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Physics Letters A

Renormalization of elementary excitations of the 2D t-J model at moderate doping

A. Sherman

Published Jan 1, 1995• 2 citations
Publisher
DOI
10.1016/0375-9601(94)00975-u

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The two-dimensional Hubbard model is studied within the composite operator method (COM) with the electronic self-energy computed in the self-consistent Born approximation (SCBA). The main idea of the COM is to describe interacting electrons in terms of the composite elementary excitations appearing in the system owing to strong correlations; the residual interactions among these excitations are treated within the SCBA. By analysing the spectral function A(k,ω) on varying the filling, we find, at high doping, the ordinary Fermi-liquid behaviour of a weakly interacting metal and, at low doping, the opening of a pseudogap, as reported for cuprates superconductors.
We calculate the charge compressibility and uniform spin susceptibility for the two-dimensional (2D) Hubbard model slightly away from half filling within a two-loop renormalization group scheme. We find numerically that both those quantities flow to zero as we increase the initial interaction strength from weak to intermediate couplings. This result implies gap openings in both charge and spin excitation spectra for the latter interaction regime. When this occurs, the ground state of the lightly doped 2D Hubbard model may be interpreted as an insulating spin liquid as opposed to a Mott insulating state.