How Cohomology Works To Help Form Electromotive Attraction

Two different covariant cohomology-related phenomena, that are here to have the opposite spin, (opposite parity), will often tend to reverse-fractal, into two different covariant charge-related phenomena, that are here to have the opposite charge (opposite chirality). Initially, Again; Electromotive charge, tends to be formed, by a tense of a kinetically symmetrical braided cohomology-related covariant structure, that is here to work to bear a directly associated hermitian Lagrangian. Now; Picture the covariant topological manifold, of two different individually taken charge-based eigenstates, that may be taken down to a fractal level, in lieu of working to consider these, at the level of behaving as two different individually taken cohomology-related structures. Let us now imagine, that both of such cohomology-related structures, are here to work to exhibit the display, of giving off the opposite directional tense of "spin." Use the right hand rule, in so as to help you to imagine this better. This will consequently work to indicate, the covariant kinematic case, of two different unique and distinct "charged" eigenstates, that are here to tend to be tugged toward each other. As basically everyone knows, two different charges that attract each other, are to work to bear the opposite chirality. This may help you to better understand, as to why I have inferred/mentioned, that such symmetrically braided cohomology-related structures, that work to bear the opposite parity, will often tend to reverse-fractal, into charge-related structures, that work to bear the opposite chirality. I WILL CONTINUE WITH THE SUSPENSE LATER! TO BE CONTINUED! SAMUEL DAVID ROACH.

Chirality, Parity, And Sets Of Cohomological Eigenstates

The condition of two different covariant sets of cohomological eigenstates, as having the opposite chirality -- will tend to cause a degeneration of their cohomology -- which will consequently reverse-fractal into a tendency, in which there will then be two different charged stratum -- that are then to work to bear a degeneration of charge, the one toward the other.  Whereas;  The condition of two different covariant sets of cohomological eigenstates, as having the opposite parity -- will tend to cause an attraction of one of these two sets of cohomological eigenstates, towards the other, -- which will consequently reverse-fractal into a tendency, in which there will then be two different charges of the opposite chirality.  (A "positively" charged stratum and a "negatively" charged stratum.) 
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Cox Rings And Tense Of Parity

When a given arbitrary Cox Ring -- that is here of one respective ordered grouping of a set of cohomological eigenstates, is to undergo a Wess-Zumino interaction at the Poincare level, -- the said ordered grouping of such an inferred respective set of cohomological eigenstates, will tend to have a higher probability of maintaining its covariant tense of parity.  Consequently -- when a given arbitrary Cox Ring, -- that is here of one respective ordered grouping of a set of cohomological eigenstates, is to undergo a Cevita interaction at the Poincare level, -- the said ordered grouping of such an inferred respective set of cohomological eigenstates, will tend to have more of a probability of reversing its covariant tense of parity.  Sincerely, Samuel David Roach.

Some More Stuff As To The Noether Current

The Noether Current is formed, by the flow of the multiplicit tense of "pressurized vacuum" -- that  the multifarious sets of cohomological eigenstates, tend to bear towards one another.  Sets of cohomological eigenstates that are of the opposite parity, tend to bear an inverted tense of a "pressurized vacuum" towards one another -- that tends to form a "suctioning" effect at the substringular level, -- that will consequently tend to form a tense of an attraction, between such sets of cohomology-related eigenstates, that are here to work to bear the opposite parity.  Whereas -- sets of cohomology-related eigenstates that are of the same parity, tend to bear a non inverted tense of a "pressurized vacuum" towards one another -- that tends to form a "conformal repulsion" effect at the substringular level, -- that will consequently tend to form a tense of a repelling, between such sets of cohomology-related eigenstates, that are here to work to bear the same parity.  Sincerely, Sam Roach.

Cohomology-Related Eigenstates Of Opposite Parity

Two different sets of cohomology-related eigenstates are of opposite parity -- when one of these two mentioned sets of cohomological eigenstates is to bear an order of grouping, that is asymmetrically isometric to the order of grouping, -- that the other respective set of cohomological eigenstates is to bear.  I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Some Stuff As To The Beti Number And Orientable Supertrings

