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    Quantum Hexodynamics
    By Johannes Koelman | November 1st 2010 08:15 PM | 11 comments | Print | E-mail | Track Comments
    About Johannes

    I am a Dutchman, currently living in India. Following a PhD in theoretical physics (spin-polarized quantum systems*) I entered a Global Fortune

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    Special Guest Post From A Far Boundary Of Our Universe

    By Richard P. Flatman


    "I call our world Flatland, not because we call it so, but to make its nature clearer to you, my happy readers, who are privileged to live in Space."

    This is how my great-grandfather, Albert Square, started his memoirs. Memoirs he wrote in solitary confinement. Years later he died, still imprisoned and alone, and unaware that his ideas slowly but steadily started to change the views and imagination, not only of his fellow Flatlanders, but also of you Spacelanders.* 
     
    How time has progressed! My great-grandfather is now regarded a science martyr and a hero. A visionary thinker who has shown us Flatlanders the route towards scientific enlightenment. His legacy triggered an avalanche of scientific growth, and an unstoppable progression of insights. 

    It is the latest of these insights that I would like to share with you: the remarkable discovery of the strange inner workings of our microscopic world. I, Richard Flatman, have played no minor part in this development. How proud my great-grandfather would have been!


    Cover of my great-grandfather's memoirs (6th Spaceland Edition)


    Zooming in on Flatland

    Our universe is two dimensional. A planar sheet that stretches endlessly. However, when thinking about Flatland, you should not imagine an infinite structureless sheet, but rather an infinite grid of microscopically small cells. These cells have a sixfold symmetry and nicely fit together in a hexagonal pattern.** Elementary particles, aptly called hexons, populate this hexagonal grid. All objects, all matter, our own bodies, everything we Flatlanders see, is build from hexons. So if you understand the interactions and behaviors of hexons, you understand the physical reality of Flatland.

    When hexons were discovered to be the elementary building block of matter, it was understood that clumps of matter move due to the hexons that constitute the clump jumping from cell to cell on the hexagonal grid. But how does this hopping dynamics work? How can we predict the movements of hexons? Years ago my investigations started with these questions. Little did I know what surprises I would encounter.


    Visualization of a small (eight hexon) lump of matter moving along the Flatland grid


    The strange behavior of caged Hexons

    I spent years fruitlessly investigating the behavior of hexons. Real progress came when I managed to control planar space at the level of individual cells. This allowed me to isolate and confine single hexons. My first successful experiment is depicted below. I call this set-up a hexon cage, but you Spacelanders might prefer the term hexon billiard. By blocking a few individual cells from the planar grid (the grey cells referred to as scatter centers) I created an area in which a single hexon can rattle around. The figures below depicts what I expected to happen: a hexon trapped forever in a cage formed by the scatter centers. The hexon would follow one of the various specific paths compatible with the shape of the cage. As the dynamics would be too fast to follow, I expected not to see the time-resolved dynamics, but rather the various hexon orbits as depicted.


    Two expected alternative orbits for a hexon rattling in a hexagonal trap (grey cells depict scatter cells that can not accommodate any hexons)


    Time average of the above rattling dynamics. For some reason only the hexagonal orbit shown on the left-hand side has ever been observed


    To my surprise I observed only one of the these predicted hexon orbits. No matter how hard I tried, I could not get any orbit different from the hexagon loop. This was puzzling. Things became even more puzzling when I realized I had forgotten about other orbits. I had overlooked the simple possibility of a hexon at rest anywhere in its cage. I never observed any such single cell 'orbit'.

    Was something wrong with the experiment? To find out, I started building alternative hexon cages. I immediately encountered further surprises. Against expectations, some of the cages built did not result in any trapped particles. Even more puzzling, I hit upon cages incapable of trapping particles, that become capable of doing so by blocking cells in the cage. This really puzzled me. If a container can not hold a certain object, how can the removal of some of the space in the container render it capable of holding that same object?


    A 'racetrack cage' incapable of holding a hexon (left), and the same cage with some inner cells removed holding a hexon (hexon orbit shown in green)

    Other experiments were even more puzzling. While I was sure at any time there was no more than one single hexon in the trap, in some cases I observed clearly separated orbits. What is happening here? Did I witness some form of hexon splitting?***


    A trap showing hexon orbit splitting. This pattern forms despite only one hexon being trapped.


