Archive for the 'String Theory' Category

Dec 22 2023


As presented before, a magnetic field can bend a charge path, but not speed it up or slow it down. k-planes are produced by magnetic fields, whereby they manipulate the direction of electric fields. Due to a charged mass, k-planes are produced, and this means that electric fields of gravitons are bent into the same plane as the vector potential comes through. A vector potential can be a charged mass or a group traveling through the gamma ray field before acting on another charge.

When two graviton electric fields are combined it is called a “k-th Chern class ck(E)” ([1], pg. 309) and a “2k form γk“. When a “4k-form βk” ([1], pg. 309), it is called a “Pontrjagin class”. We may think of a Pontrjagin class as a flat picture of a mountain range with 4 mountains in the picture. It is not a sine or cosine curve, but has 4 lobes. The curve that defines the tops of the mountains can be thought of as a string. Statistically, lobes may be combined at times. There are “two elements (A, p) and (B, q)” ([2], pg. 216), and q is the distance the p moves laterally to help form a hypersurface k-plane. For example, there is a “2k-form on P” ([1], pg. 293) for a Chern class, and in any k class there is “oriented p-planes in Rp+q” ([1], pg. 271).

k-planes are created to do heavy work, and are parts of larger Lie groups which determine the chirality. As the group approaches another charge, it determines whether the charge is positive or negative. If it is of the same charge sign, the Lie groups instruct the k-planes to slap the target charge on the face. If the target is the opposite charge sign, the k-planes split, spin around, and slap the target charge on the back. After 18 years, we really need the String Theorists working on the mathematics of this.

The k-planes take up new gravitons quickly and leave others behind. It is its own entity within a Lie group, and “(g, h, σ) is effective” ([1], pg. 249), σ being the effect of the magnetic field.

[1] Kobayashi, Shoshichi and Nomizu, Katsumi, “Foundations of Differential Geometry Volume II”, John Wiley & Sons, Inc., c. 1969

[2] Kobayashi, Shoshichi and Nomizu, Katsumi, “Foundations of Differential Geometry Volume I”, John Wiley & Sons, Inc., c. 1963

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Oct 16 2023

Atomic and Molecular Electron Arcs

Further to uniting Riemannian geometry, Lie groups, and symmetric spaces with gravity, τ is an atomic or molecular arc, and “τ is a segment” ([1], pg. 168). Also, “τ is minimizing” ([1], pg. 166).

Sometimes τ is called a complete orbital, and we “divide τ into a finite number of arcs, say, τ1, τ2, … , τk” ([1], pg. 191).


In an orbital arc the “endomorphisms A1, … , Ak are linearly independent” ([2], pg. 353), and k – 1 in this instance is the number of gravitons absorbed in an arc. “A” is the vector potential, and each time an electron absorbs a graviton in an orbital, its vector potential increases. We know that A1, … , Ak is not pulsed Lie groups in the gamma ray field, because there is no “…” after the Ak. In the same paragraph it talks about a “mapping ξ → Aξ“, therefore in a particle mass, and in groups or manifolds in the open gamma ray field, the gamma rays are blended and surjective.

If a function can be called “the growth of an orbital electron in size and charge”: ,

then “γ and f point in opposite directions” ([3], pg.165).

The Φ field is within atomic and molecular orbitals, including the boundary, and Ψ is outside of the orbitals. In an emitting antenna, it is the Ψ field as well, since the electrons are free. “Φ0 is isomorphic to Ψ0 in a natural manner” ([1], pg. 193), because the gamma ray field is normally constant in the area within and around the molecule.

Often in a molecule, or any type of p orbital, the Gaussian curvature, when ¾ through the arc compared to ¼ through the arc, is negative.

In the open gamma ray field “m = dim M and n = dim Δ” ([4], pg. 155), and m – n is the number of singularities in a locality. Stoker terms it “singularity in the coordinate system” ([5], pg. 84). A singularity is when the electric and magnetic fields of a gamma ray cross over the t axis, though when near the axis it could be called a singularity also.

If the polarization factor is greater than 2, as at the surface of the sun or Jupiter, then specific nuclei likely have more mass than on the face of the earth, and electrons in atomic or molecular arcs grow larger. It could be because of these factors the value of Newton’s gravitational constant G = 6.672 x 10-11 (N-m2)/ kg2 stays the same.

[1] Kobayashi, Shoshichi and Nomizu, Katsumi, “Foundations of Differential Geometry Volume I”, John Wiley & Sons, Inc., c. 1963

[2] Kobayashi, Shoshichi and Nomizu, Katsumi, “Foundations of Differential Geometry Volume II”, John Wiley & Sons, Inc., c. 1969

[3] Mackenzie, Kirill C. H., “General Theory of Lie Groupoids and Lie Algebroids”, c. 2005 Kirill C. H. Mackenzie, London Mathematical Society

[4] Boothby, William M., “An Introduction to Differentiable Manifolds and Riemannian Geometry”, Academic Press, 2003

[5] Stoker, James J., “Differential Geometry”, John Wiley & Sons, Inc., c. 1969

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Aug 27 2022

Concentrated Group Action

There is another slightly different view in which the Coulomb field transmits when it comes to nuclei as parts of molecules, and that is by pulsating, concentrated Weyl groups or frames of a small conical angle, toward another nucleus. It is not wholly different from the last blog entry because spherical pulses could also be seen as groups, and for a given charge these concentrated groups are in addition to spherical groups.

When an O2 or N2 binuclear molecule forms, or let us say a benzene molecule, each nucleus senses the other nuclei closest. This is a strong repulsion, so the nuclei may start sending out groups concentrated toward the other nuclei for efficiency, while the electron cloud in between the nuclei offers attraction and keeps the molecule from flying apart. This also changes the Calabi-Yau structures within the nuclei.

For Coulomb attraction, a frame may wrap around another charge. For Coulomb repulsion, there may be partial contact and some backflush. As two close nuclei in a molecule sense each other, there may also be alternating, concentrated, group pulses between the two. This is likened to a synchronization between the nuclei, without the need for backflush. With phonon transmission this is a very fast process and transmits without intercepting electrons in orbitals. When we compare the size of nuclei and electrons to molecular size, there is a lot of empty space filled with gravitons, so this synchronization is reasonable.

In larger nuclei there are more compact spaces and more affine connections between them. For a nucleus we may call these irreducible representations, where the exception is fission, as a “reduced root system in V” ([1], pg. 461). The nuclear charge manufactures springboard groups repeatedly, with oscillations and accordion motion in multiple axes. A stable nucleus in a molecule is an isomorphism, though we must be careful here because as orientations change, there may be slight changes in structure. Particle colliders are excluded from this discussion.

A nucleus consists of involutive automorphisms, the summation adding to the entity’s spin, as it absorbs gravitons for the energy to send out groups or frames. Boothby calls these “inner automorphisms of G” ([2]. Pg. 237). A Weyl chamber is part of atomic mass, while a Weyl group transmits as a packet in the not so compact space of the gamma ray field.

We see that “π is a continuous and open mapping.” ([1], pg. 120]. In certain areas of deep space we may call this Riemannian globally symmetric space I, with perfect sine waves and no circular polarization. “Riemannian globally symmetric spaces of type II” ([1], pg. 516) are due to the bi-invariant structure of the Coulomb field. In both cases there is a “strong orthogonality” ([1], pg. 576) which produces a polarization factor of 2, as used in the blackbody radiation formula and in G = 4hf/3. π may be called a free graviton, since it is one half wavelength long.

As far as the Coulomb field produced by an electron in an atomic or a molecular orbital: “Let N0 be a bounded star-shaped open neighborhood of 0 ϵ g which exp maps diffeomorphically onto an open neighborhood Ne of e in G.” ([1], pg. 552) Let e be the electron, star-shaped be the lobes of orbitals, and exp be the growth of an orbital electron in size and charge. The increase in size of an electron in the orbital enables it to absorb more gravitons at a given time, thus increasing gravitational pull in the second half of the arc.

[1] Helgason, Sigurdur, “Differential Geometry, Lie Groups, and Symmetric Spaces”, American Mathematical Society, 2012

[2] Boothby, William M., “An Introduction to Differentiable Manifolds and Riemannian Geometry”, Academic Press, 2003

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Mar 29 2022

Transmission of the Coulomb Field

The gamma ray field we live in is extremely rich and dense.  For the forms we find in nuclei and assorted particles, there is all the energy needed to drive all physical processes.

A Calabi-Yau shape within a nucleus or particle needs an external energy supply to maintain it. Gravity provides the energy. Here we are talking about force and pressure within a nucleus or particle, with only indirect connection to the outside, or connection at a point, curve, or surface.  There may also be tears joining and reforming.

Occasionally we refer to neutrons, protons, electrons, and nuclei.  A proton can be a hydrogen nucleus, though we list it separately when we talk about free protons, such as in the solar wind, particle colliders, or elsewhere.  Let’s take an Oxygen nucleus for example with the makings of 8 protons and 8 neutrons. Inside the nucleus, at the top, parachutes with baskets attached through ropes, or strings, instead of a parachutist, may cause some gravitons to loop around the insides of the parachutes, or branes, and into the baskets with enough force to hold the parachutes against the highest flux density of gravitons. Then the gravitons would find ways to tunnel through the baskets, pushed from behind.  In the motions of O2 in air, the parachutes may slide around to stay opposite the maximum flux.

This may also help explain weak interaction parity violation, because as an electron forming within a nucleus tries to escape, out the bottom is easier, due to escape out the top involving going through the gaps in the parachutes.  More than 50% would come out downward.

The manifold of the sun’s gamma ray field, the manifold of the earth’s gamma ray field, and likewise with other celestial bodies, provides a combination of symmetric spaces. During the day, at noon let’s say, the vectors of the sun’s manifold are in the opposite direction as the vectors of the earth’s terrestrial manifold. The Coulomb field uses all vectors of all manifolds to propagate, because all vectors, within a distance of 10 meters at least, are frozen in time for phonon transmission.

Let’s say M1 is the earth’s manifold, and M2 is the combination of the earth’s and sun’s manifolds. “…a diffeomorphism F: M1 → M2 of manifolds oriented by Ω1, Ω2, is orientation-preserving if F*Ω2 = λΩ1, where λ > 0 is a C function on M.” ([1] pg. 209) In our example here, λ > 1, and we have neglected the earth’s moon for simplification.

We may call a negative charge a left coset space, and a positive charge a right coset space. Each creates its own homomorphism in the dense gamma ray field, by a diffeomorphism on the electric fields of the gamma rays.  For one thing, there is circular polarization. For another, perpendicular to the greatest flux density of gamma rays the electric fields of the gamma rays may have skewed sine wave lobes, somewhere between a normal sine wave and a sawtooth. The Coulomb field acts tangent to the R vector sphere, and “(∇XY)p depends not on the vector field X but only on its value Xp at p.” ([1] pg. 309]  The way that the Coulomb field transmits radially is by centrifugal force through the gamma ray field.

The inside of an atom may be called a geodesic.  An electron path in an atomic orbital may also be called a geodesic, and “a long geodesic may not be minimal.” ([2] pg. 62)  This is due to the Lorentz force:

Gravity is an integral manifold.  Each orbital arc is a line integral absorbing gravitons.  The Coulomb field, on the other hand, is a charge induced diffeomorphism in the gamma ray field. Substantially outside of neutral atoms there is a propensity for positive and negative charges to cancel, though in the near field we have van der Waals forces.

Phonons for the Coulomb interaction are generated inside a charge.  The field created, that acts on another charge, may act on the outside of another charge, possibly only 5% of the diameter deep.  The fields may also act in the interspace, producing backflush to the charges that generate the fields.  Phonons of opposite chirality attract, and of the same chirality repel.

As points meet for the Coulomb force, the acceleration would be periodic, and relates to the vector potential.  A Fourier Series can be applied to the vector potential, with the direction of force being the side of the ‘x’ axis where the sine or cosine function has larger lobes.  Often a geodesic is called piecewise smooth, due to gravitons being separate, though on a classical scale the motion is smooth.

Two electrons can occupy the same atomic orbital if they have opposite half-integer spin projections.  This is the Pauli exclusion principle.  In terms of tensor math, “the subspaces are mutually orthogonal and each is a nontrivial irreducible subspace.” ([1] pg. 242)

[1] Boothby, William M., An Introduction to Differentiable Manifolds and Riemannian Geometry, Academic Press, 2003

[2] J. Milnor, based on lecture notes by M. Spivak and R. Wells, Morse Theory, Princeton University Press, 1969

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Feb 11 2022

Isotropic Property of the Coulomb Potential

In the vicinity of where our machines have been, we know that electric current will flow in any designated direction and is not particular to the direction of the highest flux density of gravitons.

For various reasons, we cannot have protons and electrons continuously flipping, – the Stern-Gerlach experiment proves that they do not. There must be internal processes of the proton and electron which produce isotropic electric fields. Some of this was previously addressed in two blog entries:

It is possible that not all conjugate wave gravitons pass straight through a proton or electron, or that even with a free proton or electron that the gravitons leaving have just entered. Some may make a horseshoe pattern and come out near the same point entered. They may be able to come back out at any angle. As compressed as the gravitons become inside a particle, almost any shape can occur. Gravitational pressure dictates a consistent size of a free proton or electron.

With the flux density coming out of the face of the earth, we seem to have a conundrum with the idea of gravitational pressure, one side having much greater pressure than the other. Why do gravitons not burst out the top, resulting in particle collapse? It also begs the question as to why electrons are perfectly round, and not teardrop shaped:

Possibly, branes form at the top of an electron and reform in a spin flip.  These branes would be linked inside the particle so that they do not bust out, and may deflect some exiting gravitons at various angles. These branes may also help keep the electron round. Here we are designating “top” as away from the highest flux density of gravitons.

As far as isotropic fields, at this point we must say that it is designed internal to the proton or electron and is of consistent pattern.  The open field starts just outside the particle, so it is maintained that electric and magnetic fields transmit openly by “phase shift and chirality” or “phase shift and parity”.  The Coulomb force is considered instantaneous at reasonable distances:

It appears as though this is necessary, because then the speed that free gravitons travel at, the speed of light in a vacuum, does not effect the electric and magnetic fields generated.

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Feb 10 2022


Inside a proton or electron, events may approach the Planck length.  The frequency of the waves would not change from that of a free space graviton, though wavelength and amplitude do change.

Waves inside a particle may make loops in certain circumstances, not necessarily around the perimeter, though internally, and required because of all the traffic.

Certainly, the ways these vibrations set up in a proton or electron determines whether we have a positive or negative charge.  If we did not have any loops and curves, the versatility needed would be hard to set up.  It is somewhat like a Hilbert space with wrapped up dimensions.

Put another way: “A string vibrating in one particular pattern might have the properties of an electron, while a string vibrating in a different pattern might have the properties of an up-quark, a down-quark, or any of the other particle species in Table 12.1.  It is not that an “electron string” makes up an electron …Instead the single species of string can account for a great variety of particles …” *

If you peruse this website, you will find other areas of unification.

* Greene, Brian, The Fabric of the Cosmos, c. 2004 Vintage Books, a division of Random House, Inc., p. 346-347

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Feb 09 2022

Core of an Electron or Proton

We can see from the calculation of the diameter of a free electron that as the density of the gravitational field goes down, the diameter increases.  This would be because of less gravitational pressure on the outside of the electron.

As gravitons enter a proton, electron, neutron, or nucleus, as conjugate waves or to take residence, the buildup takes on a fuzzy look that makes them look larger.  If we take a core diameter of 1.3335 x 10-15 m, the part that produces the fundamental charge, and add one graviton wavelength, we arrive at 5.30 x 10-15 m diameter, which is close to the classical diameter of the electron, 5.64 x 10-15 m *.  One graviton wavelength is used because one-half wavelength is on one side of the electron and one-half wavelength of a different graviton is on the other side.

We may call these outer layer gravitons tentacles or strings.  When nuclear fission occurs, the de Broglie wavelength of a neutron can come in at an angle where the strings on each entity hook and help pull the neutron into the nucleus. The cross section for this process is larger for slow neutrons vs fast neutrons in part because of the longer de Broglie wavelength.

* Jackson, J. D., Classical Electrodynamics, Third Edition, c. 1999 John David Jackson, John Wiley & Sons, Inc., p. 695

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Jun 22 2010

Subatomic Particle Structure

Research on the internal structure of subatomic particles has been ongoing since the early days of particle accelerators and cosmic ray experiments, and there are several points of view that merit study.  The view promoted here has not much new, and should sound familiar.  The very stable proton, as CERN would agree, is a worthy starting point.

First of all, “there is no hard core to the proton. … It could be like jelly, or it could be like a strawberry, with seeds scattered throughout, but no accumulation of them at the centre.”  When scattering e + p is elastic, the resulting Bjorken scaling “is interpreted as indicating that the scattering takes place off point like constituents of the proton, called partons.”, where “the structure factors are functions of ω only.” ([1], pgs 16-18).

Since “q is the photon 4-momentum”, for “an individual parton of mass m” we can use the relativistic mass of the graviton, mg = 5.575 x 10-28 kg [2], in which case the dimensionless ω = (2Mν)/q2, with q2 = 2mν ([1], pg 17), gives ω = mp/mg = 3.

One may think of the internal structure of the proton as a crystal lattice, with nodes, or partons, that are basically zero points of eigenvectors, where internal and pass through wave functions add or subtract momentum.  If you are a string theorist, added head to tail you may choose to look at the vector structure as vibrating strings.  If you have a Mechanical or Civil engineering degree you may think of the structure as finite elements, – not necessarily tetrahedral however.  The nodes are the seeds of Ryder’s strawberry.

The defined boundary of a subatomic particle results from gravitational pressure at its barrier domain.  Let us view then the particle as a wave packet “when the wave packet is subject to the influence of a parabolic potential.  Physically, this result arises from the fact that the tendency of the wave packet to spread is compensated by the potential, whose effect is to push the wave packet towards the origin from regions where V(x) is large.” ([3], Compl. Gv, 3.c., pg 572)  Due to gravitational pressure, V(x) would be large at the barrier domain of the particle.  With consistent frequency, ωg =  4.75 x 1023 rad. sec-1 [2], gravitons step through the barrier easily.

Baryons and fermions would be similar in structure, though differing greatly in density.  Scattering can happen through barrier elasticity or partial penetration with node to node scattering.  Deeper node penetration on a large nucleus can result in alpha decay.

[1] Ryder, Lewis H., Quantum Field Theory, Second Edition, Cambridge University Press, 1996


[3] Cohen-Tannoudji, Dui, Laloë, Quantum Mechanics, Hermann, 1977, Paris, France

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Sep 16 2009

The Fundamental Quantum Unit

With the advent of gravitons serving as conjugate wave functions that hold subatomic particles together using gravitational pressure, we can go a step further.  Could it be that all material objects in our locale are made of gravitons?  If so, the graviton is the fundamental quantum unit, or otherwise we may call it quantum 1.
Kansas the band actually got closer to the truth than Oppenheimer did when it comes to particle theory relating to electrons when they sang “Everything is dust in the wind.”  They didn’t go quite small enough though if everything is gravitons.  Every material object in our solar system may indeed be made of gravitons, however we cannot go so far as to surmise that this may be true throughout the universe.
Newton’s law of gravitation still holds true.  The magnitude of the gravitational force exerted by one mass made up of atoms on another mass made up of atoms is:
F12 = Gm1m2/r122
If the gravitational field were more uniform as one travels out from the earth we could call it the Higgs field, but because the force exerted is inversely proportional to the square of the distance between the masses we cannot.  Additionally, since gravitons are so small and only one half wavelength long we could call them strings, – if only they made loops once in a while.

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