1. Choice of relevant degrees of freedom. A beautiful example is the coexistence of collective and single-particle degrees of freedom. In nuclear physics these are the rotation (vibration) and single-nucleon motion. In hadron physics we have chiral dynamics (mesonic field) interacting with quarks (analogously as phonons interacting with polarons).
2. Fine tuning of natural constants. If masses of elementary particles
and interactions between them were slightly different,
life would not be possible. Many body effects often enhance such features.
I shall present many picturesque examples.
3. Comparison of the shell structure in atoms, nuclei hadrons. Are three
"generations" of quarks and leptons also some
kind of shell structure.