Monday, March 10, 2014

Does this theory correspond well to transitions in the standard model? (done)

 Start with wave mechanics. The sampling process always removes simultaneity by shuffling large phase variations out, and shuffling small phase variations in to the center. I work this problem assumed the system is compact, which is close for the subatomic.  Handling sparse systems with better accuracy is coming up, but I assume here that the subatomic if fairly compact and beneath the proton level I can ignore kinetic energy.

A region of very sharp peaks in phase variations works as follows.  The sampler measures zero phase near the peak of any variation, it under samples and flattens. It then measures steep variations out from the peak, which are always moved out word from the peak at Pauli rate. The peak flattens a bit more , the sample measures zero phase at the boundary of the peak, and continues measuring higher variations just out side the edge of the flattened peak.  Within a region of these peaks the process is creating standing waves, eventually the flattened regions contain half the wave variation, all zero, and there is no wave variation grater that can be packed.  The region is stable with dense pools of phase zero, and the quantization size if course, only large quantizations can pass through the peak, so the standing wave is grouped into large quantization levels, fewer quantization states.  The region will pass wave from any other longer wave without disruption, so longer wave waves superimpose in this region with pools of zero phase less than the quantization level of the shorter regions.  That is stable, no simultaneity.

Hence in the standard model, as in this model, shorter wavelength means much coarser quantization levels, and mass is proportional to the inverse of the quantization states. Short wave are of less order and massive than long wave. The Pauli sampling process insures that order N+1, longer wave, will not disrupt order N, shorter wave. But an order N+2 wave, longer cannot exist within an order N region unless it is already coded for the N+1, that is what defines order, the overlap.  The order N+2 plus the order N+1, superimposes and reach a level to disrupt the order N, causing instability.  So, in a balanced system, the orders are separated by the Pauli separation distance, the order N+2  has been removed from order N regions. At that point the compaction is done, and the standard model is known.

So, the most compact order, at the Pauil rate will have three quantization levels, and that is the measure of wavelength, short. Order N should be twice the frequency, 1/2 the wavelength of order N+1, but its not. It is 2/3 the frequency, hence 3/2 the wavelength, the Pauli ratio of wavelength. The higher order is 2/3 the wavelength of the lower order, instead of twice the quantization levels it has 1.5.

So have have as quantization levels, at the ground state, the following:




3 N
4.5 N+1
6.75 N+2
10.125 N+3
15.1875 N+4

 In this model, the Nyquist quantization levels will be twice the largest wavelength. And we see that 1/3 = .33  > 1/4.5 = .22,  no mass quantization. But 1/3 < (1/4.5 + 1/6.75)  = .37, hence quantization.

The quantization level is measured in phase as 2*pi/Nquants. The system is not at ground state, of course, as witnessed by the kinetic energy of the electron. So, the electron has electro-magnetic wave action penetrating the atob, but that generally gets sorted out at the nuclear level, and the Higgs, one or two orders below, is likely stable, it maintains its natural density level. The nuclear is too dense for stability and compact EM waves cause nuclear wave modes to leave the region and requantize two orders up.

Our region is not cooled, and magnetism has not yet pooled into mass. Its wavelength is long compared to the electron, and the quantization difference shows up in motion.  This is modelled as a static phase shift in the charge field that is very small relative to the field quantization level.  So, the mass moves to equalize phase. That is, the sampling process moves the electron slightly before the phase variation passes gains strength. We get kinetic energy when the N+1 field is very sparse and the delta change in phase per wavelength is always less than the quantization levels of the N field.

In hot regions, density, and wavelength grow at grater rates than the ground zero model would indicate. The sun is much more compact, though it is hot, it is cooler relative to total mass compacted. The magnetic energy is denser, though not yet quantized. The motion of the planets around the sun works just like the motion of the electron around the nucleus. The gravitation field is a very long wave standing wave of order N+8 or there abouts.  It comes from the original density of the disturbance measured at that distance. The roatational velocity of the planet and sun is the mild phase offset in their graviational fields.

Phase variation, then is energy.  It comes in various styles, in the phase zero mass, the wave action, and kinetic motion. Kinetic energy is another method of removing simultaneity.  As the system cools, phase excess phase variation is captured in kinetic energy, making sparse regions. Mass, wave and kinetic all measure phase variation of the original disturbance.

The electron, is very sparsely compacted, the phase variation around it has a long straight negative field, and a tightly looped positive field.  The positive end should be nearly perpendicular, then loop around the mass. Hence the magnetic field causes the positive field spiral, the induced motion an attempt to equalize the induced spiral. That is why we get spiralling particles from our accelerators.

So, in conclusion. a constant phase offset between two fields is force, causing motion. Then comes wave action, then comes mass. The three forms of phase variation that constitute the principles of physics. Quantization ratios will only be stable completely  when the system cools.

So, Bosons are waves within a quantization order. They do not have charge and the spin is assumed to be one wavelength.  The K boson is likely a standing, stable wave which can be in two forms, each form 180 radians offset from each other. The Higgs, being the shortest wavelength measurable by the Nyquist, likely has no positive/negative fields. Just a big fat quant of matter.

The phase imbalance of any quantized matter is broken into two parts, the part along the line to the center of compaction (nucleus), called charge for the electron. And the part that is at right angles to that, called spin.  We measure charge and spin relative to the electron.

Up and down refers to phase inversion, the positive phase invariance can point in or out of the center of compaction.

So I have:
Higgs with wave mode defined by the W adn K  Boson
Quarks with wave mode defined by the gluon
Electron with wave mode defined by the photon.

The quarks have gluon (order 2 ?) have wave modes with the Higgs.
The quark (Order N+1) making a photon is reall a quark decomposing into a gluon wave, entering the sparse electron field and requantizing to a form of electron. The path should be, Higgs Boson wave (Order N) plus electron order wave (N+2) making some sort of lepton.
Andd below all this is the Nyquist, having half the wavelength of the Higgs, no wave action, no matter, but can hold phase information.



The various versions of the electron defined by the various levels of unstable compactions. Same with quarks. The variable states of matter because the compaction process is not complete.

Why does this model have fractions states?

Mainly because it will be interspersed with free Nyquist layer that removes the small phase imbalance left of.  At compaction, some 33% of the region are Nyquist.
The standard model is a good job, but should be corrected a bit now that we have a real theory.

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