Well hello again world, this Sam Roach here! I am about to summarize the second part of the first session of Course 6.
Superstrings and first-ordered point particles tend to have a "home" tori-sector-range. This means that the described first-ordered point particles and superstrings tend to exist during instanton within the same layer of reality. Yet, some first-ordered point particles and superstrings may sometimes exist in individual yet various layers of reality over a sequential set of Fourier Transformations over a set period of time. Some superstrings and first-ordered point paricles are perturbated to the extent that these said phenomena never settle within a set layer of reality.
Each layer of reality is correlative to a Basis of Light. Each Basis of Light is related to one tori-sector-range. The substringular phenomena that belong pajoritatively to one layer of reality tend to remain in one tori-sector-range and thus these phenomena exist paroritatively within the neighbood of one particular indistinguishably differently localized Basis of Light. The substringular phenomena that do not have a stable "home" tori-sector-range tend to flow through the orbifold eigenset related "kernels" or the gaps in-between orbifold eigensets so as to form many differently localized bonds with different orbifold eigensets that belong to various layers of reality. This is what I mean by that some substringular phenomena tend to not have a "home" tori-sector-range in over any spontaneous Fourier Translation of Lagrangian-based kiinematic Hamiltonian eigenmetric.
Yet, in either case, whether certain substringular phenomena are to tend to have a "home" tori-sector-range while other certain substringular phenomena tend to alter the basis of what tori-sector-range that these later said phenomena are to most directly be kinematically interactive in, the Fourier Translations of superstrings and first-ordered point particles differentiate via their kinematic Hamiltonian operations in such a Gaussian based symmetry that is non-trivially isomorphic in terms of harmonically based orbifolds and orbifold eigenstates, while differentiating via their kinematic Hamiltonian operations in such a Gaussian based symmetry that is trivially isomoriphic in terms of anharmonically based orbifolds and orbifold eigenstates, in such a manner so that the operand of the interaction of the associated space-time-fabric is made to bear a hermitian interation that produces the condition of the recycling of norm to ground and ground to norm states -- as well as recycling the indistinguishable indices that define the bases of the eigenstates that are multiplicitly directoralized under the condition of altering holomorphicity (left moving versus right moving (relative)). This is because the Gaussian conditions described produce the norm conditions that are necessary for organized and thus Real Reimmanian space-time iterations in so that the conditions of smooth-curvature based norm-conditions and jointal based norm-conditions may indistinguishably intechange so as to allow for the continued existence of the interaction of substringular field networking that is necessary for continued existence. Sincerely, Sam.
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