Wednesday, March 5, 2014

Treating vacuum in the encoded sequence

The whole point of physics is to get the bit stream version of the world. In this world, when compacted, the vacuum samples are the samples saved through quantization. They react, but have no field. Very sorry, they set the vacuum phase at Nyquist. They appear, always, as one group, not interspered with any of other quantized disturbance. So in the spectrum, is the vacuum, farthest to the short end at Nyquist. Then you have, one or more sets of,[ the short lobes, a unit of matter, and the long lobe], going from nuclear up to, way over to the left, charge. Optimum congestion, which the vacuum does by sampling at less than Nyquist, instead under sampling designed to minimize Pauli and minimize, samples/disturbance.

The matter lobe is phase zero. The short lobe and long lobe, opposite phases shifted relative to zero. The greater the phase shift, the tighter the loop, opposite the short, having a much more mild loop in the other direction.

The sequence of samples that generated, the world under study,  can be read off by picking a sample from one of the three lobes, vacuum first, to make the phase systematically minimum. No simultaneity in the sequence, so fields  can be combined in order.

  Mapping the sequence to other dimensions is done by placing the vacuum sequences, in order, where you want them. simultaneity

Quantization levels and uncertainty always equalized to sub Nyquist. Vacuum has the highest SNR. Mass is the best guide to sample share, sample share  ratio of the mass to the total vacuum (is a good one here)point source sequence length.

Since the current standard model is approximate and converging, this theory is as good as it.

Lets get straight mass transfer at wave speed. A nuclear world emits nuclear-electro waves.  We get what look like a proton in our electron world. So mass transfer, down hill, and the vacuum takes a bite. Something else coming in comes from a magneto-gravitational wave. We would hardly notice, pass through with little curvature (phase shift). Apparent forward motion of the wave is very slow undulations (left lobe field) and high speed undulations (upper lobe field). Upper field, less frequent, but more phase shifted. Fields and matter behavior determiend by relative phase shift and sample space.

The mass ratio beetween the total of the proton is about 10,000. But vacuum should ba able to separate the orders by a change of three more bits of precisio9n per order.  So, a 10,000 order spread at 8 time SNR per order comes to (1/8 * 1/8 * 1/8* 1/8) etc. The Higgs field is not that far down.  So we expect total precision to increase much slower going down, sot of Moore's lew in  reverse.  In other words, the distribution of the disturbance in our world its all half the width of the proton. Most of it got quantized in two levels, Nyquist, and Higgs, and the Higgs mass per proton size is relatively large. I have not looked up the ratios here, and I am guessing. But if that is the case, our world is far from perfect quantization relative to the whol disturbance.

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