Part Two of Session 8 of Course Nine

Each individual light-cone-gauge eigenstate has 44 angular momentum components, 84 orbital components, and 128 spin components.  This is due to the condition that, for relatively time-oriented supertrings, it is most basic for a light-cone-gauge eigenstate to rotate along its axial plane over the course of sequential instantons, while it is a little less basic for a light-cone-gauge eigenstate to rotate along a radial Lagrangian while yet maintaining a directly covariant association with a specific conipoint of the coniaxial that is related to an arbitrary superstring when it is undergoing a state of conformal invariance, while it is less basic, yet essential, for a superstring to undergo a perturbation in the locus of its coniaxial.  (Although Gaussian Transformation happen all of the time, because of intertia, it takes an outward force to transversally move a supersting out of conformal invariane in such a manner so as to allow for the continued flow of the countless Fourier Transformations that are associated with the kinematic interplay that allows space-time-fabric to spontaneously continue to exist.)  In one-dimensional strings, the 44 angular momentum components are excentuated beyond the other components, do to the condition that one-dimensional superstrings comprise the existence of plain kinetic energy.  In two-dimensional superstrings associated with the upper Royal Arc section, spin-related components are excentuated beyond the other components.  One-Dimensional superstrings have relatively timeless light-cone-gauge eigenstates -- partially on account of the condition that a one-dimensional superstring has a purely Minkowsk field that is directly associated with it.  (A one-dimensional superstring directly associates with a two-dimensional field.)  Two-Dimensional superstrings have relatively time-oriented light-cone-gauge eigenstates, partially on account that the three-dimensional fields that directly accomedate the respective two-dimensional superstrings, at least, bear some basis with a Hilbert-like field.  (Hilbert-based fields may have as little as three spatial dimensions associated with these.)  Yes, Minkowski space may have up to 26 spatial dimensions under the conditions of an arbitrary Laplacian setting, yet, the foundation of Minkowski space is two-dimensional space -- the basis of flat space is a planar two-diimensional field.  Hilbert space is volume-oriented space.  Hilbert space may be comprised of as little as three spatial dimensions under certain conditions.  Time-Oriented light-cone-gauge eigenstates, which, are of two-dimensional superstrings,  have ten second-ordered light-cone-gauge eigenstates that comprise the initially mentioned first-ordered light-cone-gauge eigenstates of the described two-dimensional superstrings.  Relatively timeless light-cone-gauge eigenstates exist in the field of one-Dimensional superstrings, these of which have five second-ordered light-cone-gauge eigenstates that comprise the initially mentioned first-ordered light cone-gauge eigenstates that are associated with the described one-dimensional superstrings.  Two-Dimensional superstrings are closed, while one-dimensional superstrings are open.  Most superstrings have bear light-cone-gauge eigenstates that are relatively time oriented, so, most superstrings are closed , or, in other words, most superstrings are bosonic.  Yet, fermionic or open superstrings must exist.  If open superstrings did not exist, a photon would implode as it was formed, yet, thank goodness for the fact that their is plain kinetic energy (it is a fact of reality), so as long as there is a Continuum, there will be a certain arbitrary amount of one-dimensional (fermionic) or open superstrings.  I will continue with the suspense later!    I have a couple more posts to do on this session to ellaborate further as to the meaning of what I have been describing here.Until then, move closer and closer to your goals, and you will move in the direction of which you think!  Sincerely, Sam Roach.