A second-ordered light-cone-gauge eigenstate of a two-dimensional superstring consists of 120 fully contracted mini-string segments that are twined homeomorphically in a Laplacian-based mapping in so that the peak diameter of the cross-section of such a strand-like segmental link is 25*10^5 times as thin in scalar amplitude as a general Laplacian-based projection. This makes such a strand-like link to have a tension per abelian-based Gliossi touch at the directly associated Poincaire locus of any substrate that is Yakawa to the topological surface of such a said link -- that bears up to 120*3*10^8 times the fractal modulus of a plain fully uncontracted mini-string strand -- for second-ordered light-cone-gauge eigenstates that directly relate to a given arbitrary two-dimensional superstring. For one-dimensional superstrings the directly associated links are doubled-up in so that these bear up to 240*3*10^8 times the fracal modulus of a plain fully uncontracted mini-string strand. This is since the here said arbitrary strand-like segmental-based links that are here being considered are like the directly prior links EXCEPT these are doubled-up upon each other, in so that such segmental-like links have a tension per abelian-based Gliossi touch that is at the Poincaire locus of any substrate that is Yakawa to the directly associated topological surface of such a said link that would here bear up to the said 240*3*10^8 times the fractal modulus of a plain fully uncontracted mini-string strand. (Sorry for being redundant.) Depending on the fill of the said second-ordered point particles that is caused by the density of the directly corresponing third-ordered point particles that work to comprise the mentioned corresponding second-ordered point particles that link like "beads" to form the mentioned mini-string segments, its diameter may vary by a factor of 3*10^8.
P.S.: Point fill is a variable condition that depends upon the compactification of mini-string when in reference to first-ordered point particles, or, for second-ordered point particles, point fill depends upon the compactification, or density, of the third-ordered point particles that comprise the said second-ordered point particles -- or, the point-fill of third-ordered point particles depends upon the fill of sub-mini-string that works to comprise these. Discrete sub-mini-string is constant, yet, the scalar amplitude as to what is "phenotypically" demonstrative as sub-mini-string may vary -- depending on whether such a discrete quantum of sub-mini-string is relatively decompacified or not
I will continue with the rest of the test solutions later! Sincerely, Sam Roach.
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