Archive for May, 2020

Comparison of Quantum Field Theory and the Unitary Rotation Vector Field Theory

May 30, 2020

UPDATED with more details on the unitary rotation vector representation of the test interaction (see section UPDATE below)

The latest simulations have shown some wonderfully interesting results. The last post showed how the Unitary Rotation Vector Field theory demonstrates particles that can both repel and attract due to quantum interference effects that relocate the stability region of particles. You can read about these results in previous posts, here is a schematic diagram of what happens, along with some sim output pictures demonstrating the principle:

stability_region

I never intended to create a theory that competes with quantum field theory, but the principle of charge attraction and repulsion traditionally is derived directly from quantum field theory methods. So, it seems well worth the effort to compare the two approaches, and what I hope to gain by analyzing the properties of the unitary rotation vector field. While I have run unitary rotation vector field simulations of many particle types and interactions, I think it will be illustrative to compare how each theory handles the simplest interaction of a pair of electrons (charge repulsion).

Quantum field theory solves interactions like these by using LaGrangian mechanics, that is, minimizing the action scalar. Doing a path integral of the LaGrangian over all paths, and setting the the derivative of the action at all points over time to zero yields a motion equation for the particles in the system. This computation will find the path of minimum action and thus will correctly represent reality. More specifically, the interaction of the two electrons is mediated by virtual photons–particles that do not reside on the surface of valid position/momentum solutions in space and time (off mass shell). By prepending a creation operator to the photon wave equation and appending an annihilation operator after it, quantum field theory creates a solution where the time evolution of the electrons go in opposite directions (repulsion).

On the other hand, the unitary rotation vector field (nearly identical to a Pauli spin matrix representation) gets repulsion and attraction in a different way. Both theories do sums of wave paths to find regions of quantum interference, but the wave equation is different. In quantum field theory, the wave equation is the Hamiltonian–the sum of energies such as kinetic energy and the voltage potential in an electromagnetic field. The creation/annihilation operators are probability functions for emergence of virtual particles. The integral is computed over sufficient time so that an operator isn’t left stranded (virtual particles wont conserve momentum in that case).

The unitary rotation vector field is different–it is single valued with only one rotation possible at any given point, and this constrains where particles can exist (the stability region) because the particle phase and the wave phase must match (see the above schematic).

The wave equations in quantum field theory have wave solutions that propagate over time (for example, the propagator in the La Grange equation of action). Solutions depend on virtual particles that don’t obey classical physics. Quantum field theory can’t work without them because on-mass-shell particles will induce the momentum paradox described in the previous post. Nothing propagates in the unitary rotation vector field–each point just rotates, so conservation of momentum works without inducing the paradox.

Probably the biggest reason I pursue the unitary rotation vector field, rather than just sticking with the established science of quantum field theory? The rotation vector field seems to give another possible view of the underlying mechanics of particle interactions that might yield answers not covered by quantum field theory. The most significant possibility comes from how it postulates a formation of elementary particles from quantum interference in a field. There are other reasons, such as the theory doesn’t require renormalization methods, it doesn’t depend on off-mass-shell particles to work, and doesn’t have a probabilistic dependence on when virtual particles form.

Since quantum field computations work, it’s arguable my efforts are a waste of time (and certainly could be wrong, or not even wrong). But my curiosity is here, and so for now I will continue.

Agemoz

UPDATE:  I need to clarify the Unitary Rotation Vector Field representation of the particles involved so you can see exactly how I set up the simulation.  There may be other schemes that work, but this is the approach I used in my simulations.

The unitary rotation vector field is continuous and only rotates a unitary vector (like the Pauli spin matrix).  It can point in any of the three real dimensions in R3 or in one imaginary direction (the background state of the theory).  This is the same vector space as the continuous quantum oscillator field, except that there is no variation in magnitude and you cannot have a zero length rotation vector.

Being single valued, a rotation cannot pass thru from one location to another without affecting each location in the path.  As a result, particles must have the same phase as the sum of wave rotations (that is, quantum interference computed as a path integral) at each particle’s location, this is called the particle’s stability region, shown in black on my simulation images.  A particle cannot exist anywhere except in a stability region, otherwise the location would have to simultaneously have two different rotations. Particles are forced to move when the stability region moves–a well tested example is quantum interference resulting from a single particle passing through two slits.

