More About the Activity of the Light-Cone-Gauge

During BRST, which is the main part of a duration that is known of as instanton, superstrings and their counterparts go thru a gauge-metric that I call the Imaginary Exchange of Real Residue.  During this activity, the substringular fields, appertaining to superstings that are discrete units of energy permittivity, that interconnect superstrings with their counterparts -- the field eigenstates which are in the form of mini-string segments -- cause a wobbling motion that initially moves the counterparts of arbitrary superstrings in the forward holomorphic direction while counter-wobbling the corresponding superstrings in that same given forward holomorphic direction.  Such a gauge-metric consequently moves the given corresponding superstrings to wobble back in the associated reverse holomorphic direction while counter-wobbling the corresponding superstrings in the corresponding reverse holomorphic direction.  This happens while the Polyakov Action and the Bette Action are taking place.           
During the simultaneous activities of the Polyakov Action and the Bette Action, the associated superstrings and their corresponding counterstrings alter in scalar relative size via the increase of substringular wave or mini-string segment scalar increase in such a way that the associated superstrings and their corresponding counterstrings largen just enough to be at the length (for 1D strings) or circumference (for 2D strings) that corresponds to how small the associated Lorentz-Four-Contractions are.  As an example, if the Lorentz-Four-Contraction upon a given superstring is zero, then, the associated 1D strings increase during BRST in length by a factor of 3*10^8.  Or, as another example, if the Lorentz-Four-Contraction upon a given 2D string is zero, then the circumference of the associated superstrings increases by a factor of 3*10^8.  This is done with a maintainence of homotopy on account of mini-string being brought into the Gliossi field of where the mentioned superstrings and their counterstrings are at.  Once the corresponding superstirngs and their counterstrings have wobbled back into their original general locus via the reverse holomorphic wobbling of the associated counterstrings counter-wobbling the corresponding superstrings, the effect of this activity springs superstrings and their counterstrings into the Regge Action while then going into Ultimon Flow directly afterward, if their is no Kaeler-Metric during the course of the associated eigenstate of instanton.  If Kaeler-Metric is to happen during a particular arbitrary eigenstate of instanton, then, immediately after BRST, the mentioned superstrings initially enter their corresponding Klein Bottle eigenstate-like phenomenon for half of the rest of instanton -- the superstings of which in the process recontracting to the size that these had directly before these had expanded on account of the Polyakov Action, due to the differential geometry of the norm-states that exist in the given Klein Bottle eigenstates -- while then the superstrings go into the Regge Slope via the Regge Action for the other half of the rest of the arbitrary given eigenstate of instanton.  What we tend to notice in terms of time is instanton, or, more specifically, the BRST portion of instanton.  BRST happens for
6hbar time, while the rest of instanton happens for ((2pi hbar)-(6hbar)) time.  We only tend to notice instanton on account of the condition that superstrings are at a relatively organized standstill during the individual eigenstates of instanton.  By far though, most substringular activity happens in-between the individual eigenstates of instantons.  The Klein Bottle eigenstates are organized to be at the proper location on account of:  1) The abelian propagation of the Wick Action that is tensorically directoralized via the harmonics of wave-tug of the corresponding Schwinger Indices that travel as vibrational eigenstates along the Rarita Structure.  2) The corresponding abelian propagation of the Landau-Gisner-Acion upon the associated  Douboult cohomological section of the Rarita Structure known of as the field where the Fischler-Suskind-Mechanism happens. 3) The abelin nature of the Higgs Action eigenstates upon their associated Klein Bottle eigenstates toward the resultant of the hermitian Ward path that moves in the path of most resistance to the general location where the Kaeler-Metric is to happen.  The combined activities mentioned in the prior are what cause the proper inter-relations that allow for the correct distributions of Klein Bottle eigenstates with their corresponding superstrings so that the superstrings that need metric-gauge -- as well as the superstrings that may also then need to change in light-cone-gauge topology --  may be properly organized so that Gaussian Transformations may happen appropriately.  Sam Roach.