In Relation to Stokes Theorem

Here is a general concept of string theory that is in relation to Stokes Theorem.  Let us say that one were to here be innately dealing with the homotopic existence of a world-sheet that is delineated at a given arbitrary general locus.  Let us then say that there is a line integral that one may consider here to be placed in a flush manner across the topological surface -- of what may here be considered to be the center of the holonomic substrate, that works to comprise the here said cohomological-based world-sheet.  Furthermore, let us now say that some given arbitrary Hamiltonian-based force is applied to the said world-sheet -- as an abelian norm-state projection, that acts upon the so-stated world-sheet in a manner, in so that the direct application of the so-stated norm-state projection upon the said world-sheet acts through its respective Hamiltonian operand via a unitary Lagrangian.  Depending upon the directoral-based orientation of the overall coniaxial that is then here directly associated with the delineation of the earlier so-stated line integral that one may here then consider as going through the topological surface of the Minkowski-based holonomic surface, of the so-stated cohomological-based world-sheet, this condition of Ward-Caucy-based parameter will then work to determine the manner in which such a Yakawa-based interaction of the so-stated norm-state projection will kinematically move the said world-sheet, upon the immediately following instantons after the here implied Gliossi-based collision happens, of this here respective given arbitrary case.  So, depending upon whatever the alteration or perturbation of the here so-eluded-to coniaxials -- that one may deem as existent in so as to work to form the existence of the line integral that would then here exist along the said Minkowski topological surface of the said cohomological-based entity of world-sheet that I have mentioned here, this general genus of perturbation will then, likewise, work to alter the manner of the ensuing kinematic distributions and redistributions of the Ward-Neumman bounds of the holonomic substrate of the earlier so-stated world-sheet, in so as to work to determine the unique and specific changes in the manner that the said cohomological surface will alter in its covariant-based mode to the here Gliossi-based interaction -- that it is here involved with with the said norm-state projection that is applied to it through the here proscribed unitary Lagrangian.  I will continue with the suspense later!  Sam.