Each field location can be represented by a set of three rotation values–one straightforward basis is a rotation set that resides in the plane that includes the I dimension and the X direction, a rotation that includes both the X and Y directions, and finally one rotation that includes both the X and Z directions.  My simulation uses this basis.  All rotations are modulo 2*Pi (the simulation values go from -Pi to +Pi).

A photon in this theory is modelled with a single quantized vector rotation from the +I direction thru -I and then continues to +I (see the image figure below).  There is a lowest energy state at +I and -I, so once the rotation does one rotation, it stops. The photon also has a translation along some real dimension axis.

photon_carries_momentum

In the interaction of a photon and electron shown in the above simulation pictures, the photon induces either a positive or negative rotation offset to the receiving electron, which causes the electron stability region (via quantum interference) to displace either above or below (attraction or repulsion respectively).  The photon must be able to carry a positive or negative momentum.  You can see that the rotation must lie in the plane that includes both the +I and the translation direction vector (otherwise you will not have photon polarization using any other rotation scheme).  Note that there are two possible rotation directions–either rotation begins moving toward the direction of travel, or away from it, corresponding to the two possible rotation offset directions intercepted by the electron.

The really interesting thing about this configuration is that the photon becomes a momentum carrier, but intrinsically does not have any actual momentum due to its translation.  The source particle emitted momentum is carried by the photon’s rotation but the photon has no momentum of its own (consistent with the fact that photons are massless particles).  This is what allows photons to pass along either negative or positive momentum without inducing the momentum paradox.  That is, shooting a massive particle at a destination particle cannot ever cause attraction, but photons can.

This seems to be a much better scheme for how photons carry electrostatic force than the virtual particle scheme used in quantum field theory.  Virtual particles are just assumed to not obey momentum/position conservation from creation to annihilation, which means I can’t simulate it.  I can only define the interaction as a black box.  It computationally works, (there’s no way ever that I would say quantum field theory is wrong!!!)  but my goal is that the unitary rotation vector approach could lead to a deeper understanding of particle interactions.

Agemoz

Unitary Rotation Vector Field Mimics Electron-Photon Interaction

May 20, 2020

I set up a quantum interference unitary rotation vector field sim with a very basic idealized representation of a two pole “electron” and a much lower frequency one pole “photon” along the z-axis, and here is what I found:

a: The “photon” wave (photon meaning the sim model of a photon in this post) makes the two pole electron unstable at the z = 0 axis position. Instead, the stability region moves along the z-axis depending on the phase of the photon pole. As a result, the quantum interference pattern from all three poles appears to force the electron to translationally move along the axis of the photon z displacement, which matches the expected electron-photon interaction behavior.

b: Depending on the phase of the incoming one-pole photon, I found that the stability region for the two-pole electron can either be below (away from) OR above (toward the photon). Could we at last have an explanation for why electrostatic fields emitted from a source can either repel or attract?

There is a momentum paradox in electrodynamics–if photons have momentum toward an electron, how can momentum be conserved if the electron ends up (due to charge attraction) with momentum in the opposite direction (toward the photon)? Quantum field theory computes that the field itself absorbs the momentum difference (and yes, mathematically that works) but intuitively I rebel at that analysis. The unitary rotation vector field appears to be providing a very elegant solution–quantum interference directs where the electron stability region has to go via wave interference, and in some phase cases it exists toward the photon rather than away from it.

c: It doesn’t matter where you put the photon. I get the same results regardless of the photon offset in the x-y plane (although as mentioned, the z offset causes the electron stability region to move along the z axis).

d: It doesn’t matter what frequency is used for the photon, although the stability region displacement above or below the electron initial position will vary linearly as 1/photon frequency. Higher frequencies cause the photon phase change and hence the change in z displacement to occur at a faster rate, lending credence to the idea that higher momentum photons will induce a larger momentum change in the electron.

e: The only thing the sim seems to get wrong is the absorption of the photon, which should disappear after encountering the two-pole electron. This will require more investigation.

