The state is always in some superposition..
If it is a single eigenstate of one observable, it may be in a superposition of multiple eigenstates of another observable.
If you measure an observable of a particle, its wavefunction can be said to collapse to a single eigenstate of that observable.
Before and after that, the state evolves according to how its energy depends on its position, momentum, and other observables (i.e., its Hamiltonian).
If a particular observable is a conserved quantity (commutes with the Hamiltonian), and you measure that observable, the state after measurement will always be the same eigenstate of that observable.
If the observable is not conserved (does not commute with the hamiltonian), then after a sufficient time, the state will be in a reasonable superposition of multiple eigenstates of the observable in question.
Another way of looking at it:
The uncertainty principle tells us that a particle cannot at the same time be in a single eigenstate of all ovservables.