Part Two of the Fifth Session of Course 18

The process of the first-ordered point particles -- that have worked to comprise a superstring of discrete energy permittivity -- to partially dissociate into a format of holonomic substrate, that is relatively loosened from its initial genus of composition, that had existed at the beginning of any given arbitrary substringular state that exists at the start of one locus of one given arbitrary iteration of BRST, is called the Polyakov Action.  After many sequential iterations of group instanton -- more particularly, after many sequential iteration of group-related BRST -- the directly associated superstrings of discrete energy permittivity either gradually and/or more immediately alter in their  tense of directoralization and position, over the so-eluded-to general conditions of time that will have here been allotted.  As superstrings of discrete energy alter in the Hamiltonian-based indices that are correlative to a fractal of what may be termed of as the indices of their eigenbase of angular momenta over time -- the diretoral-based wave-tug/wave-pull of the directly corroberative superstrings will tend to alter in their individually considered Lagrangian-based path as to what will then be the newly-extrapolatable holomoprhic direction of any respective given arbitrary  superstring that will have then altered in the base as to the path integral genus as to the physical-based inclination as to the Hamiltonian-based operand that is most optimum for maximum physical-based rest. And, as the optimum fractals of both the angular momentum and the spin-orbital momentum of any given arbitrary respective individually taken superstring works to bear a directoral-based eigenbase of Hamiltonian operation that has altered in its most liable Lagrangian-based path integral over time,  the correlative Polyakov Action eigenmetric of the so-eluded-to superstring will be at least partially affected by the prior-based kinematic-based activity -- which will, at least to some degree or another, alter the manner in which the directly associated first-ordered point particles that work to comprise the correlative superstring of discrete energy permittivity act, in the details by which such constituent so-stated particles behave -- in the process of the so-stated mild dissociation, so that these may undergo such a change,  in so as to allow for the said process of the said eigenstate of the Polyakov Action. This just implied transformation in the manner of Polyakov-based nature is related to the degree and the manner of the correlative Lorentz-Four-Contractions that are applied to the so-eluded-to superstring, of any respective given arbitrary specific substringular case that may be individually considered.  Often, such a perturbation in the said Polyakov Action will ebb back-and-forth from one genus of condition to another of such a condition.  Such topological-based sways -- that are related to the activity of a Polyakov Action eigenmetric -- will always bear a state of multiplicit directoral-based indices that are pulled in some sort of oscillitory-based pulsation, over each of such individually-based gauge-metrics.  When the activity of a local respective Polyakov Action eigenstate -- that is individually considered in a specific scenario -- does the so-stated genus of ebbing that I have recently mentioned, then, this conformally invariant genus of local field delineation may be termed of as a relative conformal Polyakov field transformation.  Yet, such a so-stated transformation is often altered by an exterial interactive state that acts upon a respective superstring that had initially began in the initially stated manner.  When such a superstring is altered in this latter-based format of activity by an exterior Hamiltonian operator, the resultant kinematic activity may be viewed of as a divergent Polyakov field transformation.