About The Ghost Anomalies Of Certain Heterotic Superstrings

The ghost anomalies of E(6)XE(6) superstrings in forward-time-moving-associated space are the residue of redelineated positive-norm-states that are redelineated by the motion of the said type of hetorotic strings per iteration of group instanton.  As positive-norm-states are "bumped", the just mentioned physical memory of the motion and existence of the said E(6)XE(6) strings is formed. This redelineation of the said format of norm-states works to form ghost anomalies that work to show the directly related pattern of both the motion and the condition of the said heterotic strings as these move through their respective Lagrangians over a given arbitrary duration of Real-based time.  Over a transient period of time after the said ghost anomalies of the said heterotic strings is formed, there are negative-norm-states that scatter the ghost anomalies just discussed in so that the arrangement of the distribution of the directly related positive-norm-states is scrambled into a real-based residue per iteration of group instanton.  Such scattered ghost anomaly-based indices that are here scattered will then tend to be pulled toward the relative interior of the directly related orbifold and/or the directly related orbifold eigenset that is arbitrarily being considered here.  The ghost anomalies of E(8)XE(8) superstrings tend to be "shuffled" toward the relative exterior of its directly associated orbifold and/or orbifold eigenset, or, sometimes toward the immediate exterial field that works here to be adjacent to the directly related orbifold and/or orbifold eigenset.  Just as with E(6)XE(6) superstrings, the directly related ghost anomalies that the said E(8)XE(8) superstrings form is created by the said Yakawa-based interaction of forward-moving norm-states with the said E(8)XE(8) superstrings right before the directly associated iterations of group BRST.  Again it is the eluded to backward-moving norm-states that work to scatter the eluded to ghost anomalies that are then formed here.  The scattered ghosts of E(8)XE(8) superstrings that are not directly impending to fray and the scattered ghosts of E(6)XE(6) superstrings that are not impending to fray always tend to bear no Gliossi-based Yakawa interaction with the ghosts of superstrings of discrete energy permittivity UNLESS there is a definitive cohomoligical index that is here used to pull these into their direct ghost-based field by the holonomic substrate of a directly related group attractor.  Again, with forward-moving-time-based substringular activity, it is the positive-norm-states that form ghost anomalies and it is the negative-norm-states that scatter ghost anomalies.  With backward-moving-time-based substringular activity, it is then the negative-norm-states that form ghost anomalies and it is the positive-norm-states that scatter ghost anomalies.  I will continue with the suspense later!  Sincerely, Sam Roach.