Corrigendum to "The effective chiral Lagrangian for a light dynamical "Higgs Particle" " [Phys. Lett. B 722 (2013) 330 335]
can be reduced to a combination of P6(h) P18(h) and P21(h) P23(h) respectively, plus a term that can be absorbed in the redefinition of the couplings of the gauge bosons and h, plus a term containing a dependence on the Yukawa couplings. When fermion masses are considered, these operators are redundant; otherwise they are independent and must be taken into consideration. We profit from this erratum to point out another fact, although it has no impact on the basis. The equations of motion for the gauge fields and the Dirac equation in the section Massive fermions: DmV 0 must be substituted by DWmn j i g 4 v2 Tr[Vns j]FC (h) g 2 Q Lgns j Q L, Bmn i g 4 v2 Tr[TVn ]FC (h) g' i=L,R Q ignhi Q i,