When the Beti number is even, during either BRST and/or during the directly ensuing Regge Action, for any one given superstring of discrete energy permittivity -- the said string is orientable, -- and thence, the so-stated superstring of discrete energy permittivity is then to ensue as being of a Noether-related flow.  The reason to this -- is that, when a superstring is to bear an even chirality-related parity, -- it is then to tend to bear a resulting Reimman-based scattering.  A Reimman-based scattering is of a harmonic delineation.  When the Beti number is of an even integer, -- the consequent partition-based discrepencies of the correlative superstring, is then to work to bear a harmonic flow of a distribution among the consequent partition-based discrepencies of the directly corresponding counter string of that self-same discrete quantum of energy permittivity.  Such a delineation of an even ordering, is here to work to form a homeomorphic field between the said superstring and its correlative counter string, during BRST.  Such an even ordering will then help at working to allow for the directly corresponding discrete energy to not be perturbated-out of Noether Flow.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Parity Between Adjacent Scattered Eigenindices

Let us initially consider a cohomological pattern, that had just formed at one given arbitrary locus.  Let us next consider this said cohomological pattern, as a "snapshot" in the substringular -- as being of a Laplacian-related Ward-Cauchy case scenario.  Let us now consider that the norm-state-projections that an orbifold eigenset had acted upon here -- in so as to work to form the said cohomology -- had formed what may be termed of as a Reimman scattering to a respective extent, in so as to form the so-eluded-to generation of cohomology eigenstates.  Now, let us consider two of the eigenindices that have here to have just been formed by the said cohomological generation -- in such a case in which these two respective given arbitrary eigenindices, which are out of the much larger overall Hodge-Index of the overall cohomological phenomenology of such a respective given case, are here to be adjacent to one another, at the proximal locus of the correlative Laplacian Transform.  These two adjacent scattered eigenindices, are of a Reimman scattering -- to where these are to bear an even parity.  This then works to elude to the Ward-based condition, that, if one were to theoretically fold together the two different individually taken eigenindices at their central coniaxion towards one another -- this would work to form a general genus of an isomorphic symmetry, at the point of duration of the correlative "snapshot" of time.  I will continue with the suspense later!  To Be Continued!
 Samuel David Roach.

Clarity As To Scatterings

When one is to have a Reimman scattering -- the adjacent scattered eigenindices are chiral, with an even chirality-based parity, -- whereas, when one is to have a Rayleigh scattering -- the adjacent scattered eigenindices are antichiral, with an odd chirality-based parity.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Reason For Transmission of Scattered Cohomologies

As I have said before, the residue of the multiplicit scattered GSO cohomologies has the tendency of being pulled off of the multiplicit relative Real Reimmanian Plane into the multiplicit relative Njenhuis Plane -- as the residue of the multiplicit scattered Neilson-Kollosh cohomologies have the tendency of being pulled off of the multiplicit relative Njenhuis Plane into the multiplicit relative Real Reimmanian Plane.  This tendency is on account of the following Laplacian-based set of  conditions:  The genus of the overall general norm-state-projections that are of the multiplicit relative Real Reimmanian Plane work to bear a harmonic even parity with the genus of the overall general norm-state-projections that are off of the multiplicit relative Njenhuis Plane -- in such a manner in so as to bear a multiplicit condition of their being a tendency of the Laplacian-based existence of a mean Lagrangian-based path that is of an even chirality, -- towards each enharmonically scattered GSO ghost that has been broken down by a Rayleigh scattering, and, there is a tendency of the Laplacian-based existence of a mean Lagrangian-based path that is of an even chirality, -- toward each enharmonically scattered Neilson-Kollosh ghost that has been broken down by a Rayleigh scattering. The condition, that, for every action -- there is an equal and opposite reaction -- happening in the opposite direction from the first said action, -- works to elude to the condition in which the antichiral parity of the adjacent eigenmembers of one set of cohomological indices that have just undergone a Rayleigh-based scattering of ghost anomalies, -- will work to cause the then existent condition of a proximal local chiral parity that bears a Hamiltonian operand that works to bear a clear path that is of a mean Lagrangian, to cause the pre-existent condition that the substringular tends to work in so to move in the direction of optimum rest, to cause a wave-tug/wave-pull of what may be thought of as the so-eluded-to just scattered ghost-based indices to recycle in the manner that I have just described of earlier in this post.
I will continue with the suspense later!  To Be Continued!  Sincerely, Samuel David Roach.

