Some Stuff About Doubolt Cohomologies

When a superstring and/or a group of superstrings travel through a unitary Lagrangian, in such a manner in so  that there are more changes in the derivatives of its or their motions, respectively, than the number of dimensions that the set of superstring or superstrings are going through spatially, then, the cohomology of the world-sheet or sheets, as extrapolated by the eminent ghost anomalies that thence form, is said to bear what are said to be Chern-Simmons singularities.  If any of such superstrings, or group of superstrings, is to bear a hermitian path that is spurious -- the pulse of the eluded to orbifolds has anharmonic modes that are exhibited during the projection of its trajectory -- then, the said superstrings and/or set of superstrings is still said to bear Chern-Simmons singularities.  The cohomology of any ghost anomalies that bear Chern-Simmons singularities are said to have a Doubolt cohomology.  The extrapolation of a Doubolt cohomology is the sequential-based mapped-out trajectory of the physical memory of world-sheets -- that are the trajectory of superstrings -- that are appertaining to bearing Chern-Simmons singularities.