A Helpful Tidbit

The relative spacing increments of gauge-bosons -- which work to form the respective delineations of the so-stated gauge bosons, upon the just-eluded-to second-ordered light-cone-gauge eigenstates -- depends upon certain factors.  First, there is the factor as to the directly prior sequential series of Lorentz-Four-Contractions that had just recently, in any given arbitrary case that one may here be dealing with, been implemented upon the directly corresponding respective said second-ordered light-cone-gauge eigenstates.  For instance, if any certain given arbitrary superstring has just decreased, in a strong euclidean manner -- in terms of the scalar amplitude -- in its directly associated Lorentz-Four-Contraction, then, this manner of a strong decrease in contraction will here work to form such an alteration in the correlative Clifford Expansion of its respective delineations of its corroborative light-cone-gauge eigenstate, in so as to tend to "toggle" the directly corresponding gauge-bosons, from the here eluded-to initial staggering of delineation, into a distribution-based toggling that would then here work to pull the said gauge-bosons in the relative reverse-holomorphic direction.  Another condition that often may work to perturbate or alter the respective relative delineation of gauge-bosons from their initial distribution characteristics, in a sequential series of instantons, would be the isometric torsioning of a superstring.  If a superstring is pulled or tugged -- even if both the respective Lorentz-Four-Contraction is here to remain constant, and the respective conformal dimension of both conditions of such a superstring are here of the same Hodge-based index, the just-eluded-to torsioning may often work upon the respective relative delineatoroy index of the just eluded-to superstring.  The alteration of the delineatory index of a superstring, over time, can work to alter the distribution of the correlative gauge-bosons that work to act upon their respective second-ordered light-cone-gauge eigenstates.  One other factor that I will mention here, that can work to alter the delineation of gauge-bosons upon their stagger-based distributions -- upon their relative topological-based locus of their correlative second-ordered light-cone-gauge eigenstates, is any given arbitrary change in the Hodge-based conformal dimension of the said given arbitrary superstring.  For instance, if a superstring goes from a bosonic-based topology of holonomic substrate into a fermionic-based topology of holonomic substrate, or vice-versa, then, this alone will cause a shift in the whole general basis of the respective so-eluded-to format of the delineations of the so-stated gauge-bosons -- upon the general topology of the respective given arbitrary superstringular  phenomenon of such a case.
To Be Continued!  Sam.