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The spin-charge-family theory offers a possible explanation for theassumptions of the standard model, interpreting the standard model as its lowenergy effective manifestation. The standard model Higgs and Yukawa couplingsare explained as an effective replacement for several scalar fields, all ofbosonic (adjoint) representations with respect to all the charge groups, withthe family groups included. Assuming the Lagrange function for all scalarfields to be of the renormalizable kind, properties of the scalar fields on thetree level are discussed. Free scalar fields (mass eigenstates) differ fromeither those, which couple to $Z_m$, or to $W^{\pm}_{m}$ or to each familymember of each of the four families, which further differ among themselves.Consequently the spin-charge-family theory predictions differ from those of thestandard model.

How many scalar fields there are and how are they related to fermions and weak bosons in the spin-charge-family theory?