(T+, p+)
(p+)
(g+, T+, p+)
(T+, p+, g+) and (T+, p+, g+, T+)
(p+, g+) and (p+, g+, T+)
(g+, T+, p+, g+) and (g+, T+, p+, g+, T+)
the spins of p+ particles do not contribute to the mass of the nuclei, only the presence of g+ particle. In which case, hydrogen isotopes have zero mass, mass of one g+ and the mass of two g+. The relative abundance of these stable isotopes give rise to the decimals in hydrogen mass that can not be factored.
The notion of p+ having mass g+ is the result of having to add the tuple (g+, T+, p+) to any nucleus ending with a p+ particle in the cyclic permutation set. The tuple must contain a g+ particle. Such an array of stable isotopes with different positions of p+ in the nucleus may also add to the decimal points in experimental isotope mass measurements, if the weak g field generated by the spinning p+ particles also contribute to mass. What about spins? Spins seem to be associated with g+ particles only.
Unstable nuclei are not any members of the cyclic permutation set. For example,
(3g+, T+, p+)
(T+, p+, 3g+) and (T+, p+, 3g+, T+)
(p+, 3g+) and (p+, 3g+, T+)
are all Hydrogen-3, 3H with spin 12+; the group 3g+ spins as one. What about 3H with 2− spin?
What is g+ and how can it transmute to a charge?
The time axes, tg and tc of a g+ particle swapped. The result is an electron that leaves the nucleus; β− decay.
How does such a swap occurs? 'Til next time...