1) Ideal one-dimensional superstrings have an orientable Grassman Constant that exists as a homeomorphic vibrating one-dimensional partial field that topologically sways in a second spatial dimension in the process of the inter-relation of the said one-dimensional string with its counterstring over the course of the corresponding duration of a given arbitrary iteration of BRST.
2) Ideal two-dimensional superstrings have an orientable Grassman Constant that exists as a homeomorphic vibrating two-dimensional partial field that topologically sways in a third spatial dimension in the process of the inter-relation of the said two-dimensional string with its counterstring over the course of the corrsponding duration of a given arbitrary iteration of BRST.
3) One-Dimensional superstringular encoders consist of a relative allignment of 10^43 substrings that are completely Njenhuis to our general detection, that work to orientate with a relative allignment of 10^43 counter-substrings. Unless there is major tachyonic propulsion that is directly envolved with a given arbitrary substringular encoder, the homeomorphic vibrating substrings -- as a whole -- that are of a given arbitrary one-dimensional substringlar encoder, exist as having a homeomorphic vibrating one-dimensional partial field that topologically sways in a second spatial dimension in the process of the inter-relation of the said one-dimensional stringlar encoder with its counterstring over the course of the given arbitrary duration of an iteration of BRST.
I will provide the next three test solutions later. To Be Continued! Sam Roach.
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