So, in summary, at least on this first pass of testing, the hypothesis that quantum interference in a unitary rotation vector field is responsible for particle formation and particle interactions appears to behave correctly for the electron/photon interaction test.

That by no means is saying that my hypothesized unitary rotation vector field represents reality (if a real physicist were reading about my efforts, he/she probably would wish my efforts would die in a fire if I said something like that) but it looks pretty promising right now. In time and with more work, who knows where this will go–but the real test will be for some qualified researcher to confirm what I am seeing. Until that happens, you should assume that this is unreviewed work (by one author, the kiss-of-death for a research paper) and take it with a bucket of salt…

Agemoz

Here is a picture with the photon in the center, and the z plane is at zero (note this picture cannot be stable, the outside crosses are not in zero delta phase regions)

twopole_z_1_6_phase_unstable

Looking at the same image, the region of stability has relocated closer to the photon (representing electrostatic attraction).

twopole_z_1_6_phase_stable

The region of stability displacement linearly varies as the phase shift induced by the photon, notice the region for a smaller phase shift has not relocated as far from the original electron position:

twopole_z_0_4_phase_stable

Only Two, Three, or Four Poles Possible in a Quantum Interference Unitary Rotation Vector Field

May 18, 2020

I’ve done extensive work trying to find all possible stable particle configurations using quantum interference, and only three combinations are showing definite stability; solutions exist for two and three poles.  There is one valid set of four poles that statically would be stable but only in three dimensions (tetrahedral shape) but I see problems that indicate such a solution wouldn’t work dynamically (have to really watch out for confirmation bias because so far there is correlation to the real-life particle set) .  It’s geometrically very clear that no 5 pole or higher can exist as a stable solution.

[UPDATE] More results I forgot to mention: A consequence of the 4 pole limit is that a twist ring cannot work. I approximated a twist ring with an 8-pole solution which shows no stability, and geometrically it’s easy to see why (an infinite overlap of wave phase points on every point of the ring). A ring will generate waves from all points about the ring, and there is no possible way this can exist in the single-value unitary rotation vector field. So, the twist ring, long promoted on this site as a valid field solution, bites the dust, at least for the unitary rotation vector field case. This is really interesting because it confirms the experimentally observed infinitely small point concept of current physics, and also seems to validate the Bohm interpretation of an infinitely small core with a non-causal guiding wave for particles. Here’s a picture–note the little crosses are the pole locations with stepwise increments in phase. You can tell that this is unstable because the phase delta between the sum of waves plus the particle phase must be zero and would show here as a black region–but instead many poles do not and cannot reside in a zero phase region. That is indicating that the particle phase and the wave phase are different, an impossibility in this single-valued unitary rotation vector field.

eightpole_unstable

Also, (face-palm moment as I jumped too fast to conclusions) there actually are 5 pole and greater solutions, provided all the poles lie in a line. However, another constraint is emerging where this type of solution may not be stable except in the static case. Working on that one…

Here are pictures for two and three poles:

twopole_updated
threepole_stable_221
threepole_stable_112

I’m now working on a sim where a unitary rotation vector field “photon” approaches and is captured by a field “electron”.  Results shortly–should be interesting and a fairly definitive test for whether the unitary rotation vector field can really model reality.

Agemoz

Unitary Rotation Sim Quark Combination Results

May 9, 2020

The latest sims show yet another intriguing connection between three pole simulations and experimentally observed quark combinations.  A couple of posts ago, I wrote a surprising result that only certain three pole configurations were stable.  Those combinations happen to match the valid quark combinations for protons and neutrons, but all other combinations were clearly unstable.  At first I thought, aha, a breakthrough, but after thinking about it I thought quark interactions are extremely complex and such a simple explanation shown by the sim couldn’t be the explanation for valid quark combinations.

Nevertheless, I have continued to explore three pole configurations and came up with another consistency (yes, this is confirmation bias at work here!).  There are two valid three quark configurations, u-u-d (proton) and d-d-u (neutron).  However, only one of them, the proton is stable–a free neutron will decay into a proton, an electron, and a neutrino after a while unless accompanied by a proton in an atomic nucleus.

