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Wednesday, March 21, 2018

AuT as symmetry breaking and x vs time 1 of 2

Symmetry Breaking
What SM calls "breaking symmetry" is the idea that there are different symmetries at different dimensional levels.  AuT has a similar concept, more properly called "building symmetries" instead of breaking, but that is largely semantics.
Here is a mathematical example of how the two compare:
SM has Lagrange LQCD=Sum(over q) of QDq(the Dirac equation) -1/4GuVG^uv (Maxwell's equation in a vacuum).  This can then be normalized with a Higgs Field.
AuT has a non-similar arrangement but with similar results:
               AuT= Ordered Sum(ct1-independent)+sum(ct2 version of sum of ordered ct1)+sum(ct3 version of ct2+ordered ct1)+Sum(ct4 version of ct3+ct2+ordered ct1) yields a solution translated into a current state of the universe based on the order of the solution where each state is a built symmetry of the prior state according to either 2f(n)^2^n or some predecessor function.
                These vastly different approaches yield similar results, the Lagrange field being an approximation at a given location for the  broader result in AuT.  AuT can be summarized in a local environment, but it is a complicated analysis because the values of ct1 are varying, albeit at a very slow rate in the middle range where we live  No attempt has been made to determine how many changes of x lead to a change in the average ct1 state, but the power of entropy should provide a fairly good measurement from which this may be obtained, it is certainly a huge number.
           The next issue is how many changes occur in a pre-time environment before standard clock time is significantly affected.  This brings us to the second aspect of the building symmetries which is the different measure of time which is a subset of the ordered sum above and comes from this solution: QT(n)approx=Sum(ct4 version of ct3+ct2+ordered ct1)approx.=Sum(over 10 information arms of ct4 version of ct3) for a given ct3-ct4 state set in question.   It is worth noting that this subset for a given ct3-ct4 transition state gives a quantum time state for the ct3-ct4 transitions states in question.  This is a quantum of time.  These do not change in a vacuum, of course (there is no vacuum in AuT) instead they are separated by ordered, slowly changing ct1,ct2 and ct3 state clouds which affect the changes between and the makeup of two successive QT(n)=quantum time for a given value of x=n.  That being said, however, the actual history involved in the movement of the clock time is a function of the ct4-ct3 transition states.





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