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| Tags: code, commutative, genetic, noncommutative, universe |
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#1
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#2
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From Osher Doctorow
In classical dimensional analysis, the dimension of Length, L, is ordinarily distinguished from Lx, Ly, Lz if some event (short here for set, process, event) if not spatially or directionally homogeneous. In the absence of such homgeneity, L is enough. When the direction such as x, y, z or other directions make a difference, then one or more of Lx, Ly, Lz are used depending on which directions are relevant to the problem. What exactly the state of "only containing one event" is, is very difficult to conceive of. The Big Bang or "Almost-Big-Bang" seems roughly analogous to the idea that "a light wave 'sees' its entire past, present, and future simultaneously". In the case of the Big Bang, it would also presumably 'see' its entire spatial past, present, and future extents and masses/energies and forces. It is not difficult to see why F. Tipler became Spiritual even without PI with such Big Bang or Near-Big-Bang scenarios apparent to him, including his zero-point ideas discussed also by David Deutsch. Once more than one event existed in the universe, however, and indeed in the process of the universe "getting" more than one event, a curious thing must have happened which comes from the very nature of events which are sets (even processes as "generalized" sets). In losing its unity or unification, the universe immediately had to 'discover' both similarities ("commutative" in a sense) and dissimiliarities ("noncommutative" in a sense), the second from sets, the first from probabilities or measures of sets or more specifically orbits characterized by P(A) = P(B) = .... When we treat the universe via classical dimensional analysis, we are using dimensions as an abelian (commutative) group under multiplication with positive and negative and zero exponents. In the genetic code, we have perhaps an "ultimate" type of noncommutative treatment in a sense, with everything noncommutative in the code. All this does not require the universe to be "conscious" in the human sense, but it does indicate that it is correct to use the words "discrimination" (ability to distinguish between two (or more) stimuli) and "integration" (ability to find what is similar or common to two (or more) stimuli) in regard to the universe. When we discriminate and integrate (sometimes called "correctly generalize" for the latter), we are "true to the universe" in a rather profound sense. Both are arguably equally and highly valuable. Osher Doctorow |
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#3
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From Osher Doctorow
So we come to the question of what it means for the universe code to be noncommutative in regard to M1M2M3L1L2L3T1T2T3F1(F2). The most interesting thing is that a clue is available from metrics and of all things additively-subtractively! From ds^2 = dx^2 + dy^2 + dz^2 - dt^2 or its negative, we get an additive noncommutativity distinguishing time from space. So already whether the triple ("codon") L1L2L3 is to the left or to the right of T1T2T3 arguably makes a difference. So we already have two "strings" of characters in the universe code: 1) L1L2L3T1T2T3M1M2M3F1(F2) 2) T1T2T2L1L2L3M1M2M3F1(F2) The first string is correctly described as the representation of our "time is causal" non-black-hole universe. The second string arguably describes the reversal of time and space in black holes. Triples to the left of other triples are "causes" of the right triples. I suppose that Sir Roger Penrose's twistor theory might roughly be described by: 3) M1M2M3T1T2T3L1L2L3F1(F2) since his twistors are used to attempt to create "space-time" geometry (time, distance, etc.), while a more usual approach with spacetime either on an equal footing or causing matter and so on would have the L and T parts to the left of the M and maybe F parts or else would be commutative which wouldn't discriminate the orders. Notice that an infinite number of dimensions is neither out of the question nor indicative of nonlocality. In fact, even a Mickey Mouse-like balloon which expands differently in different directions gives us an idea of the general nature of expansion-contraction which involves an enormous number and arguably an infinite (even uncountably infinite!) number of directions/dimensions of L type but "tied to" each local point or little string. This does not yet mean that those are all dimensions in the same sense as L1, L2, L3 since arguably dimension and direction aren't the same. Osher Doctorow |
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