Some Stuff As To The Substringular Nature of Electrons In The Substringular

You may wonder about the vibrations of an electron from within the neighborhood as the said electron exists as a transposition of indical bases of which appertains to eigenstates of both mass and kinetic energy which quantify within the expected range of a double-majorized-plane-sector, which has a probablity that is minimized analogously to the elevation of tensorism as delineated by the covariance of the iteration and the reiteration of the superstrings and the quantific waves which work to form the eigenspace of the neighborhood of the said electron as it may be transiently measured within a range which is homogeneously proximal to its path operand.  Well, then, what is this vibration???  Such a vibration is the applied tensorism of the association of redistributed eigenstates of superstrings which swipe out a semigroup of heterogeneous potential morphology, whose field bears covariance with an inexact and nonlineaer differential association of reassorted factor groups -- which work to integrate the pulse of the said electron after each group convergent series of the directly corresponding magnetic dipole -- as the so-stated dipole delineates a morphological tense of permittivity -- which causes the constancy of the electrons tangency to abide by its directly associated orbital conditions.  So, what is a potential application to this eluded-to tensorism?  I will only give you a hint on my blog.  As the physical point particles (of the first-order) which work to comprise the relevant superstrings are minimized -- in terms of their repulsion factors -- the rate of the integrating factors, caused by the relative angular momentum of the orientation of that parity that is among the neighboring point commutators, increases -- in terms of the magnitude of reassortment transition.  This implied activity works to pull together first-ordered point particles to the given arbitrary regional distribution, which may be most "eigen" within the so-eluded-to tense of spontaneity.  If one were to be able to "pull" such a directoral topological sway -- on account of the added condition of all substringular wave that is unfrayed, being connected by the condition of Cassimer Invariance -- an equal and opposite "push" that would be inacted in the opposite general direction, will then be afforded by the directly corresponding activities that appertain to the presence of homotopy -- which would work to form a semi-permeable flow of wave-based delineation to be exacted, in terms of the wanted tenses of condensed wave oscillation, whose pushing-out of waves from the thence forming superstrings of discrete energy permttivity would work to help control the sub-atomic vibrations of the so-eluded-to given arbitrary electrons that appertain to such an activity.

Gell-Mann-Najshima-Relations

Those sets of boundary-based conditions of multiplicitly acting quarks -- when one discerns the covariance of their so-eluded-to parity-based interactions -- that work to establish the kinematic interplay of their Ward-Caucy-bounds, as taken over the multiplicit Sterlilng-based approximations of their sequential series of iterations of directly assoicated group instantons, that work to form that energy that such quarks function in, in so as to operate as such a partial of any directly related subatomic source of physical entity over time, is what works to define the existence of Gell-Mann-Najshima-Relations.

Different Degrees of Njenhuity

The difference between 2piI degrees and 96piI degrees is the different formats of their two respective genus-types of Njenhuity.  So, there are 48 different formats of genus-types when it comes to the Imaginary-based angles -- when this is determined in terms of the different formats of Njenhuities that exist among the various tensors that are Imaginarily based -- when certain Ward-Caucy bounds that are both covariant, codifferentiable, and codeterminable are to be compared in the various given arbitrary cases in which such relativistic tensors are to be compared.  So, there are 48 different differentially geometric genus-types of parity-based Njenhuity -- that may be mapped via their corresponding chirality-based Njenhuity formats -- in order that this may be used to describe part of the inter-relationships that exist among different superstrings and orbifolds that belong to different universes from within the Ultimon.  I will continue with the suspense later!  Sincerely, Sam Roach.

