Part Five of the Third Session of Course 16

The ability of a specific region of a world-sheet that works to form ghost anomalies may be either propagated in the relatively forward-holomorphic directoral Hamiltonian path-integral, or, are propagated in the relatively reverse-holomorphic directoral Hamiltonian path integral, or, are propagated in a relatively antiholomorphic directoral Hamiltonian path integral -- given the tense of the directly associated kinematic-based flow of the accompanying Lagrangian that the said world-sheet is being propagated through over time -- in relation to the general directoral-based-flow of the eluded to Hamiltonian holomorphicity.  This is when in terms of the genus of the said condition, that could thence be called a Kaeler condition.  So, if a world-sheet of a given arbitrary scenario is moving in either a reverse-holomorphic directoral Hamiltonian-based path flow, or, in an antiholomorphic directoral Hamiltonian-based path flow -- in terms of the given arbitrary  Sterling approximation of the kinematic mappable tracing of the respective local divergence-based covariance or local scattering-based covariance.  Such formats of covariant-based modes are often Yakawa to the eluded to perturbation of one given arbitrary world-sheet relative to its immediately surrounding world-sheets, that are propagated in a metrical-based Dirac manner -- that is either euclidean-based in expansion mode or Clifford-based in expansion mode.  On account of what I just mentioned, this may be a Kaeler condition of an antiholomorphic divergence that may be extrapolated by the mapping of either a perturbative reverse-based covariance and/or a perturbative scattering-based covariance of the directly associated ghost anomalies -- that act here as physical memories of both the existence and the activity of the directly corresponding superstrings that behave in the format of the said manner.  If the given arbitrary world-sheets of a general locus are all kinematically covariant in terms of the genus of a convergent-based mode, then, the corresponding condition of holomorphicity may be considered as a holomorphic Kaeler condition. If a Kaeler condition is of a relatively antiholomorphic mode, and/or is of a relatively reverse-holomorphic mode, then, such a format of either a respective perturbative scattering-based condition or of a perturbative divergent-based condition is of a Kaeler condition that works upon the activity of a unique set of specific Njenhuis Rarita Structure indical projection eigenstates -- to form the metrical-gauge eigencondition of a Wick Action eigenstate.  The Wick Action is multiplicitly performed by a genus of a Hausendorf Projection that is applied through a mechanism of corroborative norm-state projections, that operates in such a manner in so as to activate the activity of Gaussian Transformations -- via the general basis of the operation of the Kaeler Metric.  The Kaeler Metric is applied by the interaction of a local Higgs Boson eigenstate with a local Klein Bottle eigenstate.  Please read my previous writings for some more detail about this.  I will continue with the suspense later!  Sincerely, Samuel David Roach.