The operator that I mentioned near the end of the first part of session two is, in their respective cases, one of the following: a covariant organization of directly affiliated phenomena that are either zero-norm-states, Hausendorf-Projections, Campbell-Hausendorf-Projections, Campbell-Projections, in some cases, simply the mini-string that binds the relative "up" and the relative "down" of norm-states, or, in other cases, a combination of the just prior types of phenomena. Such respective types of operators work to pull the scattered norm-states in such a manner so that the ghost anomalies (in some cases) or the just annhilated ghost anomalies (in other cases) may manuver in an appropriate manner around the direct field density of either the two-d fields of one-d superstrings or the 3-d fields of 2-d superstrings. This helps to describe how -- to an extent -- norm-states work to form either ghost anomalies or to scatter these ghost anomalies so that gravitational particles may have a basis of formation. I will continue with the third part of this session later!
Hope in anticipation for the suspence! Sam Roach.
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