Session Five Of Course Ten

The spherical shape of a two-dimensional superstring's field may be considered as many disc-like field partials.  These field partials interact with the field partials of light-cone-gauge eigenstates.  One of these disc-likle partials may be viewed of as either a washer or an annulus shpae.  Take the conter annulus of a three-dimensional stringular field that corresponds to a two-dimensional superstring.  We will here consider the annulus section of the said three-dimensional stringular field on account of the condition that this mentioned section is the substrate of the fractal of angular momentum of the field that I have been discussing.  The holonomic part of the annulus here bears the angular momentum indices of the three-dimensional substringular field during an iteration of instanton.  On the other hand, the interior of the said annulus bears the fractal of a magnetic field in this case, since, it is in this said section of the three-dimensional field that I have been discussing in which the radial momentum of the said field exists.  The interior of the said annulus also bears the spin-orbital momentum of the given three-dimensional field of the corresponding given two-dimensional superstring, since, the radial component of the field as well as the spin-orbital momentum component of the field both act as part of the vibratorial component of the said field.  The discs I mentioned of the substringular field here that I have described integrate in a Gliossi-Hodge manner to form the overall field of the given two-dimensional superstring.  The Laplacian integrand-based discs that contain the central annulus of the described field work to form the central- field-indices of the overall field of the said two-dimensional superstring.  The integration of the said disc-like phenomena that come together to help form the said three-dimensional substringular field of the said two-dimensional superstring works to form the integration of the cohesive partial fields of the described overall general field networking that exists in the substringular neighborhood that exists in the given general locus.  This general field is the set of mementum indices that interact with the field partials of the corresponding light-cone-gauge eigenstates in order to synchronize in kinematic codifferentiation in such a manner so as to help cause the operation of the said two-dimensional superstring that here, in this given arbitary case, acts as a propagatorial operator in space-time-fabric.  Such propagation is caused, in part, by the spring-like activity that is due to the operation of the local light-cone-gauge eigenstates.  I will continue with the suspence later!  God Bless You, and I will write some more soon!
Sincerely, Samuel David Roach.

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.