More Stuff About The First Session Of Session One of Course 16

Higgs doublets are a dual condition of world-sheets of bosonic or closed-strings that bear a low-energy momenta in a common field band, that would  detectabley appear as two trajectoral paths of  bosons that merge at their tops.  This "merging" is the redistribution of the tops of the directly corresponding superstrings that exist as such after relatively many iterations of group instanton.  This forms a tubular world-sheet at their tops that shares a common band.  Yet, the just mentioned common band is unnormalized, seeing that the differing positions of their correlative Planck-related phenomena are not homogeneous -- when in terms of the flow of the hermicity that may be extrapolated along the eluded to path that works to trace the Lagrangian that may be mapped along the projection of the ghost anomalies that eigenstates of such world-sheets work to form.  This makes what I just termed of as a Higgs doublet to be as a unique form of a Chern-Simmons-based cohomology.  This would then make a Higgs doublet eigenstate a specialized genus of a Doubolt cohomology.  I have here described a Higgs doublet as a Chern-Simmons-based cohomology, on account of the condition that those superstrings that work to form the ghost anomalies that directly correspond to the said general phenomenology of a Higgs doublet differentiate kinematically in so as to virtually touch in a Gliossi manner -- to where any given arbitrary Higgs doublet eigenstate is an example of a Yakawa Coupling that does not directly form in the manner of a borne tangency.  This happens in such a manner in so that the directly affiliated format of cohomology that I am here discussing bears a spike in the non-time-oriented translation of the tracing of its Lagrangian, via the trajectory of its projection, due to the condition that the said genus of Ward-Neumman-bound ghost anomaly-based phenomenology bears a directoral path -- this of which may be termed of as Imaginary or Njenhuis.  This latter condition is since such a tracing of this given arbitrary genus of ghost-based projection is pulled at a general conilocus of delineation that is off of the relative Real Reimmanian plane for each of such eigenstate of the said genus of ghost anomaly-based phenomenology that may be here termed of as a Higgs doubled eigenstate.  I will continue with the suspense later!  Sam Roach.