Ghosts Of Orbifold-Based Phenomena

When  physical spaces -- in the form of  orbifolds and/or orbifold eigensets -- are pulled through dual discrete Lagrangians, whether or not the just mentioned general format of the respective singular Lagrangians are unitary, binary, or overtly multiplicit in directoral-based permittivity, the so-stated orbifolds and/or orbifold eigensets will form ghost anomalies as these move through the corresponding Hamiltonian-based operands of physical space in which the said orbifolds and/or orbifold eigensets move through here.  Such individual respective Hamiltonian-based operations will here involve the multiplicit formation of potentially many ghost anomalies that come together in a group-based cohomology that will here form, in so as to map-out a tracing as to the relatively recent physically-extrapolatable memory of where, how, and when an orbifold and/or an orbifold eigenset had been kinematically displaced and delineated over a sequential series of group instantons -- the physical memory of an orbifold and/or an orbifold eigenset when relative to one or more other orbifolds and/or orbifold eigensets.  Given the substringular environment that exists after an arbitrary discrete physical space has moved in so as to form a trajectory of its kinematic projection over time, the ghost anomalies that are thus formed may be anharmonically scattered at any time, once the corresponding mapping of the correlative group-based world-sheets have been traced-out by the harmonic scattering of the here given arbitrary relatively forward-holomorphic moving norm-states that get in the path of the motion of the corresponding superstrings that work to comprise the eluded to orbifolds and/or orbifold eigensets.  If such ghost anomalies are formed between two or more orbifolds and/or two or more orbifold eigensets that are Njenhuis in terms of their kinematic-based covariance towards each other over the same group metric, then, the ghosts that these form will tend to be Njenhuis relative to one another. Yet, if such ghost anomalies are formed between two or more orbifolds and/or two or more orbifold eigensets that are Real Reimmanian in terms of their kinematic-based covariance towards each other over the same group metric, then, the ghosts that these form will tend to be Real Reimmanian relative to one another.  Often, though, the residue that is formed by the anharmonic scattering of different sets of ghost anomalies that are initially of different universes may be brought into a closer Reimmanian inter-relationship towards each other after the corresponding recycling of their respective mini-string segmental partials have been recycled through enough times.  I will continue with the suspense later!  Sincerely, Sam Roach.

Vibrations that inter-relate formats of E.M.

Although a photon is comprised of a bosonic superstring of discrete energy permittivity that quantizes into beams of electromagnetic energy that move at the speed of light in a vacuum (unless it is Kirchoff radiation), the manner of the vibration of a photon works to determine the type of wave that certain quantized photons bear, the amount of energy that the photons of such a given arbitrary beam have, their J,S, and L, etc. ...


The reason as to why and how the type of vibration of a given arbitrary photon has impacts the type and amount of energy that the said photon has is based on a simple premiss: The manner in which something vibrates, radiates, and propagates effects its direct and indirect environment in a particlular way -- given the covariant codifferentiation of the surroundings of the given arbitrary photon. Such an effect is physically displayed by the electromotive interaction of the surrounding open superstrings that are at least adjacent to the tree-amplitude-based projection and propagation of a given beam of E.M.. This has a basis in Lagrangians that are either unitary, binary, and/or Lagrangians that bear Njenhuis path-based tensors.R

