Non-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals

A system with charge conservation and lattice translation symmetry has a well-defined filling ν, which is a real number representing the average charge per unit cell. We show that if ν is fractional (i.e., not an integer), this imposes very strong constraints on the low-energy theory of the system a...

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Autores principales: Dominic V. Else, Ryan Thorngren, T. Senthil
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Publicado: American Physical Society 2021
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spelling oai:doaj.org-article:430887a5269d4d44847dcba9800bc48e2021-12-02T14:25:40ZNon-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals10.1103/PhysRevX.11.0210052160-3308https://doaj.org/article/430887a5269d4d44847dcba9800bc48e2021-04-01T00:00:00Zhttp://doi.org/10.1103/PhysRevX.11.021005http://doi.org/10.1103/PhysRevX.11.021005https://doaj.org/toc/2160-3308A system with charge conservation and lattice translation symmetry has a well-defined filling ν, which is a real number representing the average charge per unit cell. We show that if ν is fractional (i.e., not an integer), this imposes very strong constraints on the low-energy theory of the system and give a framework to understand such constraints in great generality, vastly generalizing the Luttinger and Lieb-Schultz-Mattis theorems. The most powerful constraint comes about if ν is continuously tunable (i.e., the system is charge compressible), in which case, we show that the low-energy theory must have a very large emergent symmetry group—larger than any compact Lie group. An example is the Fermi surface of a Fermi liquid, where the charge at every point on the Fermi surface is conserved. We expect that in many, if not all, cases, even exotic non-Fermi liquids will have the same emergent symmetry group as a Fermi liquid, even though they could have very different dynamics. We call a system with this property an ersatz Fermi liquid. We show that ersatz Fermi liquids share a number of properties in common with Fermi liquids, including Luttinger’s theorem (which is thus extended to a large class of non-Fermi liquids) and periodic “quantum oscillations” in the response to an applied magnetic field. We also establish versions of Luttinger’s theorem for the composite Fermi liquid in quantum Hall systems and for spinon Fermi surfaces in Mott insulators. Our work makes a connection between filling constraints and the theory of symmetry-protected topological phases, in particular through the concept of “’t Hooft anomalies.”Dominic V. ElseRyan ThorngrenT. SenthilAmerican Physical SocietyarticlePhysicsQC1-999ENPhysical Review X, Vol 11, Iss 2, p 021005 (2021)
institution DOAJ
collection DOAJ
language EN
topic Physics
QC1-999
spellingShingle Physics
QC1-999
Dominic V. Else
Ryan Thorngren
T. Senthil
Non-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals
description A system with charge conservation and lattice translation symmetry has a well-defined filling ν, which is a real number representing the average charge per unit cell. We show that if ν is fractional (i.e., not an integer), this imposes very strong constraints on the low-energy theory of the system and give a framework to understand such constraints in great generality, vastly generalizing the Luttinger and Lieb-Schultz-Mattis theorems. The most powerful constraint comes about if ν is continuously tunable (i.e., the system is charge compressible), in which case, we show that the low-energy theory must have a very large emergent symmetry group—larger than any compact Lie group. An example is the Fermi surface of a Fermi liquid, where the charge at every point on the Fermi surface is conserved. We expect that in many, if not all, cases, even exotic non-Fermi liquids will have the same emergent symmetry group as a Fermi liquid, even though they could have very different dynamics. We call a system with this property an ersatz Fermi liquid. We show that ersatz Fermi liquids share a number of properties in common with Fermi liquids, including Luttinger’s theorem (which is thus extended to a large class of non-Fermi liquids) and periodic “quantum oscillations” in the response to an applied magnetic field. We also establish versions of Luttinger’s theorem for the composite Fermi liquid in quantum Hall systems and for spinon Fermi surfaces in Mott insulators. Our work makes a connection between filling constraints and the theory of symmetry-protected topological phases, in particular through the concept of “’t Hooft anomalies.”
format article
author Dominic V. Else
Ryan Thorngren
T. Senthil
author_facet Dominic V. Else
Ryan Thorngren
T. Senthil
author_sort Dominic V. Else
title Non-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals
title_short Non-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals
title_full Non-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals
title_fullStr Non-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals
title_full_unstemmed Non-Fermi Liquids as Ersatz Fermi Liquids: General Constraints on Compressible Metals
title_sort non-fermi liquids as ersatz fermi liquids: general constraints on compressible metals
publisher American Physical Society
publishDate 2021
url https://doaj.org/article/430887a5269d4d44847dcba9800bc48e
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AT tsenthil nonfermiliquidsasersatzfermiliquidsgeneralconstraintsoncompressiblemetals
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