Computation of the Masses of Other Hadrons and of the Exact Neutrino Masses

In Chaps. 5 and 6 we have examined structures of hadronsHadrons and bosonsBosons which contain only the heaviest neutrinosNeutrino types, i.e. ν3 type neutrinos which correspond to relatively stable rotating states, while in Chap. 2 we have examined the dramatic role (electromagnetic radiation) of the lightest neutrino type ν1. Here we use these light neutrinos to form bound states which are eventually the so-called mesonsMesons. From these results a third, intermediate, mass labeled m2, has emerged which is proven to be the geometric mean of m1 and m3.