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  • Such scale arises as themost natural one since in all of these models, as already mentioned, we have that theneutrino masses vanish as the lepton-breaking scale ???? ??? 046.It is also clear that in any acceptable model one must arrange for the majoronto be mainly an SU(2) ??? U(1) singlet, ensuring that it does not affect the invisibleZ decay width, well-measured at LEP. In models where the major
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