In General -- How Chern-Simons Invariants Are Embedded

Here is, in general, how Chern-Simons Invariants are embedded upon the basic forces of nature:

An orbifold eigenset has a tendency of "wanting" to move in its intrinsic holomorphic direction, over any one given arbitrary respective evenly-gauged Hamiltonian eigenmetric.  Those superstrings of discrete energy permittivity, that work to comprise any one given arbitrary set orbifold eigenset, will tend to work to have the same intrinsic holomorphic tendency as the said respective orbifold eigenset, that such said superstrings are here to work to form.  Since the said respective strings are to tend to exist in a delineation, that is here to be placed, in general, at the external outer shell of such a said given arbitrary orbifold eigenset, -- even if the said orbifold eigenset is to be moving in a manner that is completely hermitian, and thus of a De Rham cohomology-related nature, -- the said strings will tend to not to be able to move in as much of a hermitian-related manner, in as these would intrinsically "want" to be moving in, over the earlier inferred given arbitrary respective evenly-gauged Hamiltonian eigenmetric.  This will then consequently result in the condition, that these said superstrings of discrete energy permittivity that are here to work to comprise the said directly corresponding orbifold eigenset of such a case, will then tend to work to consistently bear, what may here be thought of as the correlative presence of Chern-Simons singularities.   This will then work to result in what may logically be thought of, as the proximal local presence, of what may be termed of as being Chern-Simons Invariants.  As the said composite strings are here to help to work to form the proximal local presence of cohomological eigenstates, over time, this will then work to result in the formation of the earlier inferred Chern-Simons Invariants, that work to be formed by the motion of the said strings upon their directly corresponding Hamiltonian operand -- via the tense of the presence of either their Lagrangian-based Chern-Simons singularities and/or the tense of the presence of their metric-based Chern-Simons singularities, to work to act upon the directly corresponding Rarita Structure eigenstates.  This will consequently result in the action of the presence of such Chern-Simons Invariants, to work to bear a multiplicit Yukawa Coupling upon those Schwinger-Indices, that work to act -- in so as to help in working to form the basic forces of nature.  Such said respective Schwinger-Indices are formed by the "plucking," like a harp, of the multiplicit gauge-boson eigenstates, upon their correlative second-order light-cone-gauge eigenstates.  This effect of the action of the proximal local presence of the inferred Chern-Simons Invariants, upon those Schwinger-Indices that work to help in forming the basic forces of nature, are consequently to act in a multiplicit manner, in general,  as an embedding-related operation, upon the inferred basic forces of nature, -- in so as to work in a multiplicit manner, in so as to form the seven basic influences of physical nature.  To Be Continued!  Sincerely, Samuel David Roach.
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