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).                      

Part Three of the Eighth Session of Course Nine

What I mean by relatively time-oriented and relatively timeless light-cone-gauge eigenstates is that only bosonic or closed superstrings may directly associate with a specific linearly directed time-frame.  Fermionic or open superstrings happen in time, yet, these do not have the capability to directly associate with a specific linearly directed time-frame.  This considers the condition that time moves forward and backward at the same time.  What I mean by a specific linearly directed time-frame takes into consideration that occasionally one-ten-thousandth of history changes.  What is cognitively imbued in the collective consciousness may not be changed in terms of history, yet, what is not cognitively imbued in the collective consciousness has more of a capability of changing in terms of history.
                       
There are five second-ordered light-cone-gauge eigenstates that directly associate with one-dimensional superstrings taken individually.  The second-ordered light-cone-gauge eigenstates comprise a first-ordered light-cone-gauge eigenstate.  There are ten second-ordered light-cone-gauge eigenstates that directly associate with two-dimensional superstrings taken individually.  Again, the second-ordered light-cone-gauge eigenstates comprise a first-ordered light-cone-gauge eigenstate.  The second-ordered light-cone-gauge eigenstates directly associated with one-dimensional superstrings, taken individually, are comprised of two coiled chords -- either sinusoidal-based or flushly-directed-based -- of mini-strings that tie in-between a superstring and the Fadeev-Popov-Trace that is positioned directly in the reverse-holomorphic direction of the mentioned one-dimensional superstring.  The second-ordered light-cone-gauge eigenstates directly associated with two-dimensional superstrings, taken individually, are comprised of a chord of mini-string -- either sinusoidal-based or flushly-directed-based -- that tie in-between a superstring and the Fadeev-Popov-Trace that is positioned directly in the reverse-holomorphic direction of the mentioned two-dimensional superstring.  Two-dimensional superstrings that are discrete units of energy permittivity bear two discrepencies in terms of the topologically pure hermicity that these would otherwise have -- yet, this condition is minor enough to allow for a two-dimenisional superstring to still have a conformal dimension of two.  This is because the discrepencies fit as locally hermitian cusps that help to allow for the field of an individual two-dimensional superstring to have a directly associated three-dimensional field.  These discrepencies exist to the holomorphic side and to the norm-to-holomorphic positioning at the  relative ninety-degree locus of a given two-dimensional superstring and to the reverse-holomorphic side and to the norm-to-reverse-holomorphic positioning at the relative 270 degree locus of the same given two-dimensional superstring.  Such two and three-dimensional discrepencies help to cause the potential instabillity, and thus, the potential entropy that is more associated with the kinematic translation of two-dimensional superstrings than with the kinematic translation of one-dimensional superstrings -- even though the end result of entropy itself is comrised of spurious plain kinetic energy, and, plain kinetic energy bears energy permittivity that is comprised of one-dimensional superstrings.  One-dimensional superstrings that are discrete units of energy permittivity bear one two-dimensional discepency at its relative center.  Such a discrepency deviates from th pure hermicity that these would otherwise have -- yet, this condition is minor enough to allow for a one-dimensional superstring to still have a conformal dimension of one.  This is because the discrepency mentioned fits as a locally hermitian cusp that helps to allow for the field of an individual one-dimensional superstring to have a directly associated two-dimensional field.  Such a discrepency here exists in the norm-to-norm-to-reverse-holomorphic side of any given arbitrary one-dimensional superstring.  I actually have at least a couple more parts to this one session about Fock Space and the Light-Cone-Gauge, and I do not want to bore my reader's with too much information at once.  So, I will continue to ellaborate furter as to the conditions that work to allow for relatively timeless and relatively time-oriented light-cone-gauge eigenstates later.  Until then, I will continue with the suspense later!  God Bless You!
Sincerely, Sam Roach.