As to the Rate of Approach of Proximal Indices, Part One

When a phenomenon of mass, that is composed -- in this case -- of molecules, is struck by another phenomenon of mass that is, as well, composed of molecules, there is a collision that involves a resultant state of momenta-based indices.  The faster the collision of the directly previous case that I have just mentioned, the more that the scalar magnitude is of the resultant state of momenta-based indices is.  At a much lower level, the basis of momentum is the idea behind the conditions of Hamiltonian operations -- at the substringular level.  The velocity of a phenomenon of mass is based upon the manner in which the indices that work to comprise the said mass, are comprised of orbifold eigensets, that move in such a manner in so that any here given arbitrary mass will be able to approach the speed of light, as the process in which the correlative orbifold eigensets that work to comprise the so-stated mass move in such a manner to where the composite of such said eigensets will here work towards moving in more of a unitary Lagrangian in a Noether-based flow, that will move in this case as one set organized whole at once,  to where it will then here bear an optimum linear-based propagation, that will do this same general pattern of motion up until it at least is able to interact with at least some infrared photons along the way.  The closer that a mass is able to come to doing this format of activity, the closer that the said mass will come to going at the speed of light.  Yet, as I have said before, since a mass as a mass tends to be considered here as having both a Kaluza-Klein light-cone-gauge topology, and as also having Yau-Exact singularities, a mass, when being as such, is not actually able to go at the speed of light or faster - or else it would have all of the mass in the universe.  Yet, if the light-cone-gauge topology of the said mass were to temporarily be translated from having its initial Kaluza-Klein topology to having a Yang-Mills light-cone-gauge topology, while then re-converting back into having a Kaluza-Klein light-cone-gauge topology, then, the so-stated mass will have succeeded at being temporarily translated faster than light as a tachyonic genus of holonomic substrate.  This, though, does not discredit the fact that a vast majority of the speed that is allowed by a worm-hole is caused simply by the contoursioning of space-time-fabric -- since the space-time-continuum involves a granular eigenbase of curvature that is not actually straight.  When something is actually "straight" in the substringular, without the bearings of the normal curvature of time and space, this genus of linear conditionality is called a Wilson Line.  So, when a substringular phenomenon is pulled into the Ward-Neumman bounds of the core-field-density of another substringular phenomenon, the scalar magnitude of the Yakawa Coupling that this is resulted in is higher when the globally distinguishable rate of the here implied collision is high -- whether we are comparing two of such cases that are respectively of a Gliossi-based collision, or whether we are comparing two of such cases that are not Gliossi, but are of the same respective Yakawa-based index of Hamiltonian operation.  To Be Continued!  Sam.