It is worth pointing out that the derivative needs to be covariant in order for the Lagrangian to be gauge invariant. The covariant derivative also contains a coupling to the gauge fields, which gives the minimal coupling of the fermions to the gauge fields.
I would add that this particular type of interaction term are Yukawa couplings. It would also be more appropriate to say that the spontaneous symmetry breaking occurs in the gauge sector and does not necessarily have anything to do with the Yukawa couplings to fermions. However, upon SSB, the Yukawa couplings give rise to mass terms for the fermions.
This is what the thread level indicator is for. In this case the A would mean that the reader has an understanding of the topic at graduate student level or higher. I believe the OP has used it incorrectly. (It is supposed to reflect the OP's level of knowledge, not the level of the topic itself.)
It is worth pointing out that the gauge part contains both kinetic and self-interaction terms for all gauge fields.There are no ghosts included here. They appear once you look at gauge fixing and integrating out the redundant degrees of freedom that comes with gauge transformations.Indeed, as stated in #2, there are no neutrino masses in the standard model and consequently not in your Lagrangian.