ChrisVer said:

do you have a reference about this procedure?.
Do you have any book on supersymmetry?
Well, for instance, Terning's. In the page 9, first line: "The massive vector multiplet... which corresponds to two Majorana fermions, a massive vector (spin 1) and a real scalar".
Of course, the massless vector multiplet has just the massive vector and one majorana fermion, the gaugino.
But if you want to have supersymmetry AND massive gauge fields, you must add to each gauge supermultiplet another Majorana fermion and a real scalar.
So any extension of the standard model where we restore susy but we keep the SU(2)xU(1) symmetry broken, which we could in principle do if susy breaking is independent of electroweak symmetry breaking, should have at least three extra real scalars, for the multiplets of Z0, W+ and W-.
EDIT: I am not sure if it contains or not the Higgs sector, but I guess that any Higgs sector will just include this three scalars, as surely when the massive gauge multiplet becomes massless it will produce a separate chiral multiplet with the extra Majorana, the extra scalar, and other scalar corresponding to the degree of freedom "eaten" by the massive spin 1 vector field. So it looks to me as a higgs.
I would be surprised if someone could exhibit a model extending the SM and not containing this three scalars, and their corresponding chiral supermultiplets. Because of it, I say that this "SSM" is the most minimal. The only way to avoid is is to build a model where susy breaking and electroweak breaking are retorted in a way such that you can not manipulate the langrangian parameters to restore susy and keep at the same time the electroweak bosons massive.