Posts Tagged ‘interference’

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 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

Unitary Rotation Vector Field Three Pole Solutions Exactly Mimic Quark Combinations

April 25, 2020

I apologize for overposting here–I’m definitely going to be overdoing it–but I just felt like I had one more result to post (UPDATE below).

Most three pole solutions just produce the infinite wave results that are not sustainable as a real representation of particles, I just see the infinite series of wave rings.  But I thought, what if I tried to duplicate the three quark up/down configurations?  I place three poles in a triangle, and gave them all the same energy.  Nope, infinite rings.  Next, gave one of the poles half the frequency like an up quark.  Nope, still infinite rings.  Now, give it an antipole rotation: voila!  a stable particle configuration:

three_pole_m2_4_m2

In fact, I tried all combinations of “up” particles and “down” particles, and guess what–only two produced particles, the anti-up, down, down and the up, anti-down,anti-down configuration!  Yow–that was exciting.

However, Feynman’s ghost is here, and he says: be skeptical.  This may just have a stupidly simple reason, not a physics breakthrough.  It could just simply be the fact that 1 + 1 – 2 = 0, and -1 -1 + 2 = 0.

{update}:  quark sets have extremely complicated interactions and I now doubt that this configuration directly represents them (for example, where is the mass of the gluons).  It might give a clue of internal details of a quark set, but there has to be more to it.

Something much more significant is showing up with these sim results–the hypothesis that a testable principle exists.  It is this:

Quantum interference is responsible for redirecting particles along wave interference peaks–and also for creating those particles.

It doesn’t matter that we are talking wave functions (probability distributions) rather than actual waves, the redirection still happens.

It’s becoming very clear from these sim results that at certain wave frequencies, the effect of quantum interference must control the motion of poles because in the unitary rotation vector field, every field location is single valued (only one possible rotation at each point).  As a result, the quantum interference redirection that occurs in the two-slit experiment can also cause poles to encircle each other in a stable pattern.  I’m about to set up an experiment to directly test this principle.

More pictures to come…

Agemoz

Unitary Rotation Field Simulator: More Results

April 25, 2020

I’ll try not to post here too often, but a whole ton of results are coming back from different experiment configurations using the Unitary Rotation Vector Field simulator.  One thing that became immediately obvious is that stable solutions are not going to come from most pole configurations–the spreading waves you saw on the previous post aren’t sustainable in a universe full of particles.  I was pretty suspicious of something not right when I could make the dipole disappear entirely (see previous post).

I discovered a whole new ball game when I set up opposite pole dipoles:

dipole_1

The wave pattern disappears as the poles cancel out.  The residual rotations shown occur because I have yet to apply the effect of the I dimension (the background state referred to in previous posts about the theory I’ve been working on).  Here is a picture of two such dipoles of different frequencies:

two_dipoles_1

There are wide space dipoles representing lower energy solutions:

dual_2pi_dipole

Note that I’m just barely scratching the surface of the properties of this amazing field.  I’m only using one of the rotation modes (there are three in the R3+I field of the theory), I don’t have the background state turned on yet, I am currently only studying 2D configurations, and I have not turned on any time dependent characteristics, in particular, how such particles will move.  There’s so much to do and to document!

Agemoz

Unitary Rotation Field Sim First Light

April 24, 2020

The unitary rotation vector field is a promising candidate for an underlying field that theoretically should produce solitons, quantum effects, and special relativity.  In order to see if the field really could work or is just snake oil, I wrote a simulator.  That has taken a while to get working, but now I’m starting to get results that have been truly fascinating.

I’ve posted a ton of stuff about this field in previous posts.  I’ll go over a summary:  E=hv is true for all particles, and has led to a realization that a precursor field underlying our existence would have to have one degree of freedom per field element.  In contrast, an electromagnetic field has at least two: vector direction and vector magnitude.  This precursor field must have vector direction, so I posited that existence must be based on a unitary magnitude rotation vector field.  Years of thinking have led to all kinds of insights, including that such a field has to obey special relativity–a conclusion significant enough that I wrote a paper on it.  As I worked with this field, I came to the conclusion that such a field would support formation of solitons.  I also discovered that such a field would produce quantum effects such as the two-slit experiment interference pattern.

