Some Stough As To Reimman Scattering Versus Rayleigh Scattering

When one given arbitrary substringular phenomenology is scattered harmonically, such an eluded-to semi-group is then here undergoing a Reimman Scattering.  When one given arbitrary substringular phenomenonlogy is, instead, scattered annharmonically, such an eluded-to semi-group is then here undergoing a Rayleigh scattering.  A Reimman Scattering -- in the substringular -- is one in which one given arbitrary group of superstrings that operate to perform one specific function (a given arbitrary  orbifold eigenset) is scattered in such a manner, in so that the adjacent eigenmembers of phenomenolgy that are redistributed by the so-stated scattering will bear an even chirality, as well as that these so-eluded-to eigenmembers that are adjacent are here tending to bear a trivial isomorphism -- as the so-stated given arbitrary orbifold eigenset that is here scattered is re-distributed into a different delineation, over time.  Whereas, a Rayleigh Scattering -- in the substringluar -- is one in which one given arbitrary  group of superstrings that operate to perform one specific function (a given arbitrary orbifold eigenset) is scattered in such a manner in so that the adjacent eigenmembers of phenomenology that are redistributed by the so-stated scattering will bear an odd chirality, as well as that these so-eluded-to eigenmembers that are adjacent are here tending to bear a non-trivial isomorphism. -- as the so-stated given arbitrary orbifold eigenset that is here scattered is re-distributed into a different delineation, over time.  Such just mentioned scatterings (that are either of a Reimman Scattering or that are of a Rayleigh Scattering) may be of either a euclidean-based perturbative genus, or such scatterings may be of a Clifford or euler-based perturbative genus.  A prime example of a general format of a Reimman Scattering, is the process of the formation of cohomolgical projections, over time, by the mappable tracings -- that are multiplicitly pulled into existence by the kinematic activity of substringular activities, in the process of the integration of ghost-based indices, while, a prime example of a general format of a Rayleigh Scattering, is the process of the vanquishment of cohomological projections, over time, by the mappable tracings that are multiplicitly pulled into existence by the kinematic activity of substringular activities, in the process of the reverse-derivation of ghost-based indices.
Next post, the tendencies of scatterings due to both the motion of either torroidal-based morphologies that are kinematically delineated, as redistributed orbifold eigensets that are displaced over time, and/or the motion of conical-based morphologies that are kinematically delineated, as redistributed orbifold eigensets that are displaced over time.
To Be Continued!  I will continue with the suspense later!!! Sam Roach.