This is simply a Ramsey theory problem in which the phase and nulls, packed against a Higgs bandwidth limit will adjust phase offset and mutual motion to provide separability and connectivity. The available bandwidth for exchanges is divided according to Ramsey theory. The division of bandwidth would then obey Lagrange numbers of something similar, as long as the packed nulls, the phase offset and the mutual motion make the effectively separated band gaps.
Each phase offset provides a new degree of freedom and generates a stable mutual motion and phase offset which are unique, and follow the Ramsey theory rules. The Lagrange numbers fall into place because each preceding system leaves a samples data spectrum that is mutually orthogonal to the next Lagrange number up the chain. I think each Lagrange is maximally separable to its previous, so we get a sort of Schur reduction:
In numerical analysis, the Schur complement method, named after Issai Schur, is the basic and the earliest version of non-overlapping domain decomposition method, also called iterative substructuring. A finite element problem is split into non-overlapping subdomains, and the unknowns in the interiors of the subdomains are eliminated. The remaining Schur complement system on the unknowns associated with subdomain interfaces is solved by the conjugate gradient method.I think this will apply to the Lagrange numbers when there is no system noise and both noise and bandwidth separation can be adjusted by the process of elimination.That is, both channel noise and quants are mutually adjustable. So the sequence might be:
- Free space is a half shift between phase and no pack null.
- The graviton is a full shift and the graviton with no motion, and the smallest null set, but stable in a gravitational 1/2 gradient.
- The Leptons getting a 1 and 1/2 shift, more Nulls in quant sizes basic to gravitons and mutually orthogonal to each other.
- The Leptons split a 3 shift plus half spin, Null sizes in units of the spinners, and having three degrees of motion make the quarks, in triplets
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