I have found a vast gold-mine of interesting consequences resulting from such a field to the extent that I felt a deeper dive into writing a simulator was worth the trouble.  After a long period of time, I now have initial results, and the very first pictures that were output made me realize what a very unique animal the unitary rotation vector field is.  Usually when we see interference effects between two oscillating sources (or the wave interference pattern that emerges from a two slit experiment barrier, we see something like this:

interference_pattern

But when I set up two sources using the unitary rotation vector field, I was so surprised that I thought there was something wrong with the simulator.  But then I thought about it for a while and realized–a unitary rotation field is a very different critter than what we are used to when we study EM theory or quantum mechanics.

Here is a picture of two identical (same wavelength) particles separated by a substantial distance.  It should be really clear that between these two particles the interference of rotation waves disappears.  The two particles are effectively entangled, and in this vector field the waves interfere along the path between them.

two_particle_1

Removing one of the two particles instantly removes the interference and the stable path between them.

one_particle_1

Now this is where things get bizarre beyond belief:  add a *third* particle nearby in space, and the wave pattern of the first two completely *disappear*!!  Going to four or more particles, the wave pattern causes a single new entity to appear in the center.  This aint your Gramma’s EM field here!

three_particle_unrelated_1

four_particle_same_1

five_particle_1

I will stop here, but I haven’t even begun–this is a 5D sim, I’m just testing 2D configurations to test it.  I am just capturing a single slice, but 3D configurations will be fascinating to uncover.  And–we are talking static configurations–wait until you see how these things move!

You may be completely skeptical that any of this connects with reality, or passes that ultimate test of new physics, that it predicts something new.  However, I am fascinated by the potential of this new tool, the unitary rotation vector field simulator, to lead to new insights about the theory I’ve worked on for so long.

Agemoz

Determining Subatomic Particle Characteristics from its Quantum Interference

July 18, 2019

Edit update 190719: Addendum added see below–another possible experiment

Every subatomic fermion (non exchange particle such as an electron) has a specific mass and hence wavelength, and thus will produce quantum interference with another particle of the same type or with itself.  This quantum interference will cause particle motion to be redirected, for example to specific locations (interference pattern) on a target detector in the two slit experiment.  It seems logical that studying the quantum interference effects of a particle will lead to insights about the particle structure.

In the previous post, I showed how the quantum interference pattern could be used to make a guess about particle internal structure.  It could form a soliton if the particle were a loop whose radius matched the wavelength of the particle.  But, if the particle radius is much smaller than its characteristic wavelength, this doesn’t work and the particle cannot be constructed using quantum interference.  I showed how a ring structure could produce the tiny point collision signature but still produce waves with the particle’s characteristic wavelength.  If we were able to determine if quantum interference forms electron structure, we could answer the size and topology question for once and for all.

But there’s more we can get from quantum interference.  If an electron is truly infinitesimally small, much smaller than the electron characteristic wavelength, we will have no way to determine internal structure by experimental observation.  But we can use its quantum interference pattern, whose characteristic wavelength scale is much much larger, to indirectly figure some things out.

For example, one great question to ask is whether the electron is a monopole oscillating or twisting in place– or consists of two nodes, a positive and a negative node spinning in a dipole orbit.  As far as I know, there is no experimental or theoretical work that determines which is reality for any subatomic particle.  There is no possible way to distinguish these two cases directly if the electron is infinitely small, which is the current physicist consensus.  But these two cases will have different characteristic wave patterns!  The monopole case will produce waves as concentric circles about the center.  The dipole will produce a spiral and will have a radiating peak and zero path.

monopole_down

monopole oscillates in place

monopole_up

monopole oscillates in place

monopole_pattern

monopoles produce a concentric circle pattern

dipole

dipole structure in orbit

interference_well

dipole spiral interference pattern

Admittedly, conducting an experiment that observes quantum interference in this distance range will be problematic at best.  But there’s one more important difference between the patterns generated by monopoles and dipoles that should help:  in a monopole particle, the phase of waves emitted both toward and away from the particle will be the same–but the phase of of spiral waves will be different by Pi/2 (90 degrees).

