Lorentz-Four-Contraction And Dimensinoality Of Legendre

The higher that the scalar magnitude is to be, as to the Lorentz-Four-Contraction that is here to be directly affiliated with the velocity of a mass (mass-bearing superstrings of discrete energy permittivity work to bear a symplectic homology) -- whose Lagrangian is to work to help here, at generating the delineation of a set of one or more superstrings of discrete energy permittivity that are here to work to bear a Legendre homology (superstrings of plain kinetic energy permittivity work to bear a Legendre homology over time) -- the more likely then, that the said given arbitrary set of superstrings of discrete energy permittivity -- that are here to work to bear a Legendre homology, will then tend to bear a higher dimensionality than such a Ward-Cauchy-based situation would otherwise entail.
 I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Test Solution 12 To The Last Test Of Course 19

12)  Let us consider an orbifold eigenset, that is to here be currently undergoing the process of the Kahler-Metric.   Let us say that the said respective given arbitrary orbifold eigenset, is to then be currently moving in a tachyonic manner.  Let us say that -- over the whole general course of such a respective group-based activity of the Kahler-Metric, that the said orbifold eigenset will be moving in the so-eluded-to manner, that is to then not be of the tendency of the motion of a Noether-based flow, over the directly correlative duration of time by which such a set of superstrings that operate in so as to perform one specific function, is to be going through such a so-eluded-to group-metric.  In so long as such an eigenset is to fully go through the said duration of the Kahler-Metric -- the directly corresponding orbifold will then be going through those 384 iterations of group-related instanton, that are to be related to a flow that is of the Kahler-Metric, although the so-stated orbifold eigenset will be directly associated with an indistinguishably different specific substringular neighborhood or substringular region -- over the course of each succeeding iteration of group-related instanton, in which the said orbifold eigenset is to be going through each successful ensuing step, that is here to be related to the successive series of the Kahler-Metric.
I will continue with the suspense later!   To Be Continued!  Sincerely, Samuel David Roach.

Internal Conformal Invariance

Let us initially consider an orbifold eigenset, that is moving at a constant rate in a constant direction in the substringular.  Let us consider that the said orbifold eigenset is comprised in part by internal orbifolds, that exist in a tense of conformal invariance from within the Ward-Caucy-based bounds of the so-stated orbifold eigenset.  On account of this, the internal conditions of the interior-mentioned orbifolds that are here to be undergoing the so-stated tense of conformal invariance, is of a state of proximal localized Majorana-Weyl-Invariance.  This means that the external state of the overall orbifold eigenset -- that is moving in a Fourier-based manner as a metrical-gauge-based Hamiltonian operator, has a significantly looser tense of Majorana-Weyl-Covariance than that tense of Majorana-Weyl-Covariance that is to, instead, be present in this case for the specific Ward-Caucy-based conditions -- that are of the internally stated set of orbifolds, that are in a Fourier-based state of conformal invariance.  This would then mean that the external reference frame of the said orbifold eigenset, that was initially mentioned, will tend to work to bear a relatively constant scalar amplitude of an effectual Noether Current, while the internal reference frame of the so-mentioned orbifolds that are to be to the interior of the Ward-Neumman bounds of the said overall orbifold eigenset, will work to bear a resultant tense of static equilibrium.  This state of static equilibrium will work to bear no net ulterior condition of an effectual Noether Current.  This would then mean that the overall orbifold eigenset that is here of a Calabi-Yau-related manifold, that works here to form a cohomology that acts as a GSO cohomological-based tracing -- will then tend to form a tendency, to where the resulting delineated ghost-based pattern will then tend to be of a hermitian Rham-based nature, that will then tend to propagate its directly affiliated mappable tracing as a metrical-gauge-based Hamiltonian pulsation, while the relatively internal reference frame that is of a relatively conformally invariant-based nature, will tend to have more of a tendency of working to form vibrational-based cohomological-based indices -- that will work here to bear either metrical and/or Lagrangian-based spurs.  The so-stated hermitian-based cohomology that is to here to be formed, is as to when this is taken in terms of the respective resultant hermitian singularities that are then to tend to be formed by the overall orbifold eigenset that I have mentioned, and the subsequently respective  resultant Chern-Simons singularities are then to tend to be formed by the internally so-stated orbifolds, that are to iterate as a reference frame that is to here be from within the interior of the Ward-Neumman bounds of the said overall orbifold eigenset.