When a set of relatively forward-holomorphic-norm-states are initially scattered harmonically upon set of superstrings that directly appertain to the presence of a mass -- that are moving in the membranal context of an orbifold eigenset -- the resultant ghost-based cohomological-based setting, that is formed by the just eluded-to Reimman-based scattering, may be termed of as a chiral-based cohomology that is of a Calabi-Yau-based cohomological setting. Yet, if the situation is still of the same general nature, yet, the substringular phenomenology that is scattered by the here relatively forward-holomomorphic-norm-states is directly appertaining to the presence of a quantum of plain kinetic energy -- the reslultant ghost-based cohomological-based setting that is here formed by the just eluded-to Reimman-based scattering is a chiral-based cohomology that is of a Calabi-Wilson-Gordan-based cohomological setting. Furthermore, if the situation if still yet of the same general nature, yet, the substringular phenomenology that is scattered by the here relatively forward-holomorphic-norm-states is directly appertaining to the presence of a quantum of electromagnetic energy -- the resultant ghost-based cohomological-based setting that is here formed by the just eluded-to Reimman-based scattering is a chiral-based cohomology that is of a Calabi-Calabi-based cohomological setting. The respective ensuing initial annharmonic scattering of the just mentioned ghost-based cohomologies, is a Rayleigh scattering -- that is of an antichiral or a Kusomo-Suzuki-based nature. This is on account of the condition that a chiral-based cohomology is of a Calabi-based nature, while, an antichirial-based cohomologyi is, again, of what may be termed of as a Kusomo-Suzuki-based nature. Calabi-based cohomologies are of either a trivially isomorphic or of a non-trivially isomorphic symmetry. Kusomo-Suzuki-based cohomologies are of an assymmetric nature. These here just mentioned descriptions of certain general formats of cohomological symmetry, are directly appertaining to the nature of the scattering of the ghost-based indices -- that are here correlative to the cohomological eigenbase of a set of extrapolatable mappable tracings of distinct physical memories that may be detectable in the substringular.
I will continue with the suspense later!
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