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Sunday, December 4, 2016

AuT-lumpy time edited

As I get closer to publishing the second edition of Spirals in Amber, I'm getting a little closer to the mathematics of compression and movement which, surprise surprise, are closely connected.  Space time is only relative change of multiple ct1 states relative to a single ct1 state which suggests, if not requires, that the one ct1 state must pass through all the ct1's in the ct2 256 unit matrix to achieve movement.  This also, jives with the 1 to 11 (or 2 to 22) formulation of F-series which is nice.  It allows for the illusion of spacetime to exist without other artifice.  However, the discussion has so affected the analysis of "lumpy time" that I've had to break it into several sections which may, in turn, break down further as I move forward.
Please make sure to cite spirals in amber in all your comments, I need to press.   This comes from the yet unpublished 2nd edition.

AuT-Lumpy time 1


There are two separate universes.  One is the "true" universe which has a clock based on the quantum changes in a single variable.
The second universe is the relativistic universe that we call space time.
The division between these two can be understood as follows:

The relative comparison of unbroken ct states to a broken ct state is recorded by stacking each solution to get the next solution.  The theory runs as follows;
1) 1 compared to 1,1 or 2 for photonic state. 1 compared to 1,2,3 for wave energy, etc.
2) The same process occurs and the two solutions are added to get a recorded event.
3) 0 compared with 1,1, or 2 for photonic states which creates a defect in the operation.  This defect gives rise to time and provides a mechanism for separating points giving rise to dimension and standard clock time.
4) X continues one quantum change at a time so that time is changed into two separate parts: x time which is true time; sct (which is relativistic space-time).
Also, if all times are built on the prior times, then it may be possible to mine the present for the past.  It might require “rehabilitating” past data which has changed in response to the changing value of x which is presumed to be the reason that history fades so quickly, that past information “degrades” from the state it was in when history was made to successive states one quantum instant of information at a time until it is completely degraded.
There are certainly some "elements" of time information preservation.  For example, light carrying old times, often billions of years old, into our telescopes.  This suggests that degradation is potentially slower (or even non-existent) for lower ct states (2 and 3), yet another element of ct states which suggests additional examination.  One suggestion is that the higher the ct state the faster the degradation of time carried so very little occurs with photons and waves, but it increases greatly with matter and ct5.
There is little question that in Aut the present is built on the past, but the methodology requires that standard clock time changes are relative to ct1 along with separation and velocity which otherwise would not be perceived (but for changes relative to ct1).
Time, as a relative change against ct1 can be measured in quantum steps and hence must be quantum, that is sct.  If ct2 is 256 compressed ct1 states changing with one ct1 state (one ct1 exchanging position with one of the 256 compressed ct1 states (or 1 ct2 state) at a time; then at ct3 for the “speed of light” there would be “either” (1) 6^2^3 (6^6) ct2 states changing at a time or (2) that same number of ct1 states changing at a time; either giving the same result of 1 in 256 for ct1-2 for the speed of light. 
Now some of you are wondering, ‘why an even exchange?’  There doesn’t have to be an even exchange or even any exchange at all.  But we do have “movement” based on relative comparison of ct1 to ct2.  That is where all of Einstein’s work comes from.  He had space-time down pat.  The real question is why didn’t he see where space time arose since if it were any more obvious it would jump out and bite everyone.  The answer, is that it only became obvious from a better understanding of information theory and the breakdown of information at certain boundaries.  It did, after all, take almost 3 years to burrow down to that once the boundary problems was mathematically obvious.
The even exchange comes about because movement is “quantum.”  We know that ct1 changes relative to ct2, otherwise there would be no movement.  We know that ct2 appears to travel based on being at one ct1 point one quantum instant and another ct1 point at another quantum instant and even Einstein figured out how long a quantum instant was although he largely ignored his finding in favor of ignoring the ct1-ct2 interface for whatever reason.
There are only so many ways to have this exchange. (1) One is for ct2 states (which we have to remember are only aligned ct1 states) to move along a line of ct1s.  This is not attractive because it is bulky.  This, however, the traditional method of observing movement.  The problem with this traditional method is that is requires linear space time and we know based on information theory that space time has to be quantum, otherwise there is no minimum size, even Planck would have some problems there. While we now know that Planck was wrong (minimum length is information not length at all) he did at least look as far back in space time as he could without leaving it entirely like AuT. (2)The other is for one of these ct2 states to change by substitution.  There are two forms of substitution, but they amount to the same thing, one is the exchange of one ct1 state for a ct1 within the ct2 ‘matrix’ and the other is for all of the ct1’s in the ct2 matrix to shift together from one quantum universe to the next stacked one.  Both occur together and the math is similar.  The passing through of a common ct1, exchanging with one of the ct1’s within the ct 1 matrix, over time, this means that the “compressed” ct2 state appears to be a lump even though it isn’t.  Instead the ct1 being exchanged “moves through all the “compressed” ct1s and this common movement makes them appear together.  This fits well in the 1 to 11 F model and explains why that model works.  From 1 to 11 you get the exponential exchange as discussed in detail herein comparing F series compression to information theory compression.  In other words, a compressed ct2 is merely a matrix of ct1’s that exchanges sequentially with a ct1.
This suggests that ct2 and ct1 may interchange like ct3 and ct4.  It may be that there is some mathematical reason this is unlikely; but expansion/compression inflection point theory of AuT suggests that this conversion actually happens on massive scales, otherwise there would not be big bangs and the opposite inflection points which we can call “big unbangs.”

This requires a further discussion.

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