Phase diagrams, 2D Fermi Flashcards
Landau fermi liquid
3 types of degenerate fermi liquids in nature
Electrons in metals
Neutron stars
Liquid 3He
Electrons in solids versus 3He
Phase diagram of 3He vs 4He
Clausius-Clapeyron
Minimum in 3He melting curve
degenerate fermi gas
Its pressure derives almost exclusively from pauli exclusion principle. The temperature that defines this is the Fermi temperature.
3He effective mass
How well does liquid 3He fit degenerate fermi gas picture?
The answer is, at least on a qualitative level, remarkably well. At sufficiently low temperatures the heat capacity is linear in T, and the magnetic susceptibility is temperature independent (Pauli susceptibility).
Heat capacity c= γT at the lowest temperatures but γ >> γ0 (ideal gas value)
These enhancements in the low temperature heat capacity are strongly pressure dependent. The effective mass increases with pressure. m*/m increases from 2.8 at p=0 to 5.9 at the melting curve
mag susceptibility χ is also enhanced by this effect, but its enhancement is higher than that of γ . A scaling of density of states in not sufficient to account for both observations It is the interactions between the helium quasiparticles that is responsible for the additional enhancement of χ (see later).