Posts Tagged ‘quarks’

Quantum Chromodynamics and R3+T Dual-Spin Elementary Particles

December 12, 2023

Since we live in a four dimensional spacetime, I have long known that it is possible for elementary point particles to have simultaneous independent spins on two orthogonal planes, for example, one rotation axis normal to the x-y plane, and another axis normal to the z-t plane. I discovered that when combined with the R3 hypersurface we live in within the R3+T universe, the projection of dual-spin particles onto the R3 hypersurface causes a single elementary particle to appear as (for example) two or three independent particles from our point of view.

This seemed like a great way to make progress on why we have bound systems of quarks but never see isolated quarks. I recently posted on this (see https://wordpress.com/post/agemozphysics.com/1754, for example). I had hoped that this approach would allow a more analytic view of quantum quark behavior than the perturbative methods we currently use in quantum chromodynamics, why we have bound quark systems that are color-charge neutral, and why we have the SU(3) color charge behavior of quarks and gluon interactions.

Alas, I found that dual-spin doesn’t lead directly to the SU(3) solution of chromodynamics or any of the rest of it. The observation in R3 of R3+T dual-spin particles yields three identical particles (see the 3:1 dual spin ratio shown in the figure) rather than two up quarks and one down quark, and gives no hint why most of the quark combinations in real life are unstable. It doesn’t explain conservation of baryon number, the large mass of the bound quarks in a proton, or any of the other things we see in quantum chromodynamics. Nor do I see nothing that points to where the different gluon color charge pairs come into play, for that matter, why we have gluons at all.

Here is the corrected (from the previous post) projection in R3 of a single R3+T dual spin elementary particle. Note this displays the spin direction only, there is no actual physical displacement. (You cannot have physical displacement within an elementary particle as it would cause all kinds of consistency problems in a relativistic environment). Each of these three R3 pseudo particles lie on an axis with a positive and negative direction shown.

I did a bit of research to see if anyone had looked at spins in four dimensions, or even if someone had published the fact that elementary particles in R3+T can have two simultaneous and independent spins that project onto our R3 hypersurface reality, and so far, it doesn’t look like anybody has considered this. There is no reason why a product of Pauli matrices couldn’t describe a real particle in R3+T, which I think gives the degrees of freedom we need for color charge in quantum chromodynamics. Indeed, the solution I found in the previous post listed above looks like it gives us the colors we need for quarks (red, green, blue). The fact that real-life elementary particles only have color neutral combinations (e.g., protons must have each of a red, green, and blue quark) to me hints strongly that the bound quark system making a proton is a single dual-spin elementary particle in R3+T.

So, I don’t want to give up. I still think I might be on the right track, or close to it. Do any of you agree or am I doomed to crackpot purgatory?

Agemoz

Properties of a Unitary Rotation Field

January 6, 2020

The unitary rotation field in R3+I dimensions is part of a quantum interpretation that obeys special relativity.   Recently I was able to show that the field can produce both linear and closed loop soliton solutions that do not produce discontinuities in the field.  This is a big step forward in the hypothesis that this field is a good representation of how things work at the quantum/subatomic scale.   Note that this field is NOT the EM field, which under quantum field theory reduces to a system of quantized and virtual particles.

This unitary rotation vector field is derived from the E=hv quantization principle discovered by Einstein more than a century ago.  This principle only allows one frequency dependent degree of freedom, so I determined that only a field of unitary twists of vectors could produce this principle.  (I didn’t rule out that other field types could also produce the principle, but it’s very clear that any vector field that assigns magnitude to the vectors could not work–too many degrees of freedom to constrain to the E=hv property).  This has two corollaries:  first, no part of the field has zero magnitude or any magnitude other than unity, and, the field is blocking–you cannot linearly sum two such fields such that a field entity could pass through another entity without altering it.

Why did I determine that the rotation has to be in R3+I, that is, in four dimensions (ignoring time for now)?  Because of the discontinuity problem.  If the field were just defined as R3, you cannot have a quantized twist required to meet E=hv.  No matter how you set up the rotation vectors around a twist of vectors along an axis, there must be a field discontinuity somewhere, and field discontinuities are very bad for any reality based physical model.  That makes the field non-differentiable and produces conservation of energy problems (among many other problems) at the discontinuity.

