Part Two of the Sixth Session of Course 18

Both orbifolds and orbifold eigensets may exist as either a bosonic-based configuration or as a fermionic-based configuration.   Cohomologies may exist in terms of world-sheets that work to inter-bind other substringular phenomena, as well, as a fractal of magnetic topological-based settings that work to correspond to those multiplicit respective orbifolds -- that operate in so as to form a mappable tracing that forms the so-stated given arbitrary cohomologies.  Unique relatively codifferentiable, codeterminable, and covariant cohomological-based physical patterns may be symmetrically orientable in either a relatively chiral isometric geometrical-based manner, or, other unique relatively codifferentiable, code terminable, and covariant cohomological-based physical patterns may be symmetrically orientable in a relatively antichiral isometric geometrical-based manner, over time -- as the physical memory as to the where, how, and when the directly corresponding orbifolds -- that had worked to form the so-eluded-to cohomoogical-based patterns that I had inferred -- have been mappably traced.  A chiral-based symmetry may be either trivially isometric, or, such a general genus of a chiral-based symmetry may be non-trivially isometric.  An antichiral symmetry bears a reversal in the handed-based nature of a general isomorphism, that may be reverse-symmetric in either a trivially isomorphic manner or in a non--trivially isomorphic manner.

Some Additional Help

When one given arbitrary relatively more variant-based substringular motion of superstrings strikes a riven arbitrary relatively more conformally invariant-based substringular motion of superstrings -- over a given arbitrary set sequential series of group instantons -- the so-stated more conformally invariant set of substringular phenomenology will tend to bear more of a potential to be displaced, than the so-stated more variant set of substringular phenomenology.  As this so-eluded-to set of conditions happens over time, the relatively more conformally invariant set of substringular phenomenology that I have just eluded to will tend to bear less of an overall overt basis of Lorentz-Four-Contraction, while, the relatively less conformally invariant set of substringular phenomenology that I have just eluded to will tend to bear more of an overall overt basis of Lorentz-Four-Contraction.

The Second Part of the Fifth Session of Course 16

As the transformed directly corresponding homotopic substrate that was acted upon in the eluded to perturbative manner is altered from a Rham-based cohomology into a Doubolt-based cohomology, the eluded to holonomic entity may, on occasion, twist coniaxially -- in terms of its Ward-Caucy-based field at the Poincaire level, to where the said homotopic substrate may conform to the Gaussian condition of the directly external kinematic differentiation.  This happens in enough of a scalar topological-based "quantum" of Hodge-based homotopic recycling of norm-based states, to where the eluded to internal changes in norm-coniditions may move both in the direction of being in a relaxed state, as well as acting in accordance to a fractal of the right-hand-rule in a Chan-Patton manner.  So, whatever the Ward-Derichlet condition of the regions that directly surround the intially stated locus of Gaussian Transformation eigenstate are, this will then work in a simultaneous manner through a central conipoint, in so as to cause the directly related Chan-Patton conditions.  If there are here no Chern-Simmons spikes in both the Lagrangian-based differentiation and the metrical-based differentiation of the activity of any said internal superstrings (that would here be of a Rham-based cohomology) during any given arbitrary group metric, then, these internal superstrings are said to be Yau-Exact.

A Little Bit Of A New Addition

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.