Quasiparticle dispersion of the t-J and Hubbard models

Abstract

The spectral weight $\mathrm{A}(\mathbf{p},\omega )$ of the two dimensional $\mathrm{t}-\mathrm{J}$ and Hubbard models has been calculated using exact diagonalization and quantum Monte Carlo techniques, at several densities $1.0\le ⟨\mathrm{n}⟩\le 0.5$. The photoemission $(\omega <0)$ region contains two dominant distinct features, namely a low-energy quasiparticle peak with bandwidth of order J, and a broad valence band peak at energies of order t. This behavior $persists$ away from half-filling, as long as the antiferromagnetic (AF) correlations are robust. The results give support to theories of the copper oxide materials based on the behavior of holes in antiferromagnets, and it also provides theoretical guidance for the interpretation of experimental photoemission data for the cuprates.

arXiv comment(minor changes) RevTeX, 4 figures available on request

References in corpus (3)

• Correlated Electrons in High Temperature Superconductors
• Validity of the rigid band picture for the t-J model
• Spin bags in the doped t-J model

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