This characteristic wavelength should be in reach of (very) sophisticated observation apparatus–the electron wavelength, called the deBroglie wavelength, is 1.22 e^-9 meters.   The wavelength of visible light is in the range of 400 to 700 e^-9 meters, but energetic X-rays fall into range of this characteristic wavelength. If we could match the characteristic wavelength with an X-ray emitter (using electron-positron annhiliation, perhaps?), we would see observable interference that would either be the same or different on the leading and trailing particle wave paths, leading to either a monopole or dipole determination.  If such an experiment could be made practical, we should be able to get a significant clue of the internal electron structure even if the electron is infinitesimally tiny!

Do you see why I think quantum interference could be as powerful a measuring tool for science as, perhaps, the LIGO experiment?

Agemoz

Edit Addendum:  It occurred to me that there might be a better way to detect whether electrons have a monopole or dipole structure using a diffraction grating.  Silicon processes for fabricating computer chips are at 7 nanometers–the width of 6 or 7 electron wavelengths, so we are within reach of fabricating an experimental setup for electron emitters.  When computing the expected interference pattern in a two-slit experiment, Huygen’s principle is used.   This principle conforms to the concentric circle pattern that comes from a monopole.  Unfortunately, the current typical two-slit experiment has the barrier device (with two slits) oriented perpendicular to the emitted electron’s path and will not be able to determine which interference pattern is present. The dipole structure will give the same answer as the monopole case, because the wave pattern is sampled by the two-slit apparatus at the same phase point for either of the slits.

However, if the two-slit apparatus is tilted from the normal to the electron trajectory, you will have one of the slits slightly time and space delayed from the other, and now the resulting interference pattern will be dependent on the phase shift that occurs when you encircle the particle.  In other words, the spiral will be distinguishable from the concentric structure, and this experimental setup should point to either the monopole or dipole structure.

Inferring Subatomic Particle Structure From their Quantum Interference Patterns

July 13, 2019

In the previous post, I showed a proven theorem where classical Newtonian particles composed of instantaneous phase waves must observe special relativity.  If we assume the converse is true, it becomes worthwhile to deconstruct subatomic particles, which obey the principles of special relativity, as some construction of instantaneous phase waves.

Fortunately, quantum experiments such as the two-slit experiment and the Aspect experiment already confirms this principle:  there is good evidence there are instantaneous phase waves in particles because of the experimentally observed noncausal decoherence of entangled particles.  In addition, the two-slit experiment also shows that this interference is noncausal–you can cover one of the slits in the time it takes for a particle to travel through slits to a target detector, and instantaneously alter the possible particle detection sites.  Assuming that particles are formed by nothing other than waves has significant justification, both due to experimental observation and because such particles must obey special relativity according to the theorem described in my paper (see previous posts).

So–if we assume that particles form only from composite collections of waves, can we infer from the experimentally observed quantum interference patterns what the subatomic particles must look like mathematically?

There’s a lot of reasons we might be tempted to describe electrons with a Compton radius size, but any serious physicist won’t believe such claims, here’s why.  Subatomic particles are most often measured and examined in collision experiments.  The actual collision can’t be observed in most cases, but the resulting particle trajectories and masses can be, and allows us to determine things like size, internal composition, and angular momentum of the colliding particles.  One nice way to determine internal composition is to measure elasticity.  If you hit a billiard cue ball against another billiard ball, it might bounce right back at you, whereas if you throw a water balloon at another water balloon, the whole mess of water and balloon fragments will head more or less in the direction of your throw.  In other words, we can gain a lot of information about the inelasticity of a particle by the angular distribution of the post-collision particles.  All experiments show that electrons are perfectly elastic and are measurably infinitely tiny.  Hard as a billiard ball and too small to measure any diameter.

