As To Altering The Initial Polarization-Related Effect, Of Two Different Physical Li-Based Groups

 Let us say, one were initially to have two different and distinct Li-Based groups, that were here, to initially be adjacent to one another, at a level that was here to be Poincare to the eminently inferred region, at which these two different and distinct inferred cohesive sets of discrete energy quanta, were here to be iterating at -- at a virtual metaphorical "snapshot" of duration, to where such a said "snapshot" in "time," was here to be taken, over the course of a respective given arbitrary iteration of BRST. Let us next stipulate, that these two different and distinct cohesive sets of discrete energy quanta, during such an iteration of BRST -- are to be delineated at such a general given arbitrary distribution-related manner -- to where such inferred sets of discrete energy quanta, are here to bear a covariant tense of a Nijenhuis Orthogonal nature (which is here to bear a relatively strong manner of conformal invariance, at a vantage-point, that is Poincare to that internal reference-frame, that is here to be of the eminent field-density, of the so-inferred region), at which the said sets of energy quanta, are to be both co-determinable and co-differentiable, as those composite superstrings of discrete energy permittivity, that are here to be working to make-up the external structure of such inferred "teams" of discrete energy quanta, are to be working to display the general gauge-metric-related exhibition, by which the general virtual standstill of the kinematic activity at BRST, is thence to occur. Let us next stipulate, that these two respective distinctly different "teams" of energy, are here to be Polarized -- the one from the other, -- due to the general Noether-related norm-based physical condition, that the covariant tense of the dual orthogonal projection, that is here to be existent between/amongst these two said "teams" of discrete energy, is here to be of a Nijenhuis dual state of norm-related projection  -- by which these two different Li-Based groups, that are here to be working to bear a tense of a Ward-Cauchy-related manner of norm-related projection -- are thence to be "encoded for," as belonging to two different universal settings. (Each of such individually taken Li-Based groups, is to be of a parallel universe from one another, when this is here to be taken, in correlation of the one to the other, and vice-versa), -- while all the more, this given arbitrary case scenario is to be considered, As this is here to be taken, over a basically "Laplacian" general format of stipulation. Now here's the "catcher." What If one were to alter the inferred covariant norm-conditions of each of such cohesive sets of discrete energy quanta -- the one towards the other, and vice-versa, to where the general initially considered Nijenhuis tense of orthogonal behavior, that we were just starting to discuss here, -- were now to bear a kinematic perturbation, into spontaneously and consequentially, ensuing to change into a set of two different and distinct geometric groups (groupings), that are thence to result, into working to form a case scenario, by which one is now to have two different and distinct cohesive sets of discrete energy quanta, that are now to work to bear a norm-related geometry, in which the inferred physical spaces discussed here, will now work to bear a covariant Riemann-Related geometry, that is here to be of a Real Riemann tense of norm-related projection. If and when this is here to happen in such a given arbitrary case scenario, these two different initially inferred unique "teams" of physical spaces, will then tend to end-up resulting, in working to display the exhibition, of two different and distinct sets of energy quanta, that are, at this point in duration, to be of the same universal setting. To Be Continued1 Sincerely, SAMUEL DAVID ROACH. (1989).