Monday, November 5, 2012

A Little As To World-Tubes

The following knowledge is on the nature of superstrings.:  One main world-tube is near another main world-tube.  Each of the prior mentioned world-tubes is conprised in part by one and two-dimensional superstrings.  Each one-dimensional superstring that I just mentioned bears a two-dimensional field.  Each two-dimensional superstring that I recently mentioned bears a three-dimensional field.  So, two-dimensional superstrings form world-sheets that bear a minimum of three spatial dimensions, while one-dimensional superstrings form world-sheets that bear a minimum of two spatial dimensions.  Both one and two-dimensional superstrings work to form world-sheets via the physical  mapping as to where these said strings were at -- in terms of what had happened in the substringular in the relatively transient past, relative to where the said superstrings are at in terms of their simultaneaous position aver a set conimetric.  The just mentioned world-sheets are differentially associated to each other as a function of their degree of covariant kinematic codifferentiation.  The positive-ground-states that here exist in the form of partitions are arranged at the center-state of the linkages that are binding, via the toroidal-like nature of the related world-sheets that are formed by the mapping of the trajectory of the said related superstrings over a sequential series of instantons.  The kinematic re-delineation of superstrings works to form the locus of their inter-relative covariant codifferentiation over time.  This post works to show -- to a mild extent -- the inter-relationship type of basis of every superstring, in some form or another, toward all of the other stings over time, and, time is the interaction of phenomena over a sequential series of instantons.

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