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Springer eBooks

Non-perturbative solutions to the Hubbard Model

Henry L. Neal

Published Nov 13, 2005• 0 citations
Publisher
DOI
10.1007/bfb0020697

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We use resurgent analysis to study non-perturbative aspects of the one-dimensional, multicomponent Hubbard model with an attractive interaction and arbitrary filling. In the two-component case, we show that the leading Borel singularity of the perturbative series for the ground-state energy is determined by the energy gap, as expected for superconducting systems. This singularity turns out to be of the renormalon type, and we identify a class of diagrams leading to the correct factorial growth. As a consequence of our analysis, we propose an explicit expression for the energy gap at weak coupling in the multi-component Hubbard model, at next-to-leading order in the coupling constant. In the two-component, half-filled case, we use the Bethe ansatz solution to determine the full trans-series for the ground state energy, and the exact form of its Stokes discontinuity.
The primary aim of this thesis is to understand the effects of electronic frustration generated by local interactions of the Hubbard U type on a lattice. Specifically we attempt to study the strongly interacting liquid phase of the Hubbard model and the so called extremely correlated phase of the t-J model without any broken symmetries. Of particular interest is the fate of the Fermi Liquid state under the influence of a large U. Exact solutions in solvable limits inform most of the physical intuition. Perturbative methods such as an infinite order calculation in the particle-particle channel ladder expansion yield fruitful results. Finally the non-perturbative field theory of Schwinger is used to generate a calculation scheme for the Green's function of the non-canonical Fermions of the t-J model. Numerical results are compared with important experimental results from the high-Tc Cuprate compounds.