Some Knowledge About The Bette Action

During the duration in which the Imaginary Exchange of Real Residue happens, both the Polyakov Action and the Bette Action happen.  The Polyakov Action is the reverse contraction of a given superstring that matches the degree in which the here given superstring is kept from full Lorentz-Four-Contraction.  The Bette Action is the Laplacian geometric condition in which the individual substringular fields, in the form of mini-string segments, that exist in-between a given arbitrary superstring of discrete energy permittivity and its correspondint counterpart, are attempted to bear both a homeomorphic wave pattern in-between the two just mentioned topological stringular phenomena all along the Laplacian mapped contour around (for 2-d strings) or all across the Laplacian mapped contour across (for 1-d strings) the contour that binds a superstring and its counterpart. This is as well as the condition of the superstrings in relation to their counterparts bearing an equal topological length along the Laplacian mapping of the mini-string segments that are here to interconnect the said superstring and its corresponding substringular counterpart.  The conditon of a superstring and its Laplacian-Based forward holomorphically placed counterpart bearing mini-string that interconnects these that are equal in the scalar that is relating to the topologically mapped distance that the said mini-string segments have in-between their corresponding superstrings and their counterparts is called an eigenconditon of the Grassman Constant.  If either the topological Laplacian mapping of the said segments that are here used to interconnect the said superstrings and their counterparts, as considered over each potential stretch eigenconditon of an arbitrary given superstring and its counterpart, is homeomorphic over the course of the Polyakov Action (which is during the Bette Action), and/or, if -- during the individual segments of the said potential stretching of any particular superstring, when taken as covariantly discrete integrands of correspondence with the related Lorentz-Four-Contractions that are arbitrarily related here in a specifically given scenario, bear an equally mapped scalar in terms of the length of the said contour -- (The Grassman Constant applies to the consistency of having the same topologically mapped distance between a said superstring and its corresponding counterstring over the duration and activity of the Polyakov Action) -- , then, the related superstring(s) are said to be orientable over the course of the described Bette Action.  I will elaborate later.  Got to run!  Sam.