Part Two Of The Seventeenth Session Of Course Ten

As I was discussing, as the discrete units of the directorals that here correspond to the prior eluded tensors are considered over an arbitrarily given Fourier condition that inter-relates the related superstrings that work to comprise the assoicated said traits, residue that is here delineated over a relatively brief metric works to transversally and vibrationally commute a certain degree of "tingling" that lubricates the kinematic association that covariantly binds the two said traits.  The coupling that happens over the course of the prior mentioned brief metric is an arbitrary given example of a Yakawa coupling that here involves indices that works to allow a variance that translates a tense of Weyl covariance that tends to conform to the corresponding Ward Caucy conditions that work to define the physical boundaries of the said traits in all of the Fourier-based derivatives that involve the overall dimensional scope in which the superstrings that work to define the said traits exist in.  The corresponding Cassimer Invariance that will happen here -- if the related Yang-Mills supersymmetry is to here take hold -- will then attain a spontaneous metric that here involves a parity and dual chirality that will work to even out the loci of the settings over the duration in which each associated encodement is quantized.  Yet, if the corresponding Yang-Mills supersymmetry that we are to consider were to not be attained here, then the associated holomorphic residue will flow over the duration of the brief metric that inter-relates this second possible scenario -- after each reiteration that would thence happen between the homotopic indices of the said traits.  The prior mentioned metrical condition would cause the metaphorical-based "fluid" flow that I had initially mentioned in my last post to become perturbated in terms of its displacement over a tightly-knit Fourier Transformation in which the traits mentioned earlier will, in this case, not be as superconformally invariant as these otherwise would be.  Under the conditions of such a perturbation of what would otherwise be more delineatorial-based stable, the inter-related fractal of magnetic coupling that could be extrapolated here would involve an increase in magnitude as well as an increase in terms of the corresponding fractal of charge.  The "fluid" would then snap and recoil in terms of its delineation over the course of the prior mentioned tightly-knit Fourier Transform.  If the associated holomorphic index that would then exist under the directly prior mentioned conditions were to now increase in terms of action intensity over the course of the kinematics that would involve the covariance of the related eigenstates that are comprised in part by the superstrings that work to form the prior mentioned said traits, then the recoiled sections of "amorphous" quantitative topology may -- after the coure of the proper sequence of iterations and the proper series of wave discharge -- slip in terms of its positioning of local distribution as a folded manifold to where it would go back into a connection that would here exist in-between the hyperstates of the said traits in so that the exterior counterpoise that would here be physically present, as well as the corresponding hypnostates of the related holonomic ground-states, would then differentiate through time in a singularized manner in so that the given phenomena would then act as a theoretical homotopical-based eigenbasis.  Such an eigenbasis would here be partially codifferentiable in terms of the inter-relation of the covariance of the two said traits over a related Fourier Transformation in such a manner so that the related activity would work to draw in the quanta of a re-convergent norm projection. I feel that I am burning the candle at both ends.  I will continue into course 11 when my sanity lets me.  I will continue with the suspence later!  Sincerely, Sam Roach.

Some More About The Light-Cone-Gauge

As to the discussion about two sets of superstrings that differentiate covariantly over a given arbitrary Fourier Transformation:  The discribed activity here repeats its mentioned mode in a manner so that it involves a reiterated sequential series of corresponding instantons that strays in a general spot in such a manner so as to not go as a group through a discrete unitary and/or tree-amplitude-based unitized directoral.  The more that a Wilson-Line develops in terms of having more of a basis of unitization among the superstrings that form the said two mentioned substringular groups taken individually -- and especially when such unitization combines the two said groups -- that potentially causes these to form a syncronization that will pull these into a motion that involves a discrete Lagrangian.  Then, such a unitization may spontaneously allign the parity between these related superstrings in such a manner that these would thence converge the arbitrarily related holonomic discharge of substringular field (mini-strings of which form the physical entity of the said field) which, if the Noether-Based flow of  the prior mentioned substringular group catches up with what was earlier the prior mentioned arbitrary tachyonic-based substringular group, this would then need to be on account of what would appertain to a minor spuriousness in the tachyonic scattering of both substringular groups. An example of this, when photons scatter, these are initially tachyonic for relatively few instantons.  Right after that, the said photons that just scattered slow down more than these initially sped up, as according to Snell's Law.  These photons -- in the process -- catch up to the orbifolds in which these are to quantize with in such a manner that photons that travel outside of a vacuum always travel slower On Average than these would travel in a vacuum.  Again, this happens as Snell's Law indicates.  This will be much further discussed in future books that I wrote. 
I will continue with the suspence later!  Sincerley, Samuel Roach.            

The Second of the Three Parts of the "Next" Session of Course Nine

The more that a Wilson Line develops in terms of having more of a basis of unitization among the superstrings that form the said two mentioned substringular groups taken individually -- and especially when such unitization combines the two said groups in a manner that potentially causes these to form a syncronization that wilil pull these into a motion that involves a discrete Lagrangain, the more that such a unitization may spontaneously allign the parity between these related superstrings of which would converge the arbitrarily related holonomic discharge of substringular field (mini-string fields) which, if the two Noether-Based flows of the two prior mentioned substringular groups catches up with the prior mentioned arbitrary tachyonic-based substringular group on account of what would appertain to a minor spuriousness in the tachyonic scattering of the substringular group that was Njenhuisly perturbated, then, the three groups which here represent three orbifolds will thus produce a perturbation in the related covariant codifferentiation that will potentially alter any potential Kaluza-Klein topology in the said three orbifolds into a Yang-Mills topology.  But, here, the homotopic residue of each mentioned substringular group will maintain its Fourier-based generation of substringular field as the said groups propagate along the Ultimon.  This is so that the previously mentioned homogeneous wave permittivity will allow for the commutation of spin symmetry via the indices that are local to all three substringular groups at one group metric or another on their way thru the Continuum, differentiating timewise with the chirality of the residue as it vibrates. Such a wave permittivity will then be in proportion to the related norm-conditions that are in transition via a covariance with the angular momentum of each sector of the mentioned substringular residue.             

