Part Two of the Just Started Session of Course 16

At this point, consider the directly associated Regge Slope eigenstate that corresponds to the given arbitrary superstring and its correlative counterpart, as the kinematic activity of the so-stated Regge Slope eigenstate happens during the gauge-metric of the integrand locant-based metric -- that would here be directly associated with the iteration of group instanton that corresponds to the portion of the duration of the said multiplicit instanton, that happens right after the corresponding metric or sub-metric of BRST -- during which the so-eluded to superstring is then here redelineated in such a manner in so as to be able to potentially "grasp" another chance to be able to be orientable.  This is if the case in the given arbitrary scenario, if it is that the given so-stated superstring was unorientable over the directly prior eigenmetric of that Bette Action index, that happened over the eluded to iteration of the simultaneous eigenstate of Polyakov Action -- the two different geni of kinematic activity mentioned here, of which happens at the same general duration when taken through the vantage point of a central conipoint in space.  Now, try to think about the Gaussian conditions of the differentiable subspaces of the said string, as it works to correspond to its directly associated superstring and its counterpart -- over the course of the iteration of the eluded-to eigenmetric of Regge Action.  The trajectoral path of the Regge Action is the Regge Slope.  If the supplemental delineation of those waves of core-field-density that are outwardly extended by the said prior kinematic activity of the directly corresponding Bette Action eigenstate -- as these densely distributed segments of mini-string, that bear a certain degree of torsionability, via the activity of the said eigenstate of the Polyakov Action -- will bear indices that work to orientate the directly affiliated Rarita Structure eigenstates that are most local to the activity that I am describing, on account of the "effort" of the said superstring, to bear a certain degree of renormalization with its counterpart.  If the resulting Gaussian of the just eluded-to inter-relationship works to bear an even function of wave-output --that extends from the general center-state, that may be subtended from in-between the so-stated superstring and its counterpart, over the so-stated Regge Action, then, there will be a genus of homeomorphicity that will then form between the said superstring and its counterpart, as this eluded-to phenomenology is pulled through the said Regge Slope eigenstate, which will make the superstring orientable.  If there is, instead, an odd function of wave output that extends from the so-stated center of substringular interaction, then, the superstring will remain as unorientable, and thus, the superstring will here become tachyonic.