We know if for the electron world. So, we find the symbols over fquenecy share, from our -iLog(i=i). That gives us number samples per symbol. At that quantizaion level, the quant levels and uncertainty for optimal congestion. Tells you how much space this level gets on the spectrum chart. Add one quant level going up each order.
Say the original disturbance was evenly dispersed and sparse. We can guess a finocci that subdivides the sequence in balance, up to a small order, eight or non -iLog(i). Then we assume it was bunched up into two groups. Then we guess at a very long wave quantization, the the remainer balanced. The long wave is way over to the long wave end on the spectrum chart and tightly peaked, not much spectrum space. Find the unbalanced fibonnocci to match. That is a hugejump in SNR. In the end, the two quantized clump merge in a giant cataclysm of heavy light transfer. The one clump blowing up the other to release lower order wave propagations.
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