Consider a random, all to all, complex fermion hopping model on $N$ sites with quenched (Gaussian) disorder, that has a well defined large $N$ limit (aka the SYK2 model). So, we start with free fermions in this model and after disorder averaging we lose the quasiparticles in this model. Is there a nice physical way to understand this result? Or should this simply be taken as a mathematical consequence of the Schwinger Dyson equations and that's all there is to it?
Example/Reference: Look at equation A3 on page 25 in this paper.