1/tau = A(E1 - Ef)^2 + B(Kb.T)^2, where A, B are T-independent constants.
So the scattering time tau is approximately proportional to T^2. Arguments are made in A&M that the scattering time tau depends on the interaction potential from Thomas Fermi screening: 4.pi.e^2/k_0^2.
Performing quite a rough dimensional analysis on this quantity, they get that:
1/tau ~ (Kb.T)^2 / h-bar.Ef
At room T, tau is of order 10^-10 seconds, which is 4 orders of magnitude longer than the typical scattering due to impurities. This suggests that the e-e interactions do not have a significant effect on the validity of the independent electron approximation.
it was interesting to know that Fermi liquid theory was arranged to deal with the liquid state of the isotope of helium of mass number 3. However, this theory is greatly connected to the theory of electron electron interactions in metals.(Ashcrof and Mermin,p345)
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