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Recent Developments in Non-Fermi Liquid Theory

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arxiv 1703.08172 v1 pith:D2HBLYS2 submitted 2017-03-23 cond-mat.str-el

classification cond-mat.str-el
keywords non-fermiliquidliquidsscalingtheoryfermiinteraction-drivenphysics
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Non-Fermi liquids arise when metals are subject to singular interactions mediated by soft collective modes. In the absence of well-defined quasiparticle, universal physics of non-Fermi liquids is captured by interacting field theories which replace Landau Fermi liquid theory. In this review, we discuss two approaches that have been recently developed for non-Fermi liquid theory with emphasis on two space dimensions. The first is a perturbative scheme based on a dimensional regularization, which achieves a controlled access to the low-energy physics by tuning the number of co-dimensions of Fermi surface. The second is a non-perturbative approach which treats the interaction ahead of the kinetic term through a non-Gaussian scaling called interaction-driven scaling. Examples of strongly coupled non-Fermi liquids amenable to exact treatments through the interaction-driven scaling are discussed.

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  1. Linear Resistivity from Spatially Random Interactions and the Uniqueness of Yukawa Coupling

    hep-th 2025-07 conditional novelty 6.0 of 10

    Only the two-dimensional spatially random Yukawa coupling, among all (ψ†ψ)^n φ^m scalar couplings, yields linear-in-temperature resistivity in the large-N SYK-rised framework.

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