Saturday, December 27, 2014

Part One of the Seventh Session of Course 18

Superstrings exist in fields.  Any given arbitrary one-dimensional superstring of discrete energy permittivity and/or any two-dimensional superstring of discrete energy permittivity will always bear a tense of a fractal of magnetism -- in terms of their spin-orbital momentum, when this is taken in relation to their Hamiltonian-based operation, over time.  The said fractal of the given arbitrary discrete magnetism -- that may be extrapolated, for any given arbitrary relatively conformally isolated superstring -- can not propagate through a discrete Lagrangian, over a codeterminable group metric that is Majorana-Weyl invariant, without at least bearing one eigenbasis that is directly related to one or more Njenhuis tensors -- on account of the condition that the total spatial dimensionality of the most basic Majoran-Weyl fractal of magnetism, in terms of the functionability of whatever the directly associated Hamiltonian-based operation of the so-eluded-to superstring, that one may here consider in this case, happens to be, is based upon the kinematic covariant codifferentiability of a core-field-density that will always work to involve two or more spatial dimensions at once -- over any given arbitrary sequential series of group instantons in which the so-stated superstring of discrete energy permittivity will be involved with, over time.  It takes at least three or more spatial dimensions, in any kinematic inter-play of superstrings, to propagate a fractal of magnetism, in a directly correlative Hamiltonian-based operation, so that a cubic genus of a Gaussian Transformation may work to fulfill anywhere from a freedom of 4pi degrees of radial Ward-Neumman potential delineation to a freedom of 32pi I degrees of radial Ward-Neumman potential delineation, in order for the directly corresponding norm-conditions to exist in such a manner in so that at least all of the correlative directorals of the here relative Real Reimmanian space may be viably functional by the so-eluded-to given arbitrary tense of the here given case of the fractal of discrete magnetism, over any kinematic eigenbase of Hamiltonian-based operation.  Think about it.
I will continue with the suspense later!  Sam.

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