Neutrino Oscillation: Charged Neutrinos

Larson was puzzled by the charged neutrino, because the charge for a material neutrino was in space, acting as though the magnetic rotating system had the rotational vibration rather than the electric rotation (which, being in space, would have its charge in time).

The concept of vibration in RS2 differs from Larson's work in the respect that vibration occurs from the compounding of motion, it just isn't "there" as it is in the RS. In order for a neutrino to become charged, it would have to capture the necessary motions to impart a vibrational component to its motion.

Therefore, the muon neutrino, M ½-½-0 would need to capture a charged electron, 0-0-(1)*, which has its charge in time. The composite motion would have the dimensions of the electron neutrino, M ½-½-(1)*, since the charge was necessary to trap the electron in the time of the muon neutrino rotation ("time" of rotation to "time" of charge does not constitute motion).

As determined with charged electrons, the vibration of the photon upon the rotation of the electron creates a 1-dimensional, rotational vibration. So logically, the rotational vibration of the electron would impart a rotational vibration to the magnetic component of the neutrino. The magnetic rotation, being 2-dimensional, would create a 2-dimensional, or "solid", rotational vibration.

The natural unit of 1-dimensional rotation is π radians. Thus, a 1-dimensional rotational vibration moves from 0 ⇒ π, then π ⇒ 0. When plotted on the Argand diagram, the spatial component oscillates between +1 and -1, completely skipping the imaginary axis--just what you would expect of a simple, harmonic motion.

But the solid, 2D rotation is 4π radians in "circumference", not the customary 2π (it takes 4π rotation to complete a revolution). This means that when a charged electron imparts its rotational vibration upon the neutrino, it will take a periodic, 4-phase appearance running from 1+0i, 0+1i, -1+0i, 0-1i ...  which will be viewed as π/2 steps across the real axis: +1, 0, -1, 0, ... .

In the uncharged state, there are three neutrinos: electron, muon and tau:

M ½-½-(1) -- uncharged, electron neutrino

M ½-½-0 -- uncharged, muon neutrino

M ½-½-1 -- uncharged, tau neutrino

But the situation changes in the CHARGED state. The basic rotation, the muon neutrino of ½-½-0 captures a charged electron, or an electron neutrino ½-½-(1) becomes charged, it causes the muon to being oscillating between +1, 0 and -1. The resulting motion has three different rotational combinations, that appear in sequence (remembering that conventional science can only observe and measure the REAL axis):

[RV² = -1 + 0i] M ½-½-(1) -- charged, electron neutrino

[RV² = 0 - 1i] M ½-½-0 -- charged, muon neutrino

[RV² = +1 + 0i] M ½-½-1 -- charged, tau neutrino

[RV² = 0 + 1i] M ½-½-0 -- charged, muon neutrino

In the CHARGED state, the neutrino does not appear as ONE particle, but THREE, depending on WHEN you measure it. This is referred to as neutrino oscillation, triggered by the 2-dimensional, rotational vibration that constitutes the magnetic charge.

Conclusion

1. Uncharged neutrinos always look like the particle they are, so there are three different flavors.
2. Charged neutrinos look like ALL three flavors, so depending on how and when you measure them, you could get either an electron, muon or tau neutrino.
3. The charged neutrino is observed as "neutrino oscillation"; the uncharged neutrinos are observed as stable particles.