Since we live in a four dimensional spacetime, I have long known that it is possible for elementary point particles to have simultaneous independent spins on two orthogonal planes, for example, one rotation axis normal to the x-y plane, and another axis normal to the z-t plane. I discovered that when combined with the R3 hypersurface we live in within the R3+T universe, the projection of dual-spin particles onto the R3 hypersurface causes a single elementary particle to appear as (for example) two or three independent particles from our point of view.
This seemed like a great way to make progress on why we have bound systems of quarks but never see isolated quarks. I recently posted on this (see https://wordpress.com/post/agemozphysics.com/1754, for example). I had hoped that this approach would allow a more analytic view of quantum quark behavior than the perturbative methods we currently use in quantum chromodynamics, why we have bound quark systems that are color-charge neutral, and why we have the SU(3) color charge behavior of quarks and gluon interactions.
Alas, I found that dual-spin doesn’t lead directly to the SU(3) solution of chromodynamics or any of the rest of it. The observation in R3 of R3+T dual-spin particles yields three identical particles (see the 3:1 dual spin ratio shown in the figure) rather than two up quarks and one down quark, and gives no hint why most of the quark combinations in real life are unstable. It doesn’t explain conservation of baryon number, the large mass of the bound quarks in a proton, or any of the other things we see in quantum chromodynamics. Nor do I see nothing that points to where the different gluon color charge pairs come into play, for that matter, why we have gluons at all.

I did a bit of research to see if anyone had looked at spins in four dimensions, or even if someone had published the fact that elementary particles in R3+T can have two simultaneous and independent spins that project onto our R3 hypersurface reality, and so far, it doesn’t look like anybody has considered this. There is no reason why a product of Pauli matrices couldn’t describe a real particle in R3+T, which I think gives the degrees of freedom we need for color charge in quantum chromodynamics. Indeed, the solution I found in the previous post listed above looks like it gives us the colors we need for quarks (red, green, blue). The fact that real-life elementary particles only have color neutral combinations (e.g., protons must have each of a red, green, and blue quark) to me hints strongly that the bound quark system making a proton is a single dual-spin elementary particle in R3+T.
So, I don’t want to give up. I still think I might be on the right track, or close to it. Do any of you agree or am I doomed to crackpot purgatory?
Agemoz