The Next Part Of "Entropic Photons"

Let us consider what tends to happen, over the course of the third set of 64 consecutive iterations of group-related instanton, that start from the moment that the respective given arbitrary photon acted in so as to strike another holonomic substrate-based physical phenomenology, in a Gliosis-based manner, at the Poincare level -- up to the ensuing so-eluded-to iterations of group-related instanton, by which I am about to describe as happening.  In so long as the so-eluded-to "entropic photon" does not act in such a Fourier-based manner, in so as to strike another orbifold eigenset -- from the instant that the directly associated respective photon has worked in so as to make a direct and immediate contact with another orbifold eigenset-based phenomenology, up to the so-proscribed and the soon to be described set of what are to here be mentioned, as being of the successive series of iterations of group-related instanton, -- that go from the 129th consecutive iteration of such a successive series of instantons that start from the moment of impact, up to the 192nd consecutive iteration of the self-same successive series of instantons, that had started from the moment of impact -- the same "entropic photon" will be mildly partially Yau-Exact -- since only two of the holomorphic-based coniaxions of the torsional-based eigenindices, that are to here be related to the contorsioning of the holonomic substrate of the said "entropic photon," will bear a bending that is of a hermitian-based nature.  The rest of the holomorphic-based coniaxions of the so-eluded-to torsional-based eigenindices are here to bend in a Lagrangian-based Chern-Simons nature.  The light-cone-gauge topology of the said "entropic photon," will here be of an abelian or of a Kaluza-Klein nature, instead of being as a Yang-Mills nature.  This is in contrast to the light-cone-gauge topology of a non-entropic photon -- of which is of a Yang-Mills nature.