The Very Next Part of Session Five of Course 19 -- The Klein Bottle and Orbifold Differentiation

Let us now consider the Majorana-Weyl-Invariant-based field of the so-eluded-to given arbitrary orbifold, that I was beginning to describe earlier in this respective given session.  As the Majorana-Weyl-Invariant-based field that was so-mentioned, differentiates in a Fourier-based manner, as a mechanism that works to inter-relate a Hamiltonian-based operation -- that is of a spinning-twist-based torsion.   (The orbifolds that have here been brought into a conformally invariant-based setting -- bear a here relatively locally proximal, as well, set of spin-orbital Njenhuis tensors -- that operate in so as to kinematically differentiate off of here what is of the relative Real Reimmanian Plane, that is of the here directly corresponding Majorana-Weyl-Invariant-based field.  This happens, in so as to work to form a tense of a propagation, that is of the overall summed Hodge-Index -- that is of the Hamiltonian-based-operational fractals of the so-eluded-to magnetic field eigenbase of this respective given arbitrary case.  The here mentioned relatively proximal tense of indices -- that would here work to form the overall set of Hamiltonian operators, that would work in this case in so as to be what would here work to comprise the so-stated local fractal of magnetism, this of which is demonstrative in the set respective given arbitrary substringular neighborhood of this given case, acts, in so as to comprise that interconnection of the holonomic substrate of the said locally proximal orbifolds, that have here come together or integrated in so as to work to form the so-eluded-to regional orbifold eigenset of this respective given arbitrary case.  Theses said orbifolds, that have here come together in so as to form the given said orbifold eigenset -- are binded together via a tense of heterotic strings, that may be described of as E(8)XE(8) strings, these of which are of a heterotic nature, over time.  These said E(8)XE(8) heterotic strings, work to hold together the orbifolds of an orbifold eigenset, by proximally twisting as if these were gears, that operate in so as to bear a tensoric genus of substringular torque -- in such a manner that acts as is according to the scalar magnitude of the compactified slack of that wave-tug/wave-pull -- that acts here in an abelian manner, upon the holonomic substrate of the said heterotic E(8)XE(8) strings, these of which are, again an example of what are known of as heterotic strings.
To Be Continued!  I will continue with the suspense later!  Sincerely, Sam Roach.

A little extra as to the Importance of gauge-bosons

Gauge-Bosons are essential phenomena that exist in the field of a light-cone-gauge-eigenstate, since, when individual gauge-boson eigenstates work to  "pluck" the second-ordered light-cone-gauge-eigenstates that exist from within the Ward-Neumman-based field of a first-ordered light-cone-gauge-eigenstate -- the resulting vibrations are second-ordered Schwinger Indices (the summation of such vibrations per first-ordered light-cone-gauge-eigenstate, being a first-ordered Schwinger Index) that flow through the Rarita Structure, in so as to allow for the Ricci Scalar to function -- so that gravity may take effect upon substringular phenomenology, in general.  This is just in reference to the E(6)XE(6) type of gauge-bosons.  Just as adjacent electrons have to spin assymmetrically, to give a reverse-fractaled example, in order to obey the Pauli Exclusion Principle, -- adjacent E(6)XE(6) strings must bear an assymmetric spin-orbital tensorism, in order to not infringe on each others' space.  Such an assymmetric spin-orbital tensorism, is caused by the spurious effect of the metrical-based Chern-Simmons field, that exists between adjacent E(6)X(E(6) strings.  Such a Chern-Simmons field is due to the condition of such gauge-bosons -- differentiating per instanton, in-between a discrete energy unit of permittivity and a discrete energy unit of energy impedance.  So, whether a related light-cone-gauge topology is of an abelian or of a non-abelian light-cone-gauge-based nature, the substringular field that binds these gauge-bosons, to both sides of an associated first-ordered-light-cone-gauge-eigenstate -- is primarily of a Gliosis-based abelian nature at the Poincaire level, so that the "plucking" of the second-ordered light-cone-gauge-eigenstates will not be of the nature to be able to shatter the given first-ordered light-cone-gauge-eigenstate of any respective given arbitrary case.  The fabric of a substringular field, is what I call "mini-string."  Mini-String segmentation is the fabric of gauge-boson-based-action, that works to tend to be able to interconnect the topology of all unfrayed substringular phenomena, in so as to be able to work to help form the homotopic structure – that is of the general eigenbases of the substringular.  My website is http://www.samsphysicsworld@blogspot.com.

Sincerely,

Samuel David Roach

Part Four of Session Five of Course 19 -- The Klein Bottle and Orbifold Differentiaition

The homotopic eigenbase of the conformally invariant-based, or steady-state, field, of any given arbitrary orbifold eigenset, is the Ward-Caucy-based covariant, codeterminable, and codifferentiable existence -- and also the Fourier-based activity -- of the directly corresponding Majorana-Weyl-related fluctuation of the so-eluded-to Ward-Caucy-based topological sway, that is of the summed respective given arbitrary substringular eigenmembers -- that have come together or integrated, in so as to operate as one Gaussian-based stratum of Hamiltonian Operators, that are here put into a covariant, codeterminable, and a codifferentiable locus.  This so-stated fluctuation, is here, locally, in a state of a relatively steady-state-based functionablity.  (This is the case -- whether there is a larger substringular neighborhood that this belongs to, that is in less of a state of conformal invariance, or not.)  Here is what I mean, by utilizing an alogorical example as an anectdote-based metaphore.  Let us say that one is to consider a person who is standing "completely" still on earth.  His or Her body is here in a local tense of a relative condition of being in a steady-state-based mode.  Yet, the said person exists on a planet that is moving a lot more rapidly in its rate than the so-stated person is moving -- in this case.  Likewise, a relatively local Poincare-based substringular neighborhood, may be in a tense of conformal invariance -- even though a more macroscopic or largely considered region -- that is to include the so-eluded-to initially stated substringular neighborhood, may be existent in a less conformally invariant -- or even in a relatively perturbative -- tense of its conditions, of relative covariance, when one is here to consider an observer who would be then considering a more macroscopic external viewpoint.
So, the tense of a relative given arbitrary Majorana-Weyl-Invariant-Mode -- is generally in consideration of the locally covariant Poincaire behavior of substringular events, at the cite of the relatively local environment -- whether or not there is an external perturbative state that is at a less microscopic perspective as to where one is to here consider the eigenbasis of the respective given arbitrary Poincaire level, or not.  To Be Continued!  I will continue with the suspense later!
Sincerely, Sam Roach.