Process Of Substringular Inter-Binding

Let us consider here a given arbitrary two-dimensional superstring of discrete energy permittivity, that is initially moving as one discrete orbifold eigenset -- to where it is brought into the immediate substringular physical bounds of a second given arbitrary genus of an orbifold eigenset, -- to where the resultant physical configuration of the overall net Laplacian-based holonomic substrate, is to then be one overall respective given arbitrary entity -- of what is to then be one whole entire orbifold eigenset, of which is to contain in the immediate physical bounds of its directly corresponding spatial parameters, each of such so-eluded-to superstrings of discrete energy permittivity, that were of the initially so-eluded-to case scenario that I  have here began to imply.  The initial orbifold eigenset of one freely moving bosonic superstring of discrete energy permittivity, is to be moving along an initially hermitian Hamiltonian operand, in so as to be going through a discrete Lagrangian path -- through what is to be here an initially undetermined destination.  One may arbitrarily call the initial path that is of the said initially stated bosonic superstring of a metrical-gauge-based Hamiltonian nature -- as to be in the propagational-related relatively holomorphic direction.  In the meanwhile, there is a relatively larger orbifold eigenset, that is moving gradually into the general region in which the initially so-stated bosonic superstring of discrete quantum energy -- that works to bear basically just enough of a cohesive attractive force, seeing that such a said relatively larger orbifold eigenset in this respective given arbitrary case -- is of such a relatively mild genus of as to being what may here be called a group-attractor that is at the substringualr level.  Let us next say that the combined interdependent Fourier-based activity of the initial kinematic motion of the so-stated solitary bosonic superstring, with the relatively in-coming Fourier-based activity of the kinematic motion of the so-stated relatively larger orbifold eigenset -- works to bear an ever increasing core-field-density of such a genus of Rarita Structure eigenstates, to where this latter-stated Laplacian-based condition of an increase in the Hodge-Index of the holonomic substrate of gravity-based indices, will act in this case as a tense of an ever increasing state of magnetism.  This is since this so-eluded-to genus of an increase in the Hodge-Index of Rarita Structure eigenstates will work to form an ever increasing genus of the presence of interactive Fourier-based Schwinger-Indices, or, in other words, this will work to form an ever increasing genus of the presence of interactive Fourier-based gravity waves.  This genus of a relative build-up of magnetism -- as to the so-eluded-to manner of an increase in the scalar magnitude of characteristics that are directly affiliated with the propagation of both gravity and gravity-based waves -- will tend to form an initial Yukawa Coupling upon this here attracted superstring of which had here acted initially as its own orbifold eigenset, that will "pull" this from the initial state of just being in the Ward-Derichlet bounds of the second so-stated orbifold eigenset, which is of a relatively larger Hodge-related size -- into being in the actual Ward-Neumman and Ward-Caucy-based physical bounds of the so-stated relatively larger orbifold eigenset, that I have discussed in this respective given arbitrary case.  Such a "pull" is actually the "push" that is here to be most directly due to the here increasing influx of that genus of Rarita Structure-based indices that are increased in the amount of their presence in a euclidean-based proportion to the here present increase in magnetism.  Once the here discussed interdependent interaction between these two said orbifold eigensets converges into a relatively more conformally invariant-based nature, then, it may be said that the configuration of the proximal localized eigenmembers of such a case have then become as one overall orbifold eigenset.   I will continue with the suspense later!  To Be Continued!  Sincerely, Sam Roach.