Kinetic energy, simultaneity and measurable dimensions

In this model, any complete sequence that minimizes the phase to Nyquist creates a point source model. The least relative  dense packing is the vacuum to the shortest end of the spectrum. It defines the point. The Boson and proton orders are mixed and highly dense, unstable to us, and provide no measurement. But the electron is less dense and allows us a measurement in terms of electron wave length. The magnetic dens, the gravitation less dense and we get three dimensional measurements, along which we can measure kinetic energy.

Less dense, stable spectra has simultaneity, or kinetic energy.

What happens when we sort out the boson proton world? We get an extra dimension.  That dimension appears because we can now create the proper standard model of the proton/boson world relative to the other three dimension. No matter where we are in the gravitational world, we can rescale the proton/boson fields in at that point, and thus rescale the other measurements.
For example, we can measure the distance to the nearest start assuming the vacuum is phase consistent along the gravitational line.  But if our knowledge of the proton/boson barrier is much greatly improved, then we get a better measurement of the curvature of the gravitational line between the stars. We get a better model of the standard model at that star and at our star. We measure in four dimensions.

The total amount of kinetic energy in any sequence is the phase variation of the vacuum above Nyquist. When completing the model of the atom, we know we have kinetic energy along concentric spheres, and along. We see this in the point source model in which is phase is not equalized across the sequence after the vacuum is removed. The total phase variation along the sample is greater than Sub sampling noise. When that happens in the sequence we can take on chunk (unseparated) of vacuum and place it at that point to represent simultaneity, and bring the SNR back to sub sampling. The imbalances in total phase along the sequence, absent vacuum, are the kinetic energy modes.

Consider the physicist measuring the field of a magnetron star.  He known he is measuring from our uncertain world and our viewing SNR is much lower. But the magnetron is a cooled version of the gravitron star, within its system density is more evenly spaced. So, with our low SNR, the physicist can construct the spectral of the magnetron star, and thus know, a bit better, the likely relative density of the boson/proton barrier; under the assumption that the magnetron star is a more accurate version of the standard model. The model  he learns, he applies in our world. He knows the relative density of the orders to a higher SNR, but loses relative SNR in measuring kinetic energy between within the orders.