Part Three of The Solutions to the Last Test of course 13

7)  If a one-dimensional superstring is swivel-like shaped in such a manner in so that the anharmonics of its spurious vibrations that the said superstring potentially displays between itself and its counter-string is not isometrically in terms of cyclic in the rhythm of the eluded to covariance that exists between the said counterpart, then there is an identical potential of the stated one-dimensional superstring to become tachyonic.  Any other of such covariant Chern-Simmons singularities here cause the same general effect.

8)  If a two-dimensional superstring is swivel-like-shaped -- in such a manner in so that the anharmonics of the spurious vibrations that the said superstring displays, between itself and its counter-string, (even though a two-dimensional superstring vibrates harmonically at its correlative Poincaire level) are potentially not isometrically cyclical in the rhythm of the eluded to covariance that exists between the said two-dimensional superstring and its counterpart, then, there is an identical potential of the stated two-dimensional superstring to become tachyonic.  Any other of such covariant Chern-Simmons singularities here will cause a spontaneously tachyonic effect.

9)  Light-Cone-Gauge eigenstates bear an angling from a given arbitrary superstring to its counterpart that bears one form or another of a genus of orphoganation with the connectivity of the directly corresponding superstring with its counterpart, if the said superstring is orientable.