Here’s the problem–if you test the hypothesis that particles can form group wave constructs affected by quantum interference effects, we can draw conclusions based on knowing that the particles must be composed of instantaneous phase waves.  These waves don’t have to lie in a plane–for example, waves that lie on a twisting plane obey the same Fourier composition rules as planar waves.  I hypothesized in the previous several posts that waves form a couple of opposing delta functions that follow the peaks of the self-generated quantum interference wave pattern.  We already know from the two-slit experiment that quantum interference will redirect a particle path onto the peaks of the quantum interference that results from passing the waves through two slits.  It is thus very reasonable to assume that the right setup of quantum interference would create a circular loop, and I show that in the previous two posts.

However, this wont work if the two poles of our particle are infinitesimally spaced, that is if the particle has no significant size such as a Compton radius.  The poles are too close to be able to fall into the quantum interference peak locations that guide them into a loop ring!

interference_path_size

The only way–and it seems like a tenable proposition–is to say that the electron is not an infinitesimal point, but rather, a ring whose axial diameter is infinitely small.  Now the collision cross-section is the same as the point particle and you should get the same experimentally observed angular distribution of post-collistion particles–provided that the ring does not collapse–that it is totally inelastic.  I proposed this to an experienced particle physicist, but he said that’s not possible–there should be observable characteristics of a ring that are different than for a point particle.  I tried to argue that there’s a better argument for a ring than a point, because a ring has a definite angular moment (electrons have an experimentally measurable angular moment) but a point as defined as such does not.  I see a strong case for my proposition from the quantum interference soliton point of view, the angular moment, the Planck’s constant uncertainty relation (which says that something smaller than the Compton radius cannot meet the position-momentum Heisenberg uncertainty relation), and many others.  As you can imagine, I didn’t get very far–the response was NO, subatomic particles are measurably infinitesimal points!  And that’s all he would discuss.

collision_elasticity

Regardless–it appears clear to me that examining the experimentally observed quantum interference pattern of a particle should tell us new information about what forms the particle.  Is quantum interference responsible for particle structure?  If it is, the particle has to be a lot bigger than an infinitesimal point, yet have the collision signature of a point.  The only answer I see is the ring hypothesis with an infinitesimal axial radius.  Otherwise, I will have to conclude that quantum interference must be refuted as a candidate for forming solitons, and hence, subatomic particles, from waves.

Agemoz

Noncausal Characteristics of Quantum Interference Solitons

July 6, 2019

In physics I fully understand the need to filter out the crackpots and their onslaught of verbiage, whether wrong, vague, incomplete, or meaningless.  Real science is built on a very large collection of proven concepts–if any component is wrong but makes it into the collection, trust in the system as a whole is damaged.  If you look at Arxiv.com, there’s some junk that somehow got in there, and that means you need some system of qualifying what you see so you can trust what you use in your own work.  To avoid this, new papers submitted to journals always require verification by qualified reviewers.

The problem I am having is that I tried very hard not to be a crackpot, I think i proved something important, wrote a paper that got good qualified pre-reviews, and submitted 5 times and got 5 rejections.  Nobody looked at the proof and said I did something wrong, and nobody showed me why my conclusion was wrong.  Two of the journals were probably not the right target for the paper (this), but the other three did not see value in what I did.  The trouble is–I still think the idea is important, and that the proof is valid (confirmed by the pre-reviews).

Basically, in the paper, I proved that if a classical Newtonian particle is formed by a Fourier composition of a specific class of waves, the particle must obey the principles of special relativity.  The class of waves is simple–a phase change across any wave component is noncausal, that is, instantaneous across the length of the wave, but the rate of change of that phase is causal, or limited to some maximum change per unit of time such as the speed of light.

