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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 theory predicts several scalar fieldsdetermining masses and mixing matrices of fermions and weak bosons. The scalarfields manifest as doublets with respect to the weak charge, while they aretriplets with respect to the family quantum numbers. Since free scalar fields(mass eigen states) differ from those which couple to $Z_m$ and to$W^{\pm}_{m}$ or to each family member of each of the family thespin-charge-family theory predictions for LHC might differ from those of thestandard model.

Do we have the explanation for the Higgs and Yukawa couplings of the standard model?