Tuesday, October 7, 2014

Part One of the Fifteenth Session of Course 17 About the Ricci Scalar

When we think of electromagnetic or electrodynamic energy, we tend to think of light.  Light always has some Chern-Simmons singularities, when this is considered in the topological framework that works to form the light.  So, electromagnetic or electrodynamic energy always some Chern-Simmons singularities in the cohomological framework of the mappable tracings that work to form the eigenbase of the said electromagnetic or electrodynamic energy.  Let us think of a beam of light in a vacuum.  The so-stated light in the said vacuum is unscattered, and propagates at 3*10^8 meters per second, here.  The said light here consists of an orbifold eigenset and its directly affiliated world-sheets -- in so as to bear the holonomic existence of the said light itself, and its mappable tracing.  The orbifold eigenset that works to be the eminence of the said here existent light will here act in a conformally invariant manner, and all of the here metrical-based singularities that would here exist among the orbifolds that work to comprise the orbifold eigenset of the so-stated light will bear a genus of a Chern-Simmons eigenbase.  (This is because, although light travels as straight as it is able to, in a Lagrangian-based manner, the pulsation of a beam of light varies in its vibrational-based oscillation, over time -- in so as to produce metrical-based  Chern-Simmons singularities.)
 I will continue with the suspense later!  To be Continued!  Sam.

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