Curiously, the three pole simulations are showing a similar disparity.  The geometry of the two long wavelengths plus one 1/2x short wavelength is easy to see, you can set it up as an isosceles  triangle.  Here is the sim stability test for that case:

threepole_224_stability

But the opposite case using one long wavelength and two 1/2 short wavelengths cannot produce a valid configuration, there is no way to lay this out such that wave phases match (try to lay out a triangle with two short sticks and one 2X longer stick, you can’t–they form a line).  I have tried a number of sim configurations to get a valid configuration, and haven’t found one yet–just thinking about the geometry seems to show there cannot be one.  Trying to line up the poles in any spaced combination gives unstable results:

threepole_442_stability

What if we set up a known stable quark configuration (a neutron and a proton, three up quarks and three down quarks?)  This requires 6 poles, but I haven’t found any configuration that works, at least in the 2D plane.  You have to set up the poles so all 6 locations have identical phase matches for three up wavelengths and three down wavelengths (due to the unitary rotation field requirement, every location must be single valued, that is, have identical wave phase rotation values from every pole).  Locating the poles so the long wave poles (up particles) are points on an equilateral triangle, and placing the short wave poles (down particles) on a nested upside-down triangle looked promising but doesn’t work.  There are pairs going from the up poles to the opposite down poles that have a phase change of sqrt(3)/2, and phases won’t match.  If there is a solution, maybe in 3D, I haven’t figured it out yet.  And, it’s quite likely that stability in this configuration (an ionized iosotope of hydrogen with one neutron, technically ionized deuterium) conferred due to a particle property not modeled in the sim.

Or I’m certainly open to the possibility that the sim doesn’t model reality at all.  It is intriguing, though, how many real-life quark properties are showing up in the sim.  I’ll continue to investigate.

Agemoz

Quantum Interference in a Unitary Rotation Vector Field Simulation Induces Circular Motion

May 5, 2020

UPDATE: While the validity of the claim (quantum interference will induce stable particle formation in a unitary rotation vector field) is still holding up, the math used to compute the original image was wrong, and hence the image below needs to be updated.  I’ve changed the rotation color mapping to make it easier to see the stable trajectory locations.  The phase matching points (delta phase from all sources that sum to zero) now are shown as black rather than yellow, and I now have the sim actually draw the particle points (little white crosses) rather than me post drawing dots in the wrong place on the original image.  The trouble with doing research is ensuring that everything is executed without mistakes, and that takes a lot of due diligence.  Nevertheless, even with the mistakes corrected and a healthy dose of skepticism, I still am finding that the conclusion (stable particle formation in a unitary rotation field) is correct.  Updated image:

twopole_updated

ORIGINAL POST:  Another step forward for the premise that quantum interference is responsible for the creation of particles.  The same principle that redirects particles in the two-slit experiment is shown here to induce circular motion of quantum interfering poles, provided you are willing to assume that our existence arises from a single-valued unitary rotation vector field–a field that can only assume a rotation angle but does not have any variation in magnitude.

Here is a sample output of the simulator that shows two vertically spaced, oppositely rotated poles spaced at the right distance that the propagated rotation waves output from one pole match the phase of a second pole.  In the unitary rotation field, the wave rotation from one pole must match the rotation of the second pole because the field is single valued, only one possible rotation is possible at any given point.  You can see the interference pattern from two poles spaced such the phase of one particle matches the phase of the propagated wave from the other.  Since the field is single-valued, the poles must follow the circular interference pattern produced by the simulator.  Note that the yellow region shows wave phases where rotations would not match, no particle can reside here.

The poles are clearly bounded to travel in a circular path within the regions matching the pole phase (either brown or green).  Note that quantum interference far from the actual pole positions do not affect the motion of the actual pole positions I have marked as oppositely colored dots (they actually must be the same rotation and hence the same color) on the sim.  Based on a variety of sim results, I believe there are many valid solutions consisting of different pole configurations (see previous post for a three pole solution).

twopole_quantum_interferenceAgemoz