To me, this is incredibly important because it suggests the converse–if something obeys the principles of special relativity, it must *only* be composed of instantaneous phase waves.  I haven’t proven the converse–working on it–but if this is true, then this opens a big door into what causes the existence of subatomic particles.  A logical analysis of the two-slit experiment and the entangled particle decoherence behavior comes from the paper’s derivation (discussed in previous posts).  It also shows how a soliton (stable construct) could emerge due to quantum interference (see the last two posts).  And now, it shows specifically how the waves have to exist in the first place–very specifically showing what oscillations form the waves and where causality comes from.  From this, I see how the concepts of space and time might emerge out of something like the Big Bang.

You see, if a delta function of some sort is present in 3D space, and it is composed of these instantaneous phase waves, you *cannot* see the delta function do this:

single_spiral

The waves are instantaneous!  Here you see variations in space (and time, if you were to make a movie of the particle).  But that’s not possible with one delta function–it does not oscillate.  Oh, ok, no problem, handwave it and make it oscillate from a + to – peak and back again.  You *still* would not see this first figure–the wave phases are instantaneous, but this picture has variations in space and time.  Even if you put two of these delta functions near each other, one that is Pi/2 out of phase with the other, you would see something like this, where the two delta functions oscillate up and down out of phase with each other (this shows the Pi/4 halfway point):double_deltaThere are no waves here, because the sum of the delta functions can never produce anything but a plane, no matter how fast they oscillate in time.  I realized that now I think I know why electrons are not deBroglie circular waves with a Compton radius size–they have to be infinitely small.  The waves shown in the first figure have to result from a non-causal sum of a rotating and infinitesimally spaced, oscillating pair (or more) of delta functions.  Space and time for a particle emerge in a non-causal way from the orbiting pair of oscillating delta functions to produce the spiral waves shown in the first figure.  Only then could you see non-causal spiral waves emerge.  There’s other work I’ve done that shows that the delta functions must reflect some sort of twisting vector field in R3 + I  (NOT an EM field vector, those are photons).  Along the same lines, I’m sure you’ve seen the recent experimental observation of twist momentum found in photons.  Can you see why I see so much exciting work emerging from the simple theorem proof I describe in the paper?  Frustrating not to be able to publish it–I think I have something there, but can’t convince anybody else of it!  And until someone else sees the validity of what I’ve done, there’s no science here.

Auuggh!

Agemoz

 

Quantum Interference Defines a Soliton

June 18, 2019

In my last post, I described a quantum interpretation based on group waves with an instantaneous wave phase property, and showed how it derives a constant speed regardless of an observer’s frame of reference, setting the stage for special relativity.  I also showed how it would resolve the EPR (Einstein-Podolsky-Rosen) paradox for entangled particles in the Aspect experiment cleanly without adding some unknown force.  This is a flaw with the Bohm interpretation, among others, since it means that work is done and energy expended, causing a conservation of energy violation.  We do not need to believe in multiple parallel universes (Everett interpretation) or try unsuccessfully to create a logically consistent causality using the Copenhagen interpretation.

I then showed how a instantaneous phase group wave particle could self-interfere in the two-slit experiment to logically explain the target interference pattern distribution.  In this explanation, I show the very nature of the group wave will cause particle displacement due to the summation of interfering wave components.  No pilot wave guiding, with its implied force and consequent work and energy expended, is needed.

I suddenly realized that the group wave quantum interpretation provides a possible approach for creating a soliton–a particle could form in a system based on this quantum interpretation.

For over a century, theoretical researchers have guessed that the particle zoo (the list of subatomic particles that make up protons, atoms, exchange forces, and so on) could form from a continuous field (lattices, i.e., discrete fields, have been ruled out at this time both experimentally and theoretically).  DeBroglie was one of the earliest well known scientists that worked with this idea, but Compton and others also came up with proposals.  Early efforts assumed that solitons might form from an electromagnetic field via some selected arrangement of charge distribution, but EM fields and particles have the central force property F = c_0 q_1 q_2/(r^2), and by Maxwell’s field equations behave linearly, so basing particle existence on an EM field was disproved–particles would dissipate.  If there is a field underlying formation of particles, it cannot be electromagnetic, but rather an underlying “precursor” field from which EM fields could emerge.  Dirac’s work led the way to the modern quantum field theory, which further ruled out an EM field creating solitons–EM fields consist entirely of collections of real and virtual photons that travel in straight lines (ignoring space curvature from general relativity at quantum scales).

