You seem to think that Higgs particles are a kind of marbles that you put in a proton bag to make up its mass. It is absolutely not the case.
What happens, in fact, is that the Higgs particle is a very heavy one, but - like all particles - corresponds in fact to a quantum field.
The problem people had when they were building a quantum theory of elementary particles is that the usual way of giving a mass to a fermion, namely by introducing a term m^2 psi-dagger psi in the lagrangian, didn't work because these terms do not respect the required symmetries of the theory (this is a bit a complicated issue). However, it turned out that the introduction of a scalar particle (field), that was subject to a funny potential such that in the ground state (lowest energy) the field values would NOT be 0, could solve several problems. Indeed, the non-zero value of that field, coupled with an interaction term between that field and, say, the electron field, gave a term in the lagrangian which DID respect the symmetries required, but mimicked, at low energies, as a term that was essentially the same as a mass term.
It also solved another problem: there were 2 theorems in quantum field theory that made life hard. The first one was by 't Hooft, and said that if you want to have a renormalizable (calculable) theory, your interactions need to be described by fields such that the lagrangian obeys, what is called, a gauge symmetry. The problem with a gauge symmetry was that gauge particles have to be massless. People tried to find tricks around it, but Goldstone proved an annoying theorem (Goldstone's theorem), that said that you always have to have massless particles associated with the degrees of freedom of a gauge symmetry, the socalled "goldstone bosons". As these were not observed, that was annoying.
And then the Higgs mechanism was invented. It gave terms that mimicked mass to the gauge particles, it eliminated the goldstone bosons and gave, by its interactions, a mimicked mass term to the fermions.
cheers,
Patrick.