical simulations.
dc.description8 pages, postscript
dc.identifierhttps://arxiv.org/abs/cond-mat/9603125
dc.identifierhttp://arxiv.org/abs/cond-mat/9603125
dc.identifierpublished in 'The Hubbard Model: Its Physics and Mathematical Physics' (Editors: D. Baeriswyl, D. K. Campbell, J. M. P. Carmelo, F. Guinea, E. Louis), Plenum Press 1995, p. 385-392
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/27495
dc.subjectCondensed Matter
dc.titleMetal to Insulator Transition in the 2-D Hubbard Model: A Slave Boson Approach
dc.typetext

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