Which particles does the Higgs Field give mass to? I have found contradictory information about this. Does the Higgs field give mass only to the $W^+$, $W^-$, and $Z^0$ bosons or does it give mass to other particles as well?
 A: The Higgs field is coupled to the fermions (quarks and charged leptons) in the standard model via Yukawa couplings. As a result of the Higgs mechanism, the Higgs field then gives mass to these fermions, in addition to the weak bosons.
A: 
The Higgs Field gives mass to :-

*

*Everything marked in purple i.e. the quarks and anti-quarks

*Everything marked in green i.e. leptons and anti-leptons, which includes electrons, positrons, tau-particles, neutrinos etc.

*The yellow marked particle i.e. Higgs Boson, an excitation of the Higgs Field

*The orange-red marked particles, except for 2 (photon [$\gamma$] and gluon [$g$])

A: In the Standard Model, the Higgs field also gives mass to the six quarks (up, down, strange, charm, top, bottom) and the three charged leptons (electron, muon, tau) through Yukawa couplings. Some related mechanism may give neutrinos a small mass. (They’re massless in the Standard Model, but we know this is wrong.) Finally, one can argue that the Higgs field gives the Higgs boson its mass.
In short, every elementary particle except neutrinos gets its mass from the Higgs field. We’re not sure yet how neutrinos get theirs.
A: The Higgs field $\phi$ undergoes spontaneous symmetry breaking$^\dagger$ (from a complex doublet to a real scalar field, whose quantum is the Higgs boson) in a process named the Higgs mechanism. $^\dagger$: well it's a local/gauge symmetry, not global, so it's not "real" SSB, hence the different name "Higgs mechanism".
This has two consequences:

*

*the gauge bosons $W^\pm$ and $Z^0$ acquire a mass term, which they couldn’t have had a priori without breaking gauge invariance. The mass depends on the VEV (vacuum expectation value) of the Higgs field, but it doesn’t arise from a direct interaction term (see below) between the Higgs field and the gauge bosons. This new mass mode is the “would-be” Goldstone boson associated with the breaking of the Higgs field symmetry.
(By “no direct interaction term” I mean that the term containing a product between the gauge boson and the Higgs field is hidden in the gauge covariant derivate $D^\mu$.)


*the fundamental fermions (quarks, leptons, but not neutrinos) also acquire a mass term. This arises from a direct interaction term between the fermionic field $\psi$ and the Higgs field, called the Yukawa Lagrangian sector. This looks like $ \mathcal{L}_Y \propto \Gamma \bar L \phi R, $ where $\Gamma$ is the Yukawa coupling to the specific fermionic field $\psi$, and $L$ and $R$ are the left- and right- handed components of $\psi$. Neutrinos have no right-handed partner so they cannot gain mass through a Yukawa coupling.
So the Higgs field is responsible for the masses of all the elementary particles (including the Higgs boson) short of neutrinos.
A: The Higgs field gives mass to all fermions and three weak gauge bosons (and itself) in the Standard Model. The masses of the fermions are proportional to their Yukawa couplings.
The Yukawa couplings of the neutrinos were long neglected due to their small size, and sometimes assumed to be zero. Although the evidence is consistent with nonzero neutrino Yukawa couplings, there are Standard-Model extensions where fermions also have Majorana masses. Such masses for the neutrinos have not yet been ruled out by experiment, which means we cannot be certain the neutrino Yukawa couplings are nonzero.
