Part Two Of Genus-Bases oF Chern-Simmons Indices

The reverse-holomorphism of the previously mentioned singularities would thus be -infinity,
-infinity^2, -infinity^3, and -infinity^4, -0+, -0+^2, -0+^3, and -0+^4 -- respecitively.  This is based on both the singularities that here refer to a hermitian case and also those singularities that here refer to a non-hermitian case. 
When singularities are based on spuriousness, each truncated jerk in the accelleration/decelleration of the related vibrations of the said trace fors a 0+ based singularity (if holomorphic and in one normal coniaxial framework).  If the related holomorphism is reversed with the initial conditions of what here works to define a positive directoralization, then, the singularity is based on 0- instead of 0+.  If more axials vibrate than that which allow for a condition of hermicity, then, for each added covariance, multiply the truncation-based singularity by 0+ -- for positive holomorphicity, or 0- -- for negative holomorphicity.  This is for one eigenmetric of truncated anharmonic sway.  Ellongated jerks involve the  same concept, yet here involving a multiple of singularity of infinity+ -- for positive holomorphicity, or infinity- -- for negative holomorphicity.  Indiscrete scalars may be multiplied by the values of singularity when there is a given set of conditions of an additional lack of hermicity.  For instance, if a trace similar to what I have mentioned is different on account of changes in all 32 spatial dimensions that are inter-twined in one given set of parallel universes that this situation would here refer to -- and also, if during a set of iterations of instantons that correspond to the directly related Fourier Transformation, the trace of a kinematically projected superstring bears an anharmonic sway that is ellongated during a gauge-metric that is part of the overall group metric in which the mentioned trace is vibrating, then, the superstring, in the course of kinematically traversing the said trace, will bear a singularity of infinity^31*infinity -- or, infinity^32.  Yet, if the mentioned trace that here changes in all 32 spatial dimensions bears an anharmonics that is briefly truncated in a gauge-metric that happens during the same overall group metric in which the said trace is vibrating, then, the trace will here bear a singularity of infinty^31*(0+) -- or, infinity^30.  In both cases, the Chern-Simmons index will bear a genus of 30.  (32-2=30.)  As another example, if the same type of trace that changes in all 32 spatial dimensions of its set of parallel universes is truncated in what may be here described arbitrarily as the negative direction, then the overall singularity that it will bear will be infinity^31*(0-) = infinity^(-30).  As one last example for the day, if the said just mentioned trace bears an ellongated anharmonic sway in the "negative" direction during a gauge-metric that exists within the locus of the extrapolated vibration of the said trace, then, its corresponding singularity at the junction of the change in its dimensionality will be infinity^31*(-infinity) = infinity^(-32).  That's all for now.  I will continue with the suspense later!  Sincerely, Sam.