30,640 research outputs found

    Singular Fermi Surfaces I. General Power Counting and Higher Dimensional Cases

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    We prove regularity properties of the self-energy, to all orders in perturbation theory, for systems with singular Fermi surfaces which contain Van Hove points where the gradient of the dispersion relation vanishes. In this paper, we show for spatial dimensions d3d \ge 3 that despite the Van Hove singularity, the overlapping loop bounds we proved together with E. Trubowitz for regular non--nested Fermi surfaces [J. Stat. Phys. 84 (1996) 1209] still hold, provided that the Fermi surface satisfies a no-nesting condition. This implies that for a fixed interacting Fermi surface, the self-energy is a continuously differentiable function of frequency and momentum, so that the quasiparticle weight and the Fermi velocity remain close to their values in the noninteracting system to all orders in perturbation theory. In a companion paper, we treat the more singular two-dimensional case.Comment: 48 pages LaTeX with figure

    Homogenization of the Oscillating Dirichlet Boundary Condition in General Domains

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    We prove the homogenization of the Dirichlet problem for fully nonlinear elliptic operators with periodic oscillation in the operator and of the boundary condition for a general class of smooth bounded domains. This extends the previous results of Barles and Mironescu in half spaces. We show that homogenization holds despite a possible lack of continuity in the homogenized boundary data. The proof is based on a comparison principle with partial Dirichlet boundary data which is of independent interest.Comment: Version to appear in J. Math. Pures Appl. Added Remarks 1.2 and 1.7. Removed some extraneous statements of previous results (previously Corollaries 2.7 and 2.12). Changed the statement and proof of Lemma 3.1 to fix a small error and R^{-\alpha} is now (N/R)^{\alpha} here and in later uses of the Lemma. 23 page

    A Rigorous Proof of Fermi Liquid Behavior for Jellium Two-Dimensional Interacting Fermions

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    Using the method of continuous constructive renormalization group around the Fermi surface, it is proved that a jellium two-dimensional interacting system of Fermions at low temperature TT remains analytic in the coupling constant λ\lambda for λlogTK|\lambda| |\log T| \le K where KK is some numerical constant and TT is the temperature. Furthermore in that range of parameters, the first and second derivatives of the self-energy remain bounded, a behavior which is that of Fermi liquids and in particular excludes Luttinger liquid behavior. Our results prove also that in dimension two any transition temperature must be non-perturbative in the coupling constant, a result expected on physical grounds. The proof exploits the specific momentum conservation rules in two dimensions.Comment: 4 pages, no figure
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