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      Partially gapped fermions in 2D

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          Abstract

          We compute mean field phase diagrams of two closely related interacting fermion models in two spatial dimensions (2D). The first is the so-called 2D t-t'-V model describing spinless fermions on a square lattice with local hopping and density-density interactions. The second is the so-called 2D Luttinger model that provides an effective description of the 2D t-t'-V model and in which parts of the fermion degrees of freedom are treated exactly by bosonization. In mean field theory, both models have a charge-density-wave (CDW) instability making them gapped at half-filling. The 2D t-t'-V model has a significant parameter regime away from half-filling where neither the CDW nor the normal state are thermodynamically stable. We show that the 2D Luttinger model allows to obtain more detailed information about this mixed region. In particular, we find in the 2D Luttinger model a partially gapped phase that, as we argue, can be described by an exactly solvable model.

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          Most cited references7

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          Truncation of a 2-dimensional Fermi surface due to quasiparticle gap formation at the saddle points

          We study a two-dimensional Fermi liquid with a Fermi surface containing the saddle points \((\pi,0)\) and \((0,\pi)\). Including Cooper and Peierls channel contributions leads to a one-loop renormalization group flow to strong coupling for short range repulsive interactions. In a certain parameter range the characteristics of the fixed point, opening of a spin and charge gap and dominant pairing correlations are similar to those of a 2-leg ladder at half-filling. An increase of the electron density we argue leads to a truncation of the Fermi surface with only 4 disconnected arcs remaining.
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            Doping Evolution of the Underlying Fermi Surface in La2-xSrxCuO4

            We have performed a systematic doping dependent study of La\(_{2-x}\)Sr\(_x\)CuO\(_4\) (LSCO) (0.03\(\leq x \leq\)0.3) by angle-resolved photoemission spectroscopy. In the entire doping range, the underlying ``Fermi surface" determined from the low energy spectral weight approximately satisfies Luttinger's theorem, even down to the lightly-doped region. This is in strong contrast to the result on Ca\(_{2-x}\)Na\(_x\)CuO\(_2\)Cl\(_2\) (Na-CCOC), which shows a strong deviation from Luttinger's theorem. The differences between LSCO and Na-CCOC are correlated with the different behaviors of the chemical potential shift and spectral weight transfer induced by hole doping.
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              Interacting Electrons on a Square Fermi Surface

              A. Luther (1994)
              Electronic states near a square Fermi surface are mapped onto quantum chains. Using boson-fermion duality on the chains, the bosonic part of the interaction is isolated and diagonalized. These interactions destroy Fermi liquid behavior. Non-boson interactions are also generated by this mapping, and give rise to a new perturbation theory about the boson problem. A case with strong repulsions between parallel faces is studied and solved. There is spin-charge separation and the square Fermi surface remains square under doping. At half-filling, there is a charge gap and insulating behavior together with gapless spin excitations. This mapping appears to be a general tool for understanding the properties of interacting electrons on a square Fermi surface.
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                Author and article information

                Journal
                07 July 2009
                2010-04-16
                Article
                10.1007/s10955-010-9971-2
                0907.1277
                5ec1879b-23f6-4ce9-89c7-df52629e030b

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                J. Stat. Phys. (2010) 139: 1033-1065
                v1: 36 pages, 10 figures, v2: minor corrections; equation references to arXiv:0903.0055 updated.
                math-ph math.MP

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