Wavefunction vs Quantum Field (Conceptual Approach) I'm trying to understand the connection between the wavefunction and a quantum field, so I wanted to know if my reasoning was in the right track (this is a more mathematical/conceptual approach, and it could be useful for others studying QFT)
Let's consider, for example, a system of N particles in 3D space, and examine the differences between the description by a wavefunction and a quantum field.
Wavefunction
¤ We have a total of 3N arguments (3 for each direction) that characterize the value of the wavefunction in position space $\psi(\vec{x})$
¤ The wavefunction is, mathematically, just a continuous function with (at least) first order derivatives that can satisfy boundary conditions.
¤ Given a definite momentum $\vec{p}$ of one particle, we cannot specify the value of the wavefunction for each point in space (because of the uncertainty principle).
¤ The wavefunction completely describes the evolution of the system and allows the calculation of observables that come from operators applied to it
Quantum field
¤ We have infinite degrees of freedom, so we technically have infinite arguments to describe the system (I'm not sure if this is true or we also have 3N arguments).
¤ The quantum field can be seen as an operator-valued distribution (in terms of creation and anhiquilation operators); each particle corresponds to a Fourier mode of oscillation of the quantum field.
¤ Given a particle with momentum $\vec{p}$ we can specify the value of the field $\phi(x)$ in each point (since we can just do a Fourier transform of a given oscillation mode). Does the uncertainty principle apply here?
¤ The quantum field doesn't describe one particle per-se, but the excitations in each point of some "fluid" that permeates all the space, each excitation corresponding to one possible particle.
Do you think these differences are correct? Should I add anything else?
 A: 
We have a total of $3N$ arguments (3 for each direction) that
  characterize the value of the wavefunction in position space
  $\psi(\mathbf{x})$

For a single particle, it easy to think of the (coordinate space) wavefunction $\psi(\mathbf{x})$ as 'living' in position space but for $N \gt 1$ particles, it's clear that the wavefunction $\psi(\mathbf{x}_1,\mathbf{x}_2,\cdots,\mathbf{x}_n)$ lives in a $3N$ dimensional configuration space

Given a definite momentum p⃗  of one particle, we cannot specify the
  value of the wavefunction for each point in space (because of the
  uncertainty principle).

This isn't correct.  For example, the wavefunction for a single particle with definite momentum $\mathbf{p}$ is $\psi_\mathbf{p}(\mathbf{x}) = e^{\frac{i}{\hbar}\mathbf{p}\cdot\mathbf{x}}$ which has a definite value at each point in space.

We have infinite degrees of freedom, so we technically have infinite
  arguments to describe the system (I'm not sure if this is true or we
  also have $3N$ arguments).

A quantum field is a function of spacetime, i.e., it assigns an operator to each event in spacetime so the are four arguments, the coordinates of an event

each particle corresponds to a Fourier mode of oscillation of the
  quantum field.

For a free (non-interacting) field, a particle with definite momentum is the quanta of a single Fourier mode.  But there are one particle states which are a superposition of one-particle states from different modes

Given a particle with momentum p⃗  we can specify the value of the
  field $\phi(\mathbf{x})$ in each point (since we can just do a Fourier transform of
  a given oscillation mode). Does the uncertainty principle apply here?

The quantum field $\phi(\mathbf{x})$ doesn't have a value at each point.  Remember, $\phi(\mathbf{x})$ is a field of operators.  The operator $a^\dagger(\mathbf{p})$ creates a particle with definite momentum $\mathbf{p}$ and we can express $a^\dagger(\mathbf{p})$ in terms of operator field $\phi(\mathbf{x})$ via an inverse Fourier transform

The quantum field doesn't describe one particle per-se, but the
  excitations in each point of some "fluid" that permeates all the
  space, each excitation corresponding to one possible particle.

The ontology of quantum fields isn't settled
