Thursday, December 12, 2013

Cohomology Pull

Often, a cohomology that works to inter-bind two different ghost anomaly-based patterns is pulled by a discrete substringular holonomic entity of physical substrate that is not of the phenomena-basis of either being a norm-state or a norm-state projection, that is tugged kinematically over some sort of a Lagrangian-like via homotopic residue over time.  When a cohomology is pulled kinematically through such an eluded to Lagrangian over time -- by some sort of superstring, then, it takes a different basis of either a norm-state or a different basis of norm-state projection to be able to move accordingly in a relatively reverse-holomorphic manner, in so as to anharmonically scatter the said given arbitrary ghost-like pattern in such a manner in so as to work to convert the said ghost anomalies into that substringular residue that acts as a foundation for the future formation of gravitons and gravitinos that may be able to form specific Hamiltonian-based operational-based functions via the correlative interactions with the Rarita Structure via the physical tensoric amplitude of the Ricci Scalar.  Cohomologies that are only partially anharmonically scattered via relatively reverse-holomorphic norm-states and/or norm-state projections may often interact with either discrete phenomena of substringular energy and/or other ghost-anomaly-based patterns over a relatively transient period of time -- over a sequential series of iterations of group instanton.  This often works to involve an initially Gliossi-based Yakawa Coupling that corresponds to a torsional-based wave-tug/wave-pull of one of such ghost-anomaly-based patterns with another substringular entity that has not been completely anharmonically scattered off of the relative Real Reimmanian plane.  As such a wave-tug/wave-pull tends to be relatively abelian.

No comments: