Showing posts with label Kaeler. Show all posts
Showing posts with label Kaeler. Show all posts

Saturday, November 14, 2009

About E(8)xE(8) Gauge bosons

An orbifold is a structure that contains one basic set of superstrings. An orbifold bears a fractor of magnetism that is induced by the Majorana-Weyl covariance of the superstrings that it contains. An orbifold eigenset is a basic set of orbifolds. An orbifold eigenset bears a discrete magnetism that is induced by the Majorana-Weyl covariance of the orbifolds that is contains. A Majorana-Weyl  covariance is the codifferentiation of the magnetic indices of a subatomic phenomenon. Magnetic indices are Campbell norm and Hausendorf norm states that generate gauge-metric via the action of spin-orbit. So, as superstrings obtain a translation of spin-orbit, an orbifold bears a set of Campbell and/or Hausendorf indices that are generated through space to obtain a magnetic effect. The Campbell and Hausendorf indices here that are thence generated are Majorana-Weyl indices, and the codifferentiation of these magnetic indices is an example of Majorana-Weyl covariance. Likewise, as orbifolds obtain a translation of spin-orbit an orbifold bears a set of Campbell norm and/or Hausendorf norm indices that are generated through space to obtain a magnetic effect. These norm indices here that are thence generated are Majorana-Weyl indices, and the codifferentiation of these magnetic indices is an example of Majorana-Weyl covariance. The Majorana-Weyld indices of an orbifold are a fractor of the Majorana-Weyl indices of an orbifold eigenset. When an orbifold is connected to one or more orbifolds of an orbifold eigenset, there is a buffer connection between these orbifolds that is at the conicenter of the substringular field, made of mini-string, that helps to trigger the Wick Action. When an orbifold and/or and orbifold eigenset is "backgammoned" into a change of norm conditions in terms of the conformal invariance of the given orbifold and/or orbifold eigenset, this buffer connection known as an E(8)xE(8) gauge boson will torsion to pull/push to induce the Landau-Gisner Action to work through the Fischler-Suskind mechanism to trigger the Higgs Action to raise the Klein Bottle to the locus of superstrings that are running out of permittivity so that the Kaeler metric may happen to bring metric-gauge back to the discussed superstrings so that these may have the permittivity that these need to be the energy that these are so that energy may exist. The Kaeler metric also settles the vibration level of Fadeev-Popov-Ghosts so that these may have the impedence that these need to have so that the world will not be charred by an Imaginary Supercharge. Each time that the Kaeler metric goes through an iteration, at the time (metric) that the superstrings that were in the Klein bottle go into Regge Slope, the E(8)xE(8) gauge bosons are undone of torsion to allow for the associated superstrings to go through ultimon flow. Once the discussed superstrings are done with the Kaeler metric, the E(8)xE(8) superstrings not only stop having torsion, yet these become completely hermitian until Gaussian Transformation is to happen again. A Hausendorf Projection may be a Wick Action in terms of gauge-action when it is localied and directoralized toward the effecting of a Landau-Gisner Action during a metric when this effect is to occur. A Wick Action is always a Hausendorf Projection, yet a Hausendorf Projection is not always a Wick Action.

Tuesday, October 27, 2009

FTAAN, Session 15

Protons and neutrons exist in a state of conformal invariance when these exist in the nucleus. Protons and neutrons consist of quarks, leptons, and gluons. A proton consists of gluons, two quarks, and one lepton. A quark has a charge of (+2/3). A lepton has a charge of (-1/3). So, a proton has a charge of (+1). A neutron consists of gluons and two leptons and one quark. So, a neutron has a charge of 0. Neutrons are neutral in charge. Neutrinos are also neutral in have. Protons and neutrons both have gluons, and gluons have no charge. Protons and neutrons differentiate in a vibratory kinematism that generally has a harmonic transversal motion that bears a parity and chirality that is even and Real in terms of the relatively stable oscillation of the particles that are relatively stationary when one takes the first-ordered relative motion of these given particles during transient periods of time when the given protons and neutrons are not physically perturbated by an outside force. The particles of the given protons and neutrons at the substringular level differentiate superconformally except for the vibration of the particles, although this superconformal behavior is not as limited to the prior said differentiation as with the gluons when one considers the successive motion of the leptons and quarks. The said superconformal behavior only applies to a situation of first-ordered relative motion, such as the eminent behavior of a gluon, quark, or lepton. Neutrinos have an eminent transversal motion that bears a mass of 10,000 superstrings that are Imaginarily Yau-Exact. Imaginarily Yau-Exact means that the superstrings are hermitian and non-perturbative off of and then on the Real Reimmanian plane after successive iteration. This Imaginarily Yau-Exact condition is conformally invariant in terms of the spin-orbital and radial differentiation of the given one-dimensional superstrings, although these given superstrings eminently are propagated through a transversal kinematism that differentiates directorally in a relatively Snell manner, unless these are electrodynamically, or otherwise physically, perturbated by any given holonome that interacts with its Gaussian eigenbasis. If this eigenbasis is altered in such a way that the Landau-Gisner-Action of the given neutrinos happens the Fischler-Suskind-Mechanism alters the Higgs Action in such a way so as to alter the given Klein relation. The Ricci Scalar will then perturbate to produce a Kaeler/Calabi metric that will alter the state of these neutinos. The prior potential of what was neutrinos will now have a dissapation that may, through the proper electromagnetic reinforcement, form a potential energy for the formation of other neutrinos. Hint: Cause the eletromagnetic reinforcement to have a reverse-perturbative potential so as to be able to create neutrino energy from the Kaeler/Calabi heavy water holomorphism that trapped the neutrinos.