A Little Bit About Other Formats of Scattering

Often, a substringular scattering that is acted upon from an outside source involves both a Reimman scattering and a Rayleigh scattering -- at one general given arbitrary locus.  For instance, let us say that one orbifold eigenset were to strike another orbifold eigenset, in such a manner in so that there is an initial Rayleigh-based scattering at the interial Poincaire-based locus of the so-eluded-to scattering, and, to where, there is a latter happening of a Reimman-based scattering at the exterial Poincaire-based locus of the same general genus of the so-eluded-to scattering.  Here, the interial so-mentioned scattering involves an enharmonic scattering of superstrings, and, the exterial so-mentioned scattering involves a harmonic scattering of superstrings.  The so-mentioned enharmonic scattering works to involve adjacent eigenstates of the said re-displacement of superstrings that work to bear an odd chirality of group related metric -- through the tensoric intricacies of the here spewn eigenbase of Lagrangian setting, over time.  This is while the so-mentioned harmonic scattering works to involve adjacent eigenstates of the said re-displacement of superstrings that work to bear an even chirality of group related metric -- through the tensoric intricacies of the here spawn eigenbase of Lagrangian setting, over time.  This may be more pictorially described in this manner:  The enharmonic so-mentioned scattering in this case works to form a chaotic delineation of re-displaced eigenstates -- in the form of a set of re-delineated superstrings that are not evenly redisplaced, or are outside of any particular pattern of re-established positionings -- as the so-mentioned superstrings are pulled out of an initial Ward-Caucy tense of order,  that would have existed here before the so-eluded-to scattering.  On the other hand, the harmonic so-mentioned scattering works to form a tense of a re-convened eigenbase  of delineation of re-displaced eigenstates -- in the form of a set of re-established positionings -- as the so-mentioned superstrings are pulled back into the initial Ward-Caucy tense of order, that, again, would have existed here before the so-eluded-to scattering.  This would only happen if the initial disorder that would here be caused by the Rayleigh scattering was brought back into order by the effects of an exterior-based source -- that acted upon the so-mentioned conditions of chaos, in so as to bring a state of optimum rest, in so as to scatter the so-stated delineations of chaos back into order.  Yet, eventually, such a tense of a chaotic-based scattering being scattered into a more orderly distribution by an outside source, will tend to bear a more heightened aptitude of being brought back into a condition of chaos once again.  For instance, the Big Bang -- when it created the multiverse -- formed an extreme initial degree of chaos, of which eventually was brought into some local tenses of heightened order.  Yet, the tendency of the just mentioned order is in the direction of a heightened capacity to go back into a state of disorder.  So, as long as there is no exterior influence upon an initial scattering in the substringular, the tendency is, rather, to go from an initial Reimman scattering of orderly re-displacement into a latter Rayleigh scattering of a chaotic re-displacement.