A Little About The Displacement of the Substringular

When one considers two semi-groups that collide with an equal velocity upon contact, this of which  acts as two relatively small groups of superstringular phenomenology that are alike -- except for the condition that one of the two just mentioned superstringular semi-groups bears a relatively homeomorphic pattern of Lorentz-Four-Contraction, of which is more compactified, in general, than the other of the two so-eluded-to semi-groups that I have here mentioned -- then, the first of such eluded-to semi-groups of superstringular phenomenology will tend to act as a holonomic substrate that will be able to produce more of a displacement upon the second of such eluded-to semi-groups, again, upon contact, in so long as both of the here mentioned semi-groups work to bear the same differential pattern of general morphology, and, in so long as both of the here mentioned semi-groups are of the same Hodge-based scalar magnitude of Hamiltonian Ward-Neumman-based quanta, and, in so long as both of the here mentioned semi-groups -- that will here act as two colliding respective holonomic substrates, work to bear the same genus and format of conformal invariance, upon contact.  This will then, here, work to indicate that both of the here eluded-to structures of superstringular phenomenology will bear two different resultant tenses of both their Lorentz-Four-Contraction, as well as bearing two different tenses of the scalar magnitude as to the extent of their two distinct respective gauge-metrics, when this is in consideration of the correlative eigenstates of their Polyakov-Action-based activity.  This also only tends to be true if both of the here mentioned semi-groups will here be both approaching each other at the same velocity, in relativistic terms, right before contact -- via the presence of a binary Hamiltonian operand, that acts as the mappable path of a homeomorphic binary-based Lagrangian, as well as both of these so-eluded-to semi-groups striking each other with the same genus of their overall permittivity-based index -- as taken from the vantage-point of a central conipoint.  Such a displacement may either be of a Wess-Zumio manner of metrical scalar genus, or, such a displacement may, instead, be of a more perturbative format -- in so that the displacement will then here scatter the eigenbase of the Hodge-based group index of the original composition of the initial structure of the "weaker" of such holonomic substrates, that here worked to comprise the Hamiltonian operator that acted as the here mentioned semi-group that I had initally eluded-to as being more likely to be overtly displaced -- at the here eluded-to general locus, of what may either be a euclidean or a Clifford-based scattering of one semi-group of phenomenology by another semi-group of phenomenology.  I will continue with the suspense later!  To Be Continued!!! Sam Roach.