  We address the question of whether a non-nomological (i.e., anomic)
interpretation of the wavefunction is compatible with the quantum formalism.
After clarifying the distinction between ontic, epistemic, nomic and anomic
models we focus our attention on two famous no-go theorems due to Pusey,
Barrett, and Rudolph (PBR) on the one side and Hardy on the other side which
forbid the existence of anomic-epistemic models. Moreover, we demonstrate that
the so called restricted ontic indifference introduced by Hardy induces new
constraints. We show that after modifications the Hardy theorem actually rules
out all anomic models of the wavefunction assuming only restricted ontic
indifference and preparation independence.
