Monday, January 12, 2015
Part Two of the Ninth Session of Course 18
After each successive iteration of group instanton, each individual superstring of discrete energy permittivity changes in its positional delineation by being redistributed. This general format of such a distribution is either of one Planck-Radii spin-orbital-wise (let us here arbitrarily consider this as the theta spatial manner of a degree of freedom), and/or one Planck-Radii in the here anterior radial degree of freedom (let us here arbitrarily consider this as the phi spatial manner of a degree of freedom), and/or one Planck-Length transversal-wise (let us here arbitrarily consider this as the rho spatial manner of a degree of freedom) -- in so as to concur with the Ward-Caucy-based condition, that any discrete unit of energy-based holonomic substrate is to be constantly re-distributed -- per each successive iteration of discrete time duration, -- in order for discrete energy to be accurately depicted as a constant flow of substringular phenomena that is not completely inert, in and of itself, in so long as such respective given arbitrary discrete units of holonomic substrate do not approximate a derivative of a here relatively superconformal set of superstrings of discrete energy, that would here otherwise be of a mass -- and a mass is a tense of energy that is in static equilibrium. A superstring of plain kinetic energy is of an open-loop, or, of a fermionic-based topological nature, while yet photons and mass-bearing superstrings of discrete energy permittivity are bosonic. This is due to both the condition that the Fujikawa Coupling converts the kinetic energy that is released by an electron into a photon, and also because, when a state of freely perturbative kinetic energy is made to integrate with other superstrings -- in a manner that works to form an eigenbase of a group attractor eigenmatrix -- that is basically of a here local superconformal nature, then, the here initially fermionic-based superstrings of plain kinetic energy need to bear a higher genus of mobiaty, in order to work to pull the here holistic entity of energy, that is to be of a state of relative static equilibrium, into the so-stated tense of local superconformal invariance. Closed-Superstrings that are not of a heterotic-based nature tend to bear a conformal dimension of two -- in so long as one is here talking about superstrings of discrete energy permittivity. An open-loop topological-based phenomena, that is a unit of a holonomic substrate of discrete energy permittivity, has two loose ends that do not feed into each other in a homotopic Laplacian-based manner, yet, a closed-loop has no loose-ends -- since it feeds into itself in a homotopic manner, under the respective eluded-to Laplacian-based mapping of the topology of such a so-stated general genus of superstring. To Be Continued! Sam Roach.
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Labels:
eigenbase,
Fujikawa Coupling,
holonomic substrate,
Laplacian,
superconformal invariance,
superstrings,
Ward-Caucy
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