Abstract

where On= ya(1 + Ys) and G is the Fe rmi coupl ing constant . Thcn the charged and neut ra l -cur ren t processes are universa l ly unders tood f rom these p r imary in teract ions (1) and f rom the s t ruc ture of e and ~. Fur the rmore , we can na tu ra l ly in t roduce two new composi te s tates which are possibly assigned to the heavy leptons, E + = (%r and M + = (var In the present note we would like to ex tend this scheme to include hadrons. There are two possible ways to include quarks which can restore the C,~bibbo theory at low energies. One is based on the hadronlep ton correspondence (2):

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