Chirality And Scattering

When two or more phenomena are scattered amongst each other -- in such a manner to where the resultant adjacent thus scattered eigenindices, are to work here in so as to attain an odd chirality, -- then, such a just explained general genus of scattering, may be described of as a Rayleigh scattering.  Yet, when two or more phenomena are scattered amongst each other -- in a manner to where the resultant adjacent thus scattered eigenindices, are to work here in so as to attain an even chirality, -- then, such a just explained general genus of a scattering, may be described of as a Reimman scattering.  When the respective given arbitrary gauge-bosons, that are to here bear a Laplacian-based Ward-Caucy condition of being adjacent over the course of a respective iteration of instanton, bear more of an assymetric vibratory oscillation, -- this will then result in the production of there being more harmonically formed Schwinger-Indices.  Thence, the more that the gauge-bosons, that are correlative to a discrete quantum of energy -- tend to work to bear a certain scalar amplitude of a tense of a Rayleigh scattering, then, the more that the resultant Schwinger-Indices will tend to work to bear more of a scalar amplitude of a Reimman scattering.  To Be Continued!  Sincerely, Samuel Roach.