Session 2, 3, and 4 of Course One

What do you think of when you conceptualize a circle? A circle is a curvature that

             
connects smoothly, and the distance from its center and its exterior is constant. In order

for this shape to be a circle and not a sphere, the shape must be flat. The exterior of the

circular shape is ideally a hoop of infinite thinness. As I have stated before in the last

course, something of infinite thinness has no thickness, and therefore does not exist.

Fact. Circles exist, yet there are never ideal. What is termed as a circle is actually a

hoop or a thin cylinder or an idealized theory that that is used to scientifically predict

something.

Make a “circle” yourself. Draw a line right thru its center from right to left. This line is

the diameter of the circle. Label the top of the circle as one and the bottom of the circle

as negative one. Stuff below the line is negative and stuff above the line is positive.

Have your finger trace the positive arc of the circle from right to left. This arc is a little

over one-and-a-half times the length of the line in regards to the diameter of the circle.

Now, if the line went from bottom to top, the circle would be oriented from 90degrees

from the line taken from before and vice-versa. Imagine spinning the line like the spinor

of some board game. The outer part of where the line swept would define the outer

boundaries of the circle.

Last lesson, we discussed a one-dimensional string as point that get caught-up with

each other due to their point-fill and their forming nearness as it was encoded for by

the prior iterations of those points as these had codifferentiated with other similarly

encoded points. We also mentioned the Fock Space that enabled their waves to have

a counterpart as the points of the strings ebbed in their wave’s oscillations. Point

phenomena races throughout the world-tube. So, it doesn’t just form exact and linear

differential associations at the locus of the one-dimensional strings. Fringes here are

what form on the outside surroundings. Fringe phenomena forms “circles” which two-

dimensional strings. Here, too, the points that encode at a position codifferentially as

half-full while yet its wave residue form a two-dimensional string at that general locus.

The string is encoded at that position due to how its constituent points were differential

upon by semigroups in-between prior iterations, how near the points wee brought to

each other due to exterior forces, and the intimacy of the associated Fock Space with

the forming wave residue that the forming string is acting to expel. What do I mean by

expel? I will discuss that later. Just remember, if a string of info has an even symmetry,

then, it has parity. A string with Real parity is one that bears actual residue. Residue

that is non-functional is always part of this residue. It becomes functional by being used

where it belongs. Imagine. Parity is said to have Cassimer Invariance when the residue

is not emmited at that stringular locus after many reiterations. The fray of its operand is

then renormalized, sending it elsewhere to be used as Real residue.                                  

A Description of Ghosts Of Schwinger Indices Via The Rarita Structure, Part Two

The motion of the vibrations known as Schwinger Indices causes the norm-states that are in the path of such a motion per a sequential series of instantons through a group metric that defines a very limited Fourier Transformation to be redistributed in such a manner so as to form a physical memory of where the associated Schwinger vibrations were and how these were delineated. Such a physical memory is known as a ghost of a Schwinger Index via the Laplacian trajectory of the Rarita Structure when considering a physical memory at one instanton. When considering a homeomorphic phenomenon of such a physical memory that is discrete over a sequential series of iterations, then the said Fourier related phenomenon is a kinematically based eigenstate of Schwinger Index vibration as defined by the partial differentiation of a segment of a Rarita Structure eigenstate over a limited number of instantons. The integration of the related previously mentioned differentials in order to form an isomorphic quantum of directly related physical memories which form a reverse fractored discrete ghost-like pattern is known as an eigenbasis of ghost anomalic indices of the Rarita Structure that bear a commonality of parity, angular momentum, and spin-orbital momentum.

