What's the difference between a Luttinger surface and a Fermi surface?

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SUMMARY

The discussion clarifies the distinction between the Luttinger surface and the Fermi surface, emphasizing that while they are related concepts, they are not equivalent. Luttinger's Theorem allows the application of the Fermi surface concept to interacting electrons, despite the complexities introduced by Coulomb interactions. The conversation highlights the challenges of understanding these concepts without a background in quantum mechanics (QM) and suggests that Luttinger's work provides a framework for discussing k-space in the context of interacting electrons.

PREREQUISITES
  • Understanding of Luttinger's Theorem
  • Familiarity with the concept of Fermi surfaces
  • Basic knowledge of quantum mechanics (QM)
  • Awareness of Coulomb interactions in quantum systems
NEXT STEPS
  • Research Luttinger's Theorem in detail
  • Study the implications of Coulomb interactions on electron behavior
  • Explore the concept of k-space in quantum mechanics
  • Investigate resources that explain quantum mechanics without requiring prior knowledge
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Students and researchers in condensed matter physics, particularly those interested in electron interactions and quantum mechanics, as well as anyone seeking to understand advanced topics in solid-state physics.

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I'm trying to learn about Luttinger's sum rule, but I haven't taken QM yet, and the papers on the topic are very difficult to understand without it. However it seems qualitatively like the Luttinger surface is equivalent to the Fermi surface. If this is not the case, what's the difference? Does anyone know of a source of information on the topic that can be understood without QM?
 
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What I gather from Wikipedia: Luttinger's Theorem says the concept of a Fermi Surface can be applied to interacting electrons. Electrons, as you know interact via a 1/(r-r') Coulomb interaction. That makes the quantum problem extremely difficult to solve. Nevertheless, due to screening and other reasons it is often assumed the electrons are not interacting with each other. This leads to the picture of states in k-space that get filled up to form the Fermi surface. It's not a priori clear you can adapt such a picture for interacting electrons. Luttinger showed, that with properly defined quantities, you can still talk about k-space and a Fermi surface and that the same filling law applies.
 

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