Monday, October 19, 2015

On The Format of Njenhuis Charges In General

Let us here consider the Doubolt cohomological flow of a Njenhuis charge -- that may be mapped-out in a Laplacian-based manner, after the overall motion of the said charge, over the so-eluded-to ghost-based pattern -- that such a respective given arbitrary relatively Imaginary charge is to make, over a relatively transient period of time.  Let us now think of the condition of a given arbitrary Njenhuis or Imaginary charge -- a charge that is orphoganal to a certain Real-based charge, to where this Real-based charge, of which is propagated through a discrete Lagrangian, is here being propagated as such, over time.  Let us now say that the so-stated Real-based charge is propagated as a Rham-based cohomological flow, while, the here tangent Njenhuis flow of charge, that is normal to the plane of the flow of the Real-based charge, is initially hermitian, yet, is of a relatively Doubolt nature -- due to it being orphoganal to the here relatively Real Reimmanian Plane.  Let us now say, that the so-mentioned Njenhuis flow of charge is pulled into a condition -- in so as to form a  Lagrangian-based Chern-Simmons singularity, in its cohomological wave-based pattern -- in so as to here work to pull the so-stated Njenhuis flow of charge (that is here of a discrete nature) -- in a manner that is normal to its Li-based Gaussian plane of flow.  The tendency of this, is to often be able to make -- what was directly previously a tense of a Njenhuis flow of charge -- to act to then at least become, in a transient manner, a tense of a flow of a relatively Real-based charge, for a certain potentially extrapolatable sequential series of group-related instantons -- as this may be mapped-out over a tracing of the here so-eluded-to Doubolt cohomological pattern.  This may then happen in so as to then work to become of the nature of a Rham-based cohomology, from the time after that such a flow of charge is converted into a Real Reimmanian-based charge that is to happen here, after the earlier so-mentioned formation of the said given arbitrary genus of the here respective Lagrangian-related Chern-Simmons singularity that I had mentioned -- until there is  either an effectual Yakawa Coupling that woks to form an additional Lagrangian-based Chern-Simmons singularity, or, until there is an effectual Yakawa Coupling that works to form a metrical-based Chern-Simmons singularity.  This genus of occurrence may be mapped-out, over the formation of the here directly related ghost-based cohomological pattern, over time.
I will continue with the suspense later!  To Be Continued! Sincerely, Sam Roach.

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