As To A Certain genus of Lagrangian Perturbation

Let us here take into consideration an orbifold eigenset that has its Fourier-based bearings, moving in what would here amount to the relative antiholomorphic direction -- when this is taken into comparison with an orbifold eigenset that is positioned just to the norm-to-forward-holomorphic side of the initially said orbifold eigenset, this latter mentioned orbifold eigenset of which is moving in the relative forward-holomorphic direction.  Let us next say that the initially stated orbifold eigenset is to start off with working to bear only euclidean-based hermitian singularities, at the Poincare level to the Gliosis-based topological stratum of the here so-stated initially mentioned orbifold eigenset.  Let us now say that there is a force of a given arbitrary substringular attractor, a group-attractor, that works to form a spontaneous pull upon the initially said orbifold eigenset.  The effect of the attraction of the said group-attractor upon the so-eluded-to orbifold eigenset that I have just mentioned, will then form a binary tense of Lagrangian-based Chern-Simons singularities upon the Yukawa-based field of the Hamiltonian operand -- of which the so-stated initially antiholomorphic moving orbifold eigenset had been moving through,  as a correlative Hamiltonian operator.  Let's say that the said binary tense of the so-stated Lagrangian-based Chern-Simons singularities, do what these will tend to do to the metrical operation of any respective given arbitrary orbifold eigenset that would do as I have just stated in such a situation -- this would then tend to work to form at least one viable set of metrical Chern-Simons singularities at the Poincare level that is of the parametric Hamiltonian field of the general locus of the directly corresponding Ward-Caucy boundary cite, that is of the the integration of those directly corresponding Laplacian-based mappable indices -- of which would then tend to form a sequential series of cohomological indices that would sway,  during the ensuing perturbative effects of its surroundings.  Let us say that the so-stated binary Chern-Simons singularities that are thence formed, act as a Laplacian-based metric-gauge operator, that is -- when one is looking in the cross-product-based direction of the motion of the said orbifold eigenset, to where one is looking at the orbifold eigenset as going directly forward in front of you, is as in a tense of being of a norm-to-holomorphic-to-norm-to-holomorphic tense of such a Laplacian-based metric-gauge operator.  Consider the right-hand-rule.  Let us say that the expansion of the Yukawa-based field -- that is formed by the initially antiholomorphic orbifold eigenset, is of a euclidean expansion at the Poincare level of the core-field density of the general cite of its motion.  This would then tend to cause such an orbifold eigenset to be pulled, almost imminently, into a Ward-supplemental perturbation of the holomorphic directoral-based flow of the said orbifold eigenset.  This will tend to cause an antiholomorphic Kahler condition -- of which will tend to cause the functional operation of a Kahler-Metric.  I will continue with the suspense later!  To Be Continued!  Sam Roach.