Genus-Bases For Chern-Simmons Indices

For every additional axial-related directoral-based sway that the said traversing path that is being mapped-out via a Fourier Transformation, there is an added degree of indiscrete tensorism that is involved with the here corresponding singularity format.  For instance, if a trace that a superstring is being projected through curves through a kinematic path that is moving through a binary coaxial plane, and the said trace vibrates back-and-forth in five different codifferentiable axials over the group metric that involves the related Fourier Transformation in which the corresponding superstring that is pulled through the mentioned trace, as it is swayed back-and-forth via a coniaxial that involves five different spatial axes that are redelineated along the kinematic-based mapping of the action of the mentioned trace, as it is going through its given arbitrary Lagrangian, then, the genus of the Chern-Simmons Index -- when this is in relationship to the here non-hermitian-based singularities -- will here then be of a third-ordered euclidean Hamiltonian operator.  This is on account of the condition that five axials minus two axials forms three axials, and, the existence of a tritiary coniaxial-format that extends beyond the hermicity capability of the given trace, when given the scope of the here present differential geometry, will form singularites that will here involve limits that are tantamount to numbers that are based on both infinity,infinity squared, infinity cubed, and infinity^4.  The Reverse-Dirac functions of such singularities would thus be involving limits that are tantamount to numbers based on both (0+),(0+^2),(0+^3), and (0+^4).  I have got to go now!
I will continue with the supense as soon as I can.
Sincerely,
Sam Roach.

Some Stuff About Gauge-Bosons

Gauge-Bosons are essential in the field of a light-cone-gauge-eigenstate since, when

                
individual gauge-bosons "pluck" the second-ordered light-cone-gauge-eigenstates that

exist in the 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 to allow for the Ricci Scalar to function so that gravity may

take effect. This is just in reference to the E(6)XE(6) type of gauge-bosons. Just as

adjacent electrons have to spin antisymmetrically, to give a reverse-fractored 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 antisymmetric spin-orbital tensorism is caused by the spurious effect of the 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 abelian or non-abelian, the substringular

field that binds these gauge-bosons to both sides of an associated first-ordered-light-

cone-gauge-eigenstate is primarily abelian so that the "plucking" of the second-ordered

light-cone-gauge-eigenstates will not shatter the given first-ordered light-cone-gauge-

eigenstate. The fabric of substringular field is what I call "mini-string." Mini-String is

the fabric of gauge-action that interconnects the topology of all unfrayed substringular

phenomena that forms the homotopic structure of the substringular. My website is http://

www.samsphysicsworld@blogspot.com.

Sincerely,

Samuel David Roach