However, all of quantum mechanics works on probability distributions that work in R3+I, so that is good evidence that adding a fourth dimension I for rotation direction is justified.  It doesn’t mean there is a spatial displacement component in I–unlike the R3 spatial dimensions, I is just a non-R3 direction.  And the I dimension does at least one other extremely important thing–it provides a default background state for all vectors.  In order for photons and particles to have quantized twists, a background starting and stopping vector rotation is necessary.  The unitary field thus normally would have a lowest energy state in this background state.

Aha, you say–that can’t work, the vacuum is presumably in this lowest energy state, and yet we know that creation operators in quantum mechanics will spontaneously produce particle/anti-particle pairs in a vacuum.  You would be correct, I have some ideas, but no answers at this point for that objection.  Nevertheless, I recently was able to take another step forward with this hypothesis.  As I mentioned, it is critical to come up with a field that does not produce discontinuities when vector twists form particles.  Unlike R3, the R3+I field has both linear and closed loop twist solutions that are continuous throughout.

This was very hard for me to show because four dimensional solutions are tough to visualize and geometrically solve.  I’m not a mathematician (whom would undoubtably find this simple to prove), so I used the Flatland two dimensional geometry analogy to help determine that there are continuous solutions for vector twists in four dimensions.  There are solutions for the linear twist (e.g., photons) and closed loop particles.  There are also solutions for linked closed loops (e.g., quarks, which only exist in sets of two or more).

I will follow up next post with a graphical description of the derivation process (this post is already approaching the TL;DR point).

Now, this is a very critical step indeed–there is no way this theory would fly, I think, if field discontinuities exist.  However, I’m not done yet–now the critical question is to show that the solitons won’t dissipate in the unitary rotation field.  If there are no discontinuities, then the solitons in a field are topologically equivalent to the vacuum field (all vectors in the +I background state).  What keeps particles stable in this field?  As dicussed in previous posts, my hypothesis has been to use the displacement properties of quantum interference–now that the discontinuity problem is resolved, a more thorough treatment of the quantum interference effects on the unitary rotation field approach is now necessary.

Regardless of how you think about my hypotheses that unitary rotation vector fields could represent subatomic particle reality, surely you can see how interesting this investigation of the R3+I unitary rotation field has become!

Agemoz

Summary of Findings So Far

February 5, 2018

I took the time to update the sidebar describing a summary of the unitary twist field theory I’ve been working on.  I also paid to have those horrid ads removed from my site–seems like they have multiplied at an obnoxious rate on WordPress lately.

One problem with blogs describing research is the linear sequence of posts makes it really hard to unravel the whole picture of what I am doing, so I created this summary (scroll down the right-hand entries past the “About Me” to the Unitary Twist Field Theory) .  Obviously it leaves out a huge amount, but should give you a big picture view of this thing and my justification for pursuing it in one easy-to-get place.

The latest:  I discovered that the effort to work out the quark interactions in the theory yielded a pretty exact correlation to the observed masses of the electron, up quark and down quark.  In this theory, quarks and the strong force mediated by gluons is modeled by twist loops that have one or more linked twist loops going through the center.  This twist loop link could be called a pole, and while the twist rotation path is orthogonal to the plane of the twist loop, the twist rotation is parallel and thus will affect the crossproduct momentum that defines the loop curvature.  Electrons are a single loop with no poles, and thus cannot link with up or down quarks.  Up quarks are posited to have one pole, and down quarks have two.  A proton, for example, links two one-pole up quarks to a single two-pole down quark.

The twist loop for an up quark has one pole, a twist loop path going through the center of it.  This pole acts with the effect of a central force relation similar (but definitely is not identical to an electromagnetic force) to a charged particle rotating around a fixed charge source–think an atom nucleus with one electron orbiting around it.  The resulting normal acceleration results from effectively half the radius of the electron loop model, and thus has four times the rotation frequency and thus 4 times the mass of an electron.  The down quark, with two poles, doubles the acceleration yet again, thus giving 8 times the mass of an electron.

It will be no surprise to any of you that this correlates to the known rest masses of the electron, up quark, and down quark:  .511MeV, 2.3MeV, and 4.8MeV.

I can hear you screaming to the rafters–enough with the crackpot numerology!  All right, I hear you–but I liked seeing this correlation anyway, no matter what you all think!

Agemoz