Wednesday, June 18, 2014

Computing progatation functions

I recommend we don't, mainly we need only determine the quant sequence in the digit systems of each body. Motion of a unit circle is simply the quantized change in its surface shape, which I know nothing about at the moment.  But that motions should go as fourth order, I think, though do not quote me.

After the quant sequence is determined, just go though some calculation on baud rate relative to any other baud rate and we have propagation. In our case, Higgs is the baud rate.

Motion and Compton Bandwidth

If we define Compton bandwidth as the ratio of Nulls to phase in the unit circle, then we have a definition of mass.  Mass being the resistance to motion, and it increases as the third moment of that ratio. The more internal phase imbalance that is tolerated, the more spherical the body remains and the less motion.  Wave shift raises the quantization ratio of wave and makes the unit circle larger.

Here the hyperbolic and trig functions are multiplied by root(2).

But why would there be a higher null/phase ratio as a result? Because of this:
r^2 = r+2. Two units of separation with two degrees of freedom with the large quants. Larger separation between wave quants, inside the unit circle,  means less interference.


The quarks have 4 to 10 times the mass of the electron, and over all, three have about 21 times the mass of the electron.  The gluon brackets the bandwidth of the whole system, but likely has three quants of spectrum of the form, 1/f and f.  But they are really functions of the action in the three quarks. So the quarks are wide band. So somehow the system has managed to dump much of the quark phase into the orbitals and into the gluon. The wave shift for the quarks seems larger, and it seems they have a different cubic root system then the electron.


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