Friday, July 26, 2013

A Little Bit Of Some Stough About Lorentz-Four-Contractions

Mass, in and of itself, is comprised of two-dimensional superstrings.  Besides plain kinetic energy, most superstrings are bosonic, or closed in nature.  This means that most superstrings are two-dimensional in nature.  When a superstring is expanded to the inverse of its Lorentz-Four-Contraction over the initial portion of the duration of any given arbitrary iteration of BRST, it is expanded in proportion to how it was -- as a general shape -- before it was expanded to the inverse of its generally eluded to Lorentz-Four-Contraction.  Substringular phenomena that is related to a mass is basically in reference to the condition of the presence of two-dimensional superstrings, as eluded to earlier.  That is why, when a superstring is contracted, its length is contracted to the same scalar amplitude as the degree in which it is Lorentz-Four-Contracted.  Again, since the duration in which a superstring is expanded to the inverse of its contraction is so brief when relative to the overall duration of an iteration of BRST, from within an iteration of instanton, superstrings appear to have contracted when these are not fully expanded -- to any observer of whom may happen to be extrapolating the dimensionality, mass, and time that would here directly correspond to the conditions that may relate to any given arbitrary superstrings that may here be given consideration.  Bosonic superstrings have a length and a width.  A mass is comprised of many bosonic superstrings that come together as a whole in an orbifold eigenset.  So, as a mass is LFC to a certain given arbitrary degree, its length appears to have contracted to the scalar amplitude that corresponds to the degree in which such a condition may be extrapolated. 

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