More About Heterotic Bosonic Superstrings

As both the Polyakov Action and the Bette Action happen simultaneously for their corresponding superstrings, the corelative light-cone-gauge eigenstates that directly correspond to the said superstrings are fed in mini-string so that the interconnection of the individual second-ordered light-cone-gauge eigenstates with their directly corresponding Fadeev-Popov-Trace eigenstates with their corelative superstrings mentioned may go through the process of their format of Clifford Expansion, in so that the activities that work to allow for what is known of as Lorentz-Four-Contractions may happen at the same general format of metric as when superstrings kinematically differentiate with their counterstrings.  This happens in a manner in which these said superstrings "attempt" to orientate in so as to be able to remain in the process of Noether Flow.  As the said second-ordered light-cone-gauge eigenstates go through their topological-based fed in expansion in order that superstrings may be able to arrange their relative length, time, and mass-equivalence relative to electromagnetic energy, the E(6)XE(6) heterotic-based superstrings move in the direction of the motion of that contorsioning of the holonomic substrate of the directly related second-ordered light-cone-gauge eigenstates, as this said genus of heterotic string moves in so as to "pluck" the given arbitrary mini-string that works to form the topological entity of the said second-ordered light-cone-gauge eigenstates without heterometrically or anharmonically torqueing the mentioned format of mini-string segments in the process of working to form second-ordered Schwinger Indices.  So, as gauge-bosons pluck light-cone-gauge eigenstates in order to form those vibrations that move along the Rarita Structure, in order to do various necessities -- such as causing the motion of the Wick Action, these move hermitianly and harmonically in the directoralization of the wave-tug/wave-pull of the topological substrate of the said light-cone-gauge eigenstates in so as to help fascilitate the smooth translation of Schwinger vibrations along that substrate that works to interconnect the given arbitrary relative Real Reimmanian plane considered in any given arbitrary case with the motion of rudimentary gravitational-based particles -- so  that both gravity and changes in substringular norm-conditions may be permanent.  To Be Continued!  Samuel David Roach.

Extra On The Higgs Action

When a Higgs Action reverses in relative directoralization, the “vacuumed pouch”

                    
that is Dirac relative to the Higgs Action hermitianly changes in its second derivative. It

will reverse the concavity of the mini-loop hermitian singularities that exist as the gauge-

action field sub-quantum that exist between a superstring and its associated light-cone-

gauge eigenstate. Look. As Kaeler metric happens, gauge bosons pluck the assocaitaed

second-ordered light-cone-gauge eigenstates, as is always the case during BRST. The

scattering of the norm-conditions in the Klein Bottle, also seeing that a superstring in the

substringular (fully contracted here) has a length (1-D) or circumference (2-D) of 10^

(-43) meters, inverts the vibratory holomorphicity of the associated Schwinger Index

away from the Rarita Structure. Such an inverted vibration increases the impedance of

a Fadeev-Popov-Trace while it allows for the increase in permittivity of the associated

superstring. Again, gauge-bosons have twice the circumference of a two-dimensional

regular superstring. Each Kaeler metric in a superconformal Fourier Klein Bottle

transformation during a Gaussian Transformation equally increases the metric-gauge

potential of the superstrings, while increasing the metric-impedance potential of the

superstrings’ associated Fadeev-Popov-Trace or Planck phenomenon related phenomena.                   

Part One of the Solutions To Test One of Course 5

1)  A Basis of Light has the shape of a hermitianly shaped-wise majorized Laplacian giant Planck Phenomena related phenomenon with an initially relatively small central "knot" that starts out just six first-ordered point particles thick.  The increase in size when one, in a Laplacian manner, goes from the center of such a Basis to the rest of the morphology of that Basis goes from an euler increase in holonomic morphology to more of a euclidean Laplacian delineation once the mapping of the described configuration is observed  to be co-determinant with the morphology of a spacially majorized Planck Phenomena related phenomena.

2)  Right after instanton, first-ordered point particles of superstrings scatter mildly into point commutators that, besides indistinguishable differences, tend to maintain a Fourier-based covariant localization during the Imaginary Time of Ultimon Flow.