GUFT, Session 14

What makes the gravitational force stronger than the weak force? The weak force is the spontaneous force of neucleons to degenerate so that the atoms of the given neucleons will break down into simpler atoms that do not have as many protons and so that these given atoms will not have as many electrons. An atom of an element has as many protons as electrons in so long as this atom is not ionic. Ionic atoms are unstable. Atoms that are not ionic are stable unless these are spontaneously radioactive. Spontaneously radioactive atoms are of short-lived elements. Short-lived elements decay spontaneously because of the weak force. The weak force is a mini-string pull that exists because of the weak gluon combination that binds the given neucleons and the Van der Waals like metric-gauge of the electrons that associate at the outer valence levels of the spontaneously radioactive atoms of the elements given. This mini-string pull is intrinsic to a gluonic force that is tied in a non-superconformal way in that the De-Sitter and Anti-De-Sitter forces of the gluons work to unfurl the given gluonic force due to singularized mini-string tug that is not hermitian and non-perturbative because the interior mini-strings are relatively isolated in terms of spacial metric-gauge-tug neighborhood. This pulls the gluons apart and thereby produces less protons in the nucleus of the given atom. The Van der Waals like energy of the given electrons at the outer valence shells holds these weakly by loose mini-string-tug. The surrounding forces thus remove these outer electrons from the given Real Reimmanian plane. So, the weak force is due to the surrounding forces scattering the isolated mini-strings of overbuilt protons and overbuilt electrons shells. The protons of an atom work together by electromotive force. The build up of excessive protons produces a strong electromotive force in the nucleus that damages gluon fractal modulae in terms of impedance and permittivity because the hermitian and non-perturbative nature of the gluons begins to implode. That produces the prior conditions. Gravity, however, has multiple strands of mini-string that interrelate sets of supplemental norm thru Ricci Scalar eigenstates that push or pull upon all forces via the gravitational formation of the interdimensional Lagrangian of space-time cushion. The ordered and linear fashion of Ricci Scalar eigenstates that intertwine in a multi-faceted intwining that is generally not isolated causes the gravitational force to be stronger than the weak force.
The severred protons, two of these at a time, are then shot out of the atom along with two loosely held electrons to restructure as an alpha particle or helium atom that radiates outward. Sometimes, other electrons on the outside of the atom shoot out as Beta radiation. Sometimes, space energy of an atom shoots out as light or gamma radiation. Occasionally, neutrons then form as protons because of a change in parity and chirality that I described above yet as a reverse process. Changes in gluonic force and changes in electromotive impedance and permittivity may alter the spin-orbital delineation and orbifold handedness in terms of the directoralization of the orbifold Gaussian norm conditions of protons and neutrons to bring about these changes.

GUFT, Session 11

Electrons have wave-tug. Protons have wave-tug. All physical phenomena have a certain degree of wave-tug upon all other physical phenomena. Even ghost anomalies exhibit a certain degree of wave-tug upon all other physical phenomena, and ghost anomalies are often considered to be non-physical, partially since these are only a memory of superstrings and also partially since ghost anomalies of a light-cone-gauge-eigenstate are not plucked by the gauge-bosons that exist in the region of that given light-cone-gauge-eigenstate. Electrons have a charge, as do protons also. Yet, the charge of electrons is negative while the charge of protons is positive. The reason for this is the holomorphicity of electrons versus the holomorphicity of protons. Electrons have a holomorphic wave-tug basis, while protons have an antiholomorphic wave-tug basis. The impetus of an electron is holomorphic, while its impedance is antiholomorphic relative to a framework that establishes the neucleus of t he atom as its center. Since the neucleus of the atom is its center, the impetus of the electrons is left-tended. The impetus of an electron is the metric-gauge directoralization here. The metric-gauge directoralization taken kinematically is its attraction. Protons have an antiholomorphic impetus directoralization, since these want to move outward toward the electron. The reason for this is that protons are bosonic masses of high mass and direct wave-tug upon electrons. This wave-tug is formed by the parity and chirality of the orbifolds and their correlative superstrings. The protons thus have an antiholomorphic metric-gauge directoralization that is kinematically an antiholomorphic attraction. Thus, electrons have an antiholomorphic impedance and protons have a holomorphic impedance, since impedance is an equal and opposite reaction directed upon impetus. Thus, electrons have a holomorphic permittivity and protons have an antiholomorphic permittivity. Parity refers to the spin symmetry, while chirality refers to the handedness of the orbifolds in terms of the relative Gaussian Jacobian eigenbases of the orbifolds and the protons and electrons as a whole. A Jacobian eigenbasis refers here to a relative differentiation in the Gaussian structure of an orbifold.