A Little Bit of Preparation

I have recently discussed gluons and ghost anomalies.  My next six posts involve the four parts to session 13 of Course 14 about Group Action.  In the posts that appertain to the four parts of session 13 about Group Action, I thoroughly discuss the activity of ghosts -- as various formats of delineated displacements of the physical memories of world sheets.  World-Sheets are the physical trajectories of superstrings.  Such physical memories are mappable traces that are comprised of mildly bumped into forward-holomorphic norm-states, whose delineations work to show the directly prior motion as to what, how, and where various superstringular phenomena had been kinematically placed over a sequential series of iterations of group instanton.  The reverse-holomorphic norm-states that act as counterparts to the forward-holomorphic norm-states work to scatter ghost anomalies, so that the residual indices of the eluded to physical memories of superstrings may be extrapolated into fractals of Hamiltonian operators that subsequently work to form those gravitational particles that act in so as to interact along the Rarita Structure in order to operate the function of gravity -- when in conjunction with superstrings that act as discrete units of energy permittivity.  In later sessions, I will explain as to how the ghost anomalies of gravitational-based particles, which are known of as Neilson-Kollosh ghosts -- work to exchange indices with the ghosts of discrete units of energy permittivity, which are known of as Gliossi-Sherk-Olive ghosts -- in so as to balance the various loci as to where there needs to be room for both gravitational particles and the eluded to Gliossi-Sherk-Olive ghosts, so that there may be adequate space for energy to move kinematically over time in so as to remain as energy.  You will then soon learn about both the hermitian-based ghost anomalic formats, as well as the Chern-Simmons-based ghost anomalic formats, so that there may be a viable dialogue as to the harmonic nature of both the permittivity, impedance, and the mappable tracing of the integrable delineations of such ghosts in both a time-wise and in a time-less extrapolatory genus of parity.  Knowing how to trace and determine any given arbitrary past motions of superstirngs works to help one to understand the activity of the substringular. By the way, forward-moving time associated ghost anomalies are formed by positive-norm-states and scattered by negative-norm-states, yet, with backward-moving time associated ghost anomalies, ghosts are formed by negative-norm-states and are scattered by positive-norm-states.  This is because the holomorphic direction of reverse-time-based substringular action is in the reverse genus of general parity of the holomorphic direction of forward-time-based substringular action.  I will continue with the suspense later!  Sincerely, Sam Roach.