Friday, July 1, 2011

Session 10 of Course 9

Hello there world, this is Sam Roach here!  I hope that you enjoy the ensuing post!
Here's how the exchange between Real and Fock Spaces is Imaginary between Real and Fock superstrings:  As an example, the bottom of the bottom of point particles of Real-Based superstrings exchanges a little bit of mini-string to the top of the bottom point particles of a Fock strings point particles in a sinusoidal manner, lifting the Fock strings mentioned to a certain gauged distance.  This also goes for all of the first-ordered point particles that comprise Real and Fock-based superstrings. The superstrings then lower due to the added phenomena.  Once this is done, the botom of the bottom mentioned Fock string's point particles exchanges a little bit of mini-string to the top of the bottom point particles of Real strings in a sinusoidal manner, raising the Real strings to the same extent that the Fock strings were originally raised.  Agian, this also goes for all of the first-ordered point particles that comprise the arbitrarily mentioned superstirngs.  The strings then lower due to the added phenomena that I have been describing here.  This happens with superstrings during the course of what is known as BRST.  This helps settle the "dance" of the Planc phenomena that these strings are connected to by light-cone-gauge eigenstates via mini-string segments.  This exchange is Imaginary since the mini-string segments' ( exchange that happens between the point particles of the Real and Fock stringular counterparts) happens at the opposite ends of the point particles, causing the exchange to be off of the Real Reimmanian plane that is subtended between the point particles of the Real and Fock Strings.  Before the Imaginary Exchange, the Real Reimmanian-based superstrings' (as compared with their counterparts) point particles are just over half condensed oscillation, and the Fock strings' point particles are just under half full.  During the first Imaginary exchange under the condition of a superconformally invariant setting, both the Real and the Fock-related superstrings are half condensed oscillation.  After the Imaginary exchange of the given iteration (which is the duration during instanton),  the Real strings' point particles are just over half conesnsed oscillation, and, the Fock strings' point particles are just under half full.  So, even though a first-ordered point particle always has the same total locus of volume, the degree to which it is filled is defined by the density of the mini-string that comprises a said first-ordered point particle.  For instance, a just over half-filled point particle of the first order is just over 50 percent of the maximum density that second-ordered point particles -- in the context of mini-string -- can possibly fill the associated volume that a first-ordered point particle tends to have.  Yet, a just under half-filled point particles of the first order is just under 50 percent of the maximum density that second-ordered point particles -- in the context of mini-string -- can possibly fill the associated volume that a first-ordered point particle tends to have.  The relatively Laplacian-based degree of what I call point-fill here refers to a non-time oriented perspective as to the density of mini-string while it exists in the Neumman bounds of the locus where a first-ordered point particle is existing ( the density of such in one "snapshot" of duration).                      

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