Chapter 6 Notes on Primary Equations
While the basic algorithms do not
change, compression upon information concentration and increased place and
dimension ensures that the solution will get more complicated past the basic
solutions for the ct0 and ct1 carrier states. The initial solutions giving rise to the 64
ct2 carrier/information arms the 2^2 part of the f(2)^(2^2) equation do not
require an examination of the effect of curvature when y increases in the sin
equations and the evolving values which occur once the matrix is complicated
past the initial ct1 carrier. The first
carrier is in a ct1 environment where these effects are marginalized, allowing a
simple proof giving rise to the ct2 carrier in the ct1 environment (64).
The original reason theorized for
the existence of more matter than antimatter is because the solutions define
more positive carrier states because ct2 and higher ct states have only positive
solutions for curvature. A closer examination
indicates that a more likely reason is that the net expansion or contraction
state of the ct1-ct2 carriers is mostly positive at this point of time (net universal
expansion) and that as the universe slows, even less antimatter will be
present. However, when the universe
starts to contract, the amount of anti-matter/dark energy will begin to
increase with a maximum defined by the inflectio point where the next big bang occurs.
F(pluspix) is the derivative feature
of 0’ that gives the state (+/-) to all subsequent ct states. F(x) is the Fibonnaci number portion of the solution.
The lifespan or length of any state, via
the carrier state which is a combination of the F(x) for life and the F(pluspix)
for state (+/-) and the information arm length, at least for the initial ct1-ct2
carrier; can vary greatly depending on the F-series solution to the underlying
ct1 states which is the way that durability is maintained. In addition, the curvature results show that
the manipulation of this feature (see the relative sin functions) for
degrees. Since it is a quantum universe,
the fractional ct states seen with sin series greater than one are not
considered accurate or as accurate as the the f(pluspix) function.
The plus or minus length of ct0 durable
solutions leads to ct1 durable solutions of lengths defined by F(x) which forms
the carrier/information arms defined by 2^n and initially based on the more complex
1/0’2n+1 solutions for ct 2 which in turn forms carriers for the next higher ct
states which can only be populated with exponentially higher quantities by definition
as set out in Figure 3 which quantities are defined by the equation f(n)^(2^n).
If the sum of ct1 carriers are 5000,
still very short, then it would take 5000 changes of x before there would be a state
(+/-) change. If -7000 it would also
take 7000 changes of x but it would be a negative or antimatter state for that period.
The current universe is using up all
the negative states in expansion via the breakdown of higher states into space.
At the inflection point when compression
states begin to outnumber decompression states, we will begin to build an anit-matter
universe.
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