A Start As To Rham Cohomologies

When a superstring travels through a projection via any given arbitrary trajectory, it produces a physical memory in the form of ghost anomaly-based indices.  When a given arbitrary superstring travels straight through a unitary Lagrangian, it may often bear a hermitian delineation of physical memory in the form of a ghost anomaly-based formation of traceable mapping, that here bears no Chern-Simmons singularites.
This is considering the said given arbitrary superstring, when in terms the supplemental distribution of the corresponding ghost-based indices that, here, form an integrable linear trace as to where and how the said given superstring had moved in the relatively transient past sequential series of iterations of group instanton.  Such a path -- more than likely -- will not trace a Wilson linearity through the non-time-oriented Lagrangiann of the multiplicit coniaxial of the traceable mapping of the strings previous motion.  This is because, even at the Poincaire level that is adjacent to and/or Gliossi to any actual superstrings, space-time-fabric bends to an extent.  Yet, the supplemental basis of a physical memory of the mapable trace, as to where and how such said superstrings had kinematically differentiated over time, is said to be hermitian if the activity of the directly corresponding superstrings bears only as many changes in the derivative of its motion as the number of spatial dimensions that it is traveling in over time.  And, if the said superstrings pulse harmonically, then, the given superstrings are said to be kinematically differentiating in the just mentioned hermitian manner that bears no spurious-based conditions  -- as can be related to the eluded to group of superstrings that are being considered here.  The just mentioned general format of substringular motion is said to then bear no Chern-Simmons singularities.  Any ghost anomaly that bears such a genus of a traceable mapped-out holonomic path is said to bear a Rham cohomology, of which exists here between the individual ghost anomaly-based indices that come together in so as to form the eluded to extrapolation of what tends to be a relatively straight, or jointal, format of a smoothly curved physical memory of the described general format of superstring -- if the directly corresponding format of mapped-out tracing is not perturbated by its exterial-based surroundings.  Again, as a reminder, ghost anomalies include the immediate field of their multiplicit directly corresponding field -- that is Gliossi to the Poincaire level of such given arbitrary superstrings. This is why a world-sheet and the ghost anomalies that it forms always exists in one more spatial dimension than than the dimensionality of its directly corresponding superstring that works to form it.   I will continue with the suspense later!  Sincerely, Samuel Roach.