Tenses Of Relative Stability

Let us first consider an initially relatively stable atom, that is functioning as a metrical-gauge-based Hamiltonian operator -- at one set locus, in which such a respective stable atom is in a tense of conformal invariance, from within its general Ward-Caucy-based physical framework -- in which the said atom is to be operating at -- over a relatively transient duration of an initial set metric.  Let us next consider that this said atom had just previously been slowed into the earlier mentioned tense of conformal invariance -- to where the so-stated atom was kinematically converging into that so-eluded-to tense of Majorana-Weyl-Invariance, that was eluded to at the beginning of this post.  In the process of the so-mentioned atom being brought here into the said condition of conformal invariance -- the here so-eluded-to harmonic-based perturbation, that had then worked to cause the said atom to go into a state of relative Majorana-Weyl-Invariance, happens in such a manner to where the so-stated atom was then brought into a relatively stable kinematic condition of being at a steady-state, that is to here exist from within the general proximal localized region of its Poincare-based framework, to where such an atom may be said to have undergone a tense of a Wess-Zumino genus of an interaction -- over the directly corresponding sequential series of instantons, by which such a convergence that leads into a tense of conformal invariance had to have then happened, directly prior to the conditions that I had stated at the beginning of this given arbitrary respective post.  Let us then say that there is an interaction of that form of electromagnetic energy, that is of the genus of an infrared or heat-based energy -- that is to then be applied to the topological surface of the holonomic substrate of the atom that I have been discussing here in this given arbitrary post.  Let us then say that the interaction of heat energy with the said atom, will then tend to work to cause one or more electrons -- that are from within the Ward-Neumman bounds of the said atom, to be excited -- to where the so-stated one or more electrons that have then become excited, will then drop an energy level, while then "leaping" back to its initial energy level that I have here so-implied.  This will then tend to work to cause the emission of one photon per electron that had dropped an energy level.   The so-eluded-to electrons, that had just been excited by the Gliosis-based interaction of heat with the topology of their holonomic substrate -- happens, to where this said heat will have had been applied to the Ward-Neumman bounds of the so-stated atom that I have been writing about, in this respective given case scenario.  This so-eluded-to enharmonic tense of a perturbation, may be viewed of as an example of a Cevita interaction.  Thurthermore, whenever electromagnetic energy is scattered upon any general genus of phenomenology -- this general genus of a Fourier-based activity will tend to form a gauge-transformation, during which there is then what may be termed of as a Calabi-based interaction.  Calabi-interactions always tend to work to form a certain scalar magnitude of entropy, which is needed in order for the changes of physical states to happen. (For instance, such entropy is needed in order for ice to melt into plane water.)  Whenever any electromagnetic energy is scattered upon any orbifold eigenset of mass-bearing superstrings, that are of discrete energy permittivity -- this general genus of interaction is known of as a Calabi-Yau interaction.  This is why the orbifold eigensets, that are directly associated with mass-bearing superstrings -- are known of as Calabi-Yau manifolds.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.