A Little Bit About Spurious Eigenbases

What type of a perturbation series would propagate if certain superstrings of covariant traits were to aquire topological sways, and how would this alter the angular momentum of the thus related homotopy -- whose phenomenology is defined by the interaction of those covariant traits which act eigen to the pertainent differentiable semi-groups (The semi-groups here are norm-states that act as catylists to the formation of those superstrings which encode for the mentioned covariant traits)?  As an arbitrary example:  A superstring is reiterated within the same neighborhood.  Quadrillions of related superstrings do too.  A miniority of the two-dimensional strings here iterate and reiterate side to side on a slightly differentiable coaxial basis.  These superstrings maintain an even function of polar shift in order to not get "kicked-out" of their association with the other superstrings which help define the basis of their respective covariant traits.  The change in the holomorphic index, thus caused, commutes phase change in the nodation of anharmonic oscillation.  This kinematic activity causes a change in wave connection and wave-tug between the other corresponding superstrings and the initially stated ones that are associated with the mentioned norm-states . This phase alteration repositions the parallax of the related homotopic Fourier differentiation by setting up a buffer in the prior mentioned related semi-groups.  This activity localizes as a supplement in the Imaginary tense to the change of angular homotopy caused by the coaxial twists that the said superstrings are kinematically undergoing.  The buffer is produced by the harmonic sway of those wave connections which were relocalized by the propagation of axions.  Such axions, under the course of such an arbitrary scenario, were generated by the tensors that in this case caused a euclidean repositioning during each time that the related superstirngs were spontaneously torqued.  This angular momentum change would, by intereacting with the mentioned buffer, cause a divergence in the local invariance of the set interactive traits, yet, it would converge the kinematic differentiatiion of the given covariance that is happening when the said metrics that were just mentioned are undergoing the described Fourier Transformation.  This is since the co-differentiation with the "buffer" would act as a "check and balance" to the inertial Dirac of the given homotopic configuration that has been described here.  If, after a discrete series accumulation of differenial variance, and if the homotopy has undergone global kinematics in the process of such a related Fourier Transformation, then, the series here would converge upon a local basis of a fractal of static equilibrium that may be described as a tense of conformal invariance.  It is then that the given "buffer" is said to be a member of a potentially spurious eigenbasis that may be physically denoted by an orbifold that bears a relatively strong tendancy for Chern-Simmons Laplacian-based and Chern-Simmons Fourier-based singularities over a metric that would involve a relatively brief number of instantons per duration of cyclic permutation.  I will continue with the suspence later!  Sincerley, Samuel Roach.