Why do we have to introduce quasiparticles in the Fermi liquid theory Why is it necessary in Fermi liquid theory to introduce quasiparticles? I understand the notion of system where someone can turn on the interactions slowly (i.e., adiabatically), but I do not understand why there is any difference between a Fermi liquid and a system with just "normal" electrons when the interaction is not turned on adiabatically.
 A: When Lev Landau first derived the Fermi liquid, he defined it as a many-body system of interacting electrons whose interacting eigenstates can be adiabatically connected to the eigenstates of the Fermi gas. In other words, Landau defined the eigenstates of the Fermi liquid as having a one-to-one correspondence with the eigenstates of the non-interacting system. It is for this reason that we can write down the free energy as
$$
\delta F=\frac{1}{V}\sum_{k}(\epsilon-\mu)\delta n_k+\frac{1}{2V}\sum_k f_{kk'}\delta n_k\delta n_{k'}
$$
where $\delta n_k=n_k-n_k^0$, where $n_k$ is the distribution function of the interacting system and $n_k^0$ is the distribution of the non-interacting system. If there are no quasiparticles, this entire description fails by definition. The advantage of this is that we can define a lot of the thermodynamics of the interacting system with nearly the same formalism as the non-interacting case, except with re-defined parameters. For example, in a Fermi liquid, the quasiparticles have a mass $m^*$ that can be related to the bare electron mass via 
$$
\frac{m^*}{m}=1+\frac{F_1^s}{3}
$$
where $F_1^s$ is the $\ell=1$ channel of the symmetric Landau parameter after I expand the free energy in terms of spherical harmonics. 
Another way to see this is by looking at the quasiparticle weight, $Z$:
$$
Z=\left(1-\frac{\partial \Re \Sigma}{\partial \omega}\bigg|_{\omega=0}\right)
$$
where $\Re \Sigma$ is the real component of the fermionic self energy. If $0<Z<1$, then I have a finite quasiparticle lifetime. If $Z\rightarrow 0$, then I have an interacting fermionic system without well-defined quasiparticles. One example of such a model is a strange metal, which is a metallic state which lacks a quasiparticle description.
