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arXiv:cond-mat/0007020 · Solid State Communications

Exact ground state of the two-dimensional Hubbard model at half-filling for U=0+

Michele Cini, Gianluca Stefanucci

Published Feb 1, 2001• 3 citations
arXivHTMLPDF
DOI
10.1016/s0038-1098(00)00504-4

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We investigate the ground state of the Kondo-Hubbard model employing the recently introduced idea of spin-reflection positivity. It is shown exactly that the Kondo-Hubbard model for J<0J<0J<0 and U>∣J∣/4U>|J|/4U>∣J∣/4 at half filling has a unique ground state which can be ferromagnetic or singlet according to the lattice structure. In particular, for the Kondo lattice with U>∣J∣/4U>|J|/4U>∣J∣/4, the ground state is a singlet. We also show a theorem for the Kondo-Hubbard model with the anisotropic antiferromagnetic coupling ${J}_{\ensuremath{\perp}}>0$ and ${J}_{z}\ensuremath{\le}0$ for U>∣Jz∣/4U>|{J}_{z}|/4U>∣Jz​∣/4.
Working on a square lattice with an even number of sites N2{\mathit{N}}^{2}N2 and assuming a smooth connection between strong and weak coupling, we show that the ground state of the two-dimensional half-filled Hubbard model has momentum kx{\mathit{k}}_{\mathit{x}}kx​-ky{\mathit{k}}_{\mathit{y}}ky​=0, it is even under reflections, and transforms as an s wave under rotations when N/2 is even and as a d wave when N/2 is odd.