In post 24, juanrga already points out that fields are not more fundamental than particles. So while it is useful to think of particles as excitation of fields, and indeed the one particle states of a particle at a position x in QM can be written as |x>=\psi (x) |0>, where |0> is the vacuum state and \psi (x) is the field at point x. That is, when a field operates on the vacuum, it creates a particle at point x.
Perhaps your confusion is that you are thinking of a particle in the traditional sense, that is a infinitely small billard ball with a definite position. In field theory, particles are really irreducible representations of the Poincare group and some gauge groups (U(1), SU(2), etc.). I like to think of them as little chunks of the symmetry of our universe, but maybe this is not entirely correct. That is, to me the universe has some symmetry, and particles are the simplest form of how the symmetry manifests itself.