The Third Session Of Course Ten

Stringular fields of one-dimensional superstrings are disc-like, and stringular fields of two-dimensional fields are spherical-like.  The light-cone-gauge eigenstates intaeract with substringular fields -- and are joined together with these.  Superstrings tend to be centered in their substringular fields.  World-Sheets are enacted upon by these fields by acting conformally invariant with the Ward-Caucy boundaries and the other related Ward conditions of the radial and transversal differentiation of the fileds of one and two-dimensional substringular fields.  The corresponding ghost anomalies that form during the Fourier-metric differentiation of the said substringular fields form as core stringular ghost fields that are surrounded by core stringular ghost anomailies.  The ghost anhilators that form disperse the ghost anomalies by normalizing the point commutator fields that are distributed by the related ghost anomalies.  The said ghost anomalies that are thus formed are due to the differentiation of the said corresponding world-sheets upon the positive-norm-states that surround the related superstrings, as well as the related stringular fields.  The ghost annhilators are the negative-norm-states that happen to move in the reverse-holomorphic directoralization of the respective positive-norm-states.  Positivt-Norm-States are comprised of the point commutator orientation that I have discussed before, and, these here are near the respective superstrings and their respective substringular fileds that are in the general direction -- as may be derived based on the norm-conditions that correspond between these both during the same general metric.  The negative-norm-states are comprised of the same general type of phenomenology as positive-norm-states, except, these move in the reverse holomorphicity (reminder).  The zero-norm-states are the loose point commutators that work to open two-dimensional superstrings at certain times, while these at other times work to close one-dimensional superstrings.  Every point commutator is a first-ordered-point-particle that is not in either a superstring, a counterstring, or a Fadeev-Popov-Related-Type-Ghost when considered during BRST in their respective world-tubes.