Let’s quickly look at quantum numbers and map them to the point potential universe.
There is a set of quantum numbers at the Bohr atom model scale, but we want to study the quantum numbers for standard model particle assemblies.
| Quantum Number h/t Wikipedia | Standard Model | Point Potential Model |
|---|---|---|
| Electric charge (Q) in units of |e|, the magnitude of the charge on the electron. | {-1, -2/3, -1/3, 0, 1/3, 2/3, 1} | {-1/6, +1/6} constant rate emitters |
| Weak isospin (T3) — relating to the electrically charged part of the weak interaction: Particles with half-integer weak isospin can interact with the W± bosons; particles with zero weak isospin do not | See mapping in chart. | |
| Baryon number (B) — strictly conserved additive quantum number of a system. Baryons (three quarks) have a baryon number of +1, mesons (one quark, one antiquark) have a baryon number of 0, and antibaryons (three antiquarks) have a baryon number of −1. | B = (quarks – antiquarks)/3 | For quarks: (* – !*)/3 * = Noether core ! = anti |
| Lepton number (L) — strictly conserved additive quantum number of a system. In a reaction, the lepton number of reactants equals lepton number of products. | L = leptons – antileptons | For leptons: (* – !*) |
| Standard Model | Point Potential Model |
|---|---|
| Strong interactions conserve all flavours | Strong interactions are those that involve coupling the polar vortices of binaries in two Noether cores. |
| Lepton flavor is not conserved in neutrino oscillation. | The neutrino is a quasi-stable assembly. The change in the neutrino geometry reveals the shielded energy of the gen II and gen III binaries. |
| Baryon number and lepton number conservation. | These quantum numbers map directly to Noether cores. |
| All flavour quantum numbers are violated (changed, non-conserved) by electroweak interactions | Electroweak interactions involve the personality potentials. These types of interactions are able open up an assembly and transform it in a reaction. |
The overall observation is that not only does the point potential geometry explain the quantum numbers, but it also provides insight into the related behaviour.
J Mark Morris : Lynn : Massachusetts
Neoclassical 