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Thursday, April 21, 2016

AuT-compressed quantum change and time dilation

We have seen that speed and sharing more ct1 states by a higher state gives rise to time dilation.
This raises a curious question as to what happens when you have higher compressed states (231).  It is clear that a ct0 state may only change in one way at a time, presumably from non-linearity to linearity.  A ct1 state presumably can change is at least one dimension at a time (2^1 is 2 however).  Ignoring for the moment the two faces of ct1, ct2 has sufficient compression so that it might be possible to imagine different compressed components changing in more than one coordinate at a time.  This would be more pronouced for the higher states.  Given the lack of separation between quantum phenomena, like photons, we can ignore, to some extent, ct1 and ct2 as having insufficient separation for multiple ct1 states to become engaged with any  point source.  While ct3, wave energy, clearly interacts with more than one ct1 state at once and while we can be certain that this interaction is with multiple ct1 states, the fluid relationship between ct2 and ct3 (possibly tied to the relationship indicated by the compression equation: F(series)(x-2,x-1,x)^2^x) might eliminate this as a significant factor.  Once, however, you get to the more "stable" ct4 state (10^2^4) or (2plus3plus5)^8 compression, the interaction with multiple ct1 states becomes more complicated and only with acceleration do you obtain time dilation whether by spin, vibration or straight acceleration would presumably have differing effect, although it may not be measurable.
This will be explored in more detail in Volume II.
The change in CT2 and 3 is at such a rapid pace that it is likely that the effects of time dilation would be limited because of how much ct1 is contacted due to the movement.  Perhaps the study of "trapped light" would give unique insights especially if compared to the study of accelerated particles approaching light speed or those super heated to get a similar effect.

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