But instantaneous phase group wave theory can form solitons.  No matter what quantum interpretation you believe in, you have to face the fact that a single particle going through two slits is going to experience redirection when you open one of the slits.  The fact that this redirection happens means that at some scale, a particle will curve in on its path–it must follow the interference pattern.  I have found a variety of ways that a moving interference pattern will circulate or follow more complex loop variations.  For the same reason that the two-slit setup forms an interference patterned domain of existence for a particle, the appropriate pair (or more) of particles will self interfere to form stable loops.  Follow the interference and you will describe a variety of possible particle paths.

Does this reflect reality–dunno, but work is ongoing.  I’m coming up with a mathematical toolset that will describe various interference path constructions.  I will follow the yellow brick road and see where it leads…interference_path_soliton

Agemoz

Precursor Field Connection to Quantum Field Theory

November 8, 2016

I’ve done some pretty intense thinking about the precursor field that enables quantized particles to exist (see prior post for a summary of this thought process) via unitary field twists that tend to a background state direction. This field would have to have two types of connections that act like forces in conventional physics: a restoring force to the background direction, and a connecting force to neighborhood field elements. The first force is pretty simple to describe mathematically, although some questions remain about metastability and other issues that I’ll mention in a later post. The second force is the important one. My previous post described several properties for this connection, such as the requirement that the field connection can only affect immediate neighborhood field elements.

The subject that really got me thinking was specifically how one field element influences others. As I mentioned, the effect can’t pass through neighboring elements. It can’t be a physical connection, what I mean by that is you can’t model the connection with some sort of rubber band, otherwise twists could not be possible since twists require a field discontinuity along the twist axis. That means the connection has to act via a form of momentum transfer. An important basis for a field twist has to consist of an element rotation, since no magnitudes exist for field elements (this comes from E=hv quantization, see previous few posts). But just how would this rotation, or change in rotation speed, affect neighboring elements? Would it affect a region or neighborhood, or only one other element? And by how much–would the propagation axis get more of the rotation energy, if so, how much energy do other non-axial regions get, and if there are multiple twists, what is the combined effect? How do you ensure that twist energy is conserved? You can see that trying to describe the second force precisely opens up a huge can of worms

To conserve twist energy so the twist doesn’t dissipate or somehow get amplified in R3, I thought the only obvious possibility is that an element rotation or change of rotation speed would only affect one field element in the direction of propagation. But I realized that if this field is going to underlie the particle/field interactions described by quantum mechanics and quantum field theory, the energy of the twist has to spread to many adjacent field elements in order to describe, for example, quantum interference. I really struggled after realizing that–how is twist conservation going to be enforced if there is a distributed element rotation impact.

Then I had what might be called (chutzpah trigger warning coming 🙂 a breakthrough. I don’t have to figure that out. It’s already described in quantum theory by path integrals–the summation of all possible paths, most of which will cancel out. Quantum Field theory describes how particles interact with an EM field, for example, via the summation of all possible virtual and real particle paths via exchange bosons, for instance, photons. Since quantum field theory describes every interaction as a sum of all possible exchange bosons, and does it while conserving various interaction properties, all this stuff I’m working on could perhaps be simply described as replacing both real and virtual particles of quantum theory with field twists, partial or complete, that tend to rotate to the I dimension direction in R3 + I space (the same space described with the quantum oscillator model) of my twist theory hypothesis.

I now have to continue to process and think about this revelation–can all this thinking I’ve been doing be reduced to nothing more than a different way to think about the particles of quantum field theory? Do I add any value to quantum field theory by looking at it this way? Is there even remotely a possibility of coming up with an experiment to verify this idea?

Agemoz