Part One Of The Tenth Session Of Course Ten

Let's say that there were, in the following case scenario, three covariant substringular groups that are here going through a Fourier Transformation that is here perturbated in a Njenhuis manner in such a way to where the three said groups which here represent three orbifolds work to produce a alterior perturbation in the corresponding covariant differentiation that will potentially alter any potential Kaluza-Klein light-cone-gauge topology in the said three orbifolds to be brought into having a Yang-Mills light-cone-gauge topology.  Yet here, the homotopic residue of each mentioned substringular group will maintain its  Fourier-based generation of substringular field during the duration in which the said three mentioned groups propagate along the Ultimon Flow -- when one considers the integration of both the Real Reimmanian-based time that involves the reiterating of instantons along with the Imaginary-based time that exists in-between the durations of the said individual instantons over the course of the iteration and the reiteration of the integrated sequential series of instantons that form the time that involves the mentioned Fourier Transformaion illuded to here.  Homotopic residue is the mini-string segments that begin to break off while yet reconnect to other topology during what I term of as the space-hole.  The space-hole is the duration that happens right before the instanton-quaternionic-field-impulse-mode in which topology virtually disconnects in just of a manner in so that homotoy may be altered in just enough of a degree in order that norm-conditions may be able to change in the manner that these need to change so that the proper Gaussian Transformations may happen so that the substringular may be spontaneously and perpetually kinematic so that energy may be able to persist.  The prior activity that I was describing before I mentioned what homotopic residue is happens so thawt the previously mentioned homogeneous wave permittivity will allow for the commutation of spin symmetry via the indices that are relatively local to all three of the described substringular groups at one general group metric or another on their way through the Lagrangian-based operand that each group is kinematically pulled into through their motion along the Continuum.  Such an activity allows for the said three substringular groups to here differentiate in a timewise manner with what is in this case an even chirality that exists in an isometric fashion among the vibratory operation of the homotopic residue that respectively exists in correspondence with the three said substringular groups when in covariant relation with each other.  This prior activity is happening in holonomic proportion, in terms of their corresponding Hodge-Indices and the parity of their respective fractal of angular momentum, in such a manner so that their related norm-conditions that are in transition are here to be in covariance with the fractal of angular momentum of each sector of the described homotopic residue.  In the meanwhile, the tri-local substringular encodements that help to determine the positioning of the corresponding superstrings along with helping to determine the positioning of said superstrings homotopic residue, here works to converge the coniaxial that is related to the conipoint that helps to define the relativistic center of the general activity that I am describing here so that the locus of the related orbifolds that represent the three substringular groups may be in isometric and Hodge proportion to the euclidean-based even distribution of their wave propagation and their respective residue over what may be described here as an inverse of a Clifford Expansion that brings the three orbifolds into an interactive-based region.  Those semi-groups that here arbitrarily commute a kinematic discharge of phenomena that is related to the superstrings that comprise the said orbifolds as the said orbifolds exist in relation to one another will here form spin-symmetries that become covaliant via wave coaxials that kinematically differentiate thru Lagrangians that occur over an arbitrary Fourier Transform.  I will continue with the suspence later!  Part Two Soon!  Sincerely, Sam.           

Addendum 1 to GUFT

The Klein Bottle has an exterior surface area of 768 Planck lengths by 384 Planck lengths. The Klein bottle allows for a group metric of 191 iterations that produce 191 mini-loops to be acquired by each superstring that undergoes the Fourier translation of the set of Kaeler metrics that allows superstrings to attain the permittivity that thee need and to allow their respective Fadeev-Popov-Traces, or, in other words, their Planck phenomenon related phenomena, to attain the impedance that these need to be the discrete units of energy that these are. 768*38*191 = 56,328,192. So, in general, each time that a superstring undergoes 56,328,192 iterations along the ultion whether tachyonic or not since either way these go thru the ultimon or go around the Overall Physical Portion of the space-time-continuum per iteration, the associated discrete units of energy, 56,328,192 iterations after their respective Kaeler metrics, go thru the Klein metric again. The kinematic redifferentiation of superstrings via their Lagrangians through their respective Fourier Transformations allow for redistribution of correlative superstrings and their respective Fadeev-Popov-Traces to allow Minkowski-Wise indistinguishablly different stringular groups that are Hilbert-Wise and Njenhuis-Wise indistinguishablly different stringular groups, seeing that group Ward substringular groups alter in group angle codifferentiation during each successie set of superconformal transposition. When Minkowski-Wise kinematism becomes multiplicit, then the stringular groups associated with the altering Kaeler metrics then become distinguishablly different. This happens when Clifford differentiation becomes Real Reimmanian relative to the associated substrigular fields.