A two-Higgs doublet model with a discrete symmetry acquires, in its scalar and gauge sectors, an accidental continuous symmetry. One therefore finds, after spontaneous symmetry breaking of those symmetries, that a massless pseudoscalar arises, as expected by Goldstone’s theorem. In the fermion sector, however, it is possible to obtain Yukawa matrix textures which distinguish between the and symmetries, so one expects loop corrections to originate a non-zero pseudoscalar mass for the case. We perform an explicit calculation that shows that at one-loop the pseudoscalar remains massless for all but one tested Yukawa matrices. The pseudoscalar mass thus found is highly suppressed by the hierarchy of fermion masses.

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