How Do Landau Levels Function in Solid State Band Theory?

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Landau levels represent quantized energy levels of electrons in a magnetic field, crucial for understanding solid state physics. In band theory, these levels arise from the Hamiltonian of electrons interacting with a vector potential, resembling a harmonic oscillator to derive eigenvalues. The de Haas-van Alphen effect links the oscillation period to the extremal orbit of the Fermi surface, highlighting the relationship between electron density and the Fermi surface volume. In metallic systems modeled as a free electron gas, interactions lead to long-lived quasiparticles that behave similarly to free electrons, despite renormalized properties. The semiclassical model illustrates electrons in cyclotron orbits, drifting under an electric field, further elucidating Landau levels' significance in solid state phenomena.
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Landau level is the energy levels of free electron gas in a magnetic field. However, this term is also frequently used in solid state physics. I have the following questions:
1. what does this term exactly mean in band theory? After all, electrons are not free here.
2. why is de Haas-van Alphen period related to extremal orbit of the Fermi surface?
 
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A lot of metallic systems can be modeled as a free electron gas. If they have a certain type of interactions they can be classified as Fermi liquid meaning there are long lived quasiparticles near the surface. The volume enclosed by the FS is proportional to the electron density. The charge, spin and momentum of the electrons remain the same but other quantities are renormalized. So basically the quasiparticles behave like free electrons.

Landau levels are obtained from the Hamiltonian of electrons coupled to a vector potential. It turns out you can manipulate the expression to make it look like a harmonic oscillator to obtain the eigenvalues.

A semiclassical picture in 2d (like the QHE) has the electrons in cyclotron orbits with the radius eB/m. The centers drift in an E field.
 

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