As a person majoring in condensed matter physics, I frequently encounter Landau Fermi-liquid theory. Almost every literature says that the concept of the adiabatic continuity (to the non-interacting ground state) is the heart of the theory so that the notion of a $\it{quasiparticle}$ is well-defined. For the practical aspect, the energy of the electronic system (relative to that of the ground state) is given in Landau Fermi-liquid theory as $$E[\delta n_\vec{k}]=\sum_{\vec{k}}\varepsilon_{\vec{k}}\delta n_\vec{k} + \frac{1}{2}\sum_{\vec{k}\sigma,\vec{p}\sigma'}f(\vec{k}\sigma,\vec{p}\sigma')\delta n_{\vec{k},\sigma }\delta n_{\vec{k},\sigma'},$$ where $\delta n_\vec{k}$ is the deviation of the distribution of the $\it{quasiparticle}$ from the value at the ground state.
What makes me astnonished is that the energy functional is just expressed with classical functions $\delta n_\vec{k}$ rather than quantum-mechanical operators. Could I or we say that the Landau Fermi liquid theory a classical theory?
Also, why (or how) could (or should) an interacting ground state of a Fermi liquid be completely or well described by $\delta n_\vec{k}$? Is this feature associated with the adiabatic continuity?