3)  Residue of superstrings is never permanently squandered.  Even when superstrings go into a black-hole, their holonomic components eventually leave the said black-hole's torsioning apex as antimatter that eventually reorganizes into matter.

GUFT, The New Addition

A Higgs-Action is an example of a tiny particle that is smaller than a superstring. A one-dimensional superstring is
3*10^(-35) meters long when fully uncontracted and is 10^(-43) meters long when fully contracted. A regular two-dimensional superstring, besides gauge-bosons, has a circumference of 3*10^(-35) meters around when fully uncontracted and has a circumference of 10^(-43) meters around when it is fully contracted. A superstring is 10^(-43) meters long when it is one-dimensional in the substringular and a regular two-dimensional superstring besides gauge-bosons has a circumference of
10^(-43) meters around in the substringular. A Higgs-Action or an eigenstate of the Higgs-Action has a length when fully uncontracted, which is in the globally distinguishable, of 10^(-43) meters. A Higgs-Action or an eigenstate of the Higgs-Action has a length when fully contracted, which is in the substringular, of 3 and one-third * 10^(-52) meters. An eigenstate of the Higgs-Action is an oval type point particle-like structure that is conical at both ends while hermitianly curving from its center of 10^(-43) meters in the globally distinguishable and 3 and one-third * 10(-52) meters in the substringkular to its respective apexes at both ends of 3*10^(-78) meters in the globally distinguishable in thickness and 10^(-86) meters in the substringular. The associated hermitian-like quality involves a parabollic shape that exists in central locus of the associated Higgs-Action eigenstate at an equal theta and phi, at the same initial rho as the length of the associated Higgs-Action eigenstate, while the parabollic shape given smoothly curves in all 32 first derivatives to a shaft on either end of the associated parabollic structure to the given thickness. (3*10^(-78) meters thick in the globally distinguishable and 10^(-86) meters thick in the substringular.) The mini-string or field that comprises the construction of the Fischler-Suskind-Mechanism is 10^(-129) meters thick in the substringular and 3*10^(-121) meters thick in the globally distinguishable. The Shotcky construction of the Klein bottle has outer Neumman boundaries that are 3*10(-35) meters thick in the globally distinguishable and 10^(-43) meters thick in the substringular. The norm conditions in the Klien bottle are interconnected by mini-string, or, in other words, by subsringular fields, in such a way that the Klein bottle bears a subtended Ricci Scalar metric-gauge that is equal to 6.25*10^(18) in both the globally distinguishable and in the substringular. The associated Higgs-Action eigenstate bears a Hodge-Index in terms of Poincaire interelation of the overall first-ordered-point-particles that could fit in the given Higgs-Action eigenvalue. The structure here allows for just the leverage needed for the lifting of the given Klein bottle. The "top", or norm to holomorphic end of a Higgs-Action eigenstate, bears a borne tangency with the "bottom", or norm to antiholomorphic end of the associated Klein bottle via a supplementally norm mesh of mini-string, or, in other words, substringular fields.

A Fujikawa Coupling

A Fujikawa Coupling is an example of a Yakawa Coupling. The Fukikawa Coupling is when a one-dimensional superstring bends hermitianly to form a two-dimensional superstring via the Green function. A hermitian gauge-metric is a substringular action that is smooth in topological redistribution in all of the derivatives equal to the number of dimensions that it is differentiating in.

A Yakawa Coupling is a touch, rub, and/or curl of one substringular phenomenon upon another.
A Gliossi norm gauge-metric is a borne tangency of one substringular phenomenon upon another.

A borne tangency is a direct touch. Ward conditions are the multi-dimensional Caucy-like conditions that define the physical boundaries that bear upon the multi-dimensional setting of a substringular phenomenon. Neumann conditions are the direct boundaries of a physical phenomenon. Derichlet conditions are the boundaries of the first derivative of a physical phenomena. When considering the boundaries denoted by alterior derivatives of a physical phenomenon, you have Ward conditions. So, a Fujikawa Coupling is a Yakawa Coupling that produces a Gliossi condition between the two ends of a one-dimensional superstring, allowing for a bend in the associated one-dimensional superstring that is hermitian throughout the given Ward Conditions.