Operators And Group-Attractors, Part Five

Superstrings of discrete energy permittivity, that act over time via a divergent series -- in so as to perturbate out of a relative tense of conformal invariance -- tend to have both more Laplacian-based changes and Fourier-based changes as well, to happen to the Gliosis-based respective field, that would directly appertain to the correlative nature of such superstrings in question.  Such so-stated strings of discrete energy permittivity, also tend to work to bear more Gliosis-based accelerations to happen to the holonomic substrate of their immediate field, at the Poincare level to their topological surface, than an otherwise convergent set of such superstrings would.  This  just-stated general tendency, tends to work to form more varied tenses of wave deformation to the multiplicit topological surface of such correlative superstrings of discrete energy -- that are to perturbate in a divergent manner, from one general substringular locus to another, via the processes of a relative tense of what would often here be the case of what may happen in a given arbitrary situation such as this, to where this could here work to form a Rayleigh scattering.  This is because, if a superstring is to be annharmonically altered in its Hamiltonian operand via a Cevita interaction -- to where the correlative adjacent eigenindices are of an odd chirality -- this will then tend to work to form a divergent re-delineation and/or a divergent re-distribution of the here mentioned eigenindices.  As a substringular entity is to be scattered through a field operand, to where this of which is to bear a scalar amplitude that may be described of as bearing a Clifford Expansion -- then, the multiplicit intermittent disturbances of space, that will thus bear more of a tendency to permutate such a "widening" Hamiltonian operand, will then tend to increase in its Hodge-Index, when this is taken relative to the euler eigenbase of the so-stated expansion.  Such an ever increasing influx -- that would often be happening in such a given arbitrary respective case, will often be borne into an expanding operand -- that will then tend to interact more than otherwise, with the so-eluded-to attenuated metrical-gauge-based Hamiltonian operator, that is to here be in the process of diverging as such.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.