    Shortest paths

    As I started contemplating these results, I remembered a recent theory from a fellow Flatlander. The theory was supposed to be an alternative description of the known laws of mechanics. It states that particles going from A to B always select the shortest path possible. It is a remarkable statement, and it seems to work for large scale objects. When applied to my microscopic experiments, the principle seemed capable of describing some of the orbits observed, in particular the orbits that originated in larger cages. Case in point is the trace shown below that could be described as the shortest path that hits all six scatter centers. Similarly, one could describe the hexagonal orbit observed in the first successful trapping experiment as the shortest path that hits all scatter centers forming the cage. Although it was not clear to me how the shortest path rule could be morphed to describe all observed traces including the one consisting of the double loop, I started to entertain the thought that maybe it all depends on looking at these matters from the right perspective. 


    Hexon orbit observed in a larger cage. The trajectory can be described as the shortest path that hits all scatter cells.
     
    Yet I didn't really like the minimum path theory. How would a particle know what lays ahead? And if it doesn't, how can it be able to decide at each step which one would lead to a shorter route? Shortest path selection can only happen if the particle would 'sniff out' the various possible paths. Somehow this idea struck an inner chord, and I tried to work out scenarios for hexons 'sniffing out' their environment.                


    Quantum Hexodynamics

    What if a hexon tries all possibilities and 'sniffs out' all neighboring cells, and in the next step all neighbors of these neighboring cells, etc? An avalanche of sniffing paths would result. A remarkable thought occurred to me. What if these path to some degree cancel each other, and thereby largely wipe out the avalanche resulting from the sniffing process? 

    For cancellation to occur, hexons must have associated with them a number that can be positive as well as negative. Let's assume this number, which I will refer to as the amplitude of the hexon, can take on only two values, +1 and -1. 

    So we have a grid of hexagonal cells, and each cell carries an amplitude. This amplitude can be +1 (a cell occupied by an hexon with positive amplitude), it can be -1 (a cell occupied by an hexon with negative amplitude), or it can be 0 (an empty cell). In discrete time steps the hexons jump from cell to cell and thereby carry amplitude across cells. 

    Which jumps happen? 

    All of them! At each time step each hexon sniffs out all seven possibilities by carrying it's amplitude to each of the six neighboring cells as well as to its own cell. When all hexons have carried their amplitudes in sevenfold fashion, for each cell the resulting amplitude is determined simply by adding all the amplitudes that have arrived at that cell.   

    I started drawing hexagonal grids and soon found myself busy experimenting with different amplitude configuration. A cell with a positive amplitude hexon I marked red, a negative amplitude hexon cell blue, and an empty (zero ampIitude) cell faint yellow. As before, the scatter cells used to trap the hexons I colored dark grey. When I started experimenting with different amplitude patterns, the configurations invariably resulted in runaway processes. In all the cases that I tried, the sniffing out led to avalanches that filled the grid with ever larger positive and negative amplitudes. Just as I was about to abandon this pointless 'sniffing idea', I realized that for stable patterns to result, empty (yellow) cells need to be surrounded by an equal number of red and blue cells. This simplified the trial and error process, and almost immediately I stumbled upon a stable pattern. A pattern not hampered by any runaway processes. This pattern is depicted below. Recognize it? Yes, it is the hexagonal trace observed in my first experiment. 


    Eureka! A stable path that results when allowing positive and negative amplitude hexons to follow all possible paths. The alternation between red and blue colors represent amplitude sign flipping.

    I immediately turned to the racetrack cage, and indeed discovered a stable amplitude pattern is only possible if the center cells contain scatter cells. I then turned to the geometry that resulted in the apparent 'hexon splitting'. I again had to experiment a bit with different hexon amplitude configurations. I soon found a stable configuration: the puzzling two-loop configuration. I knew I had struck gold. The enigmatic hexon dynamics had succumbed. Quantum Hexodynamics (QHD) was born.


    Stable hexon amplitude patterns for racetrack cages.

    The simple 'sum over all possibilities algorithm' not only delivers the right hexon paths, it also excludes those paths I initially expected but never observed. A case in point is provided not only by the racetrack cage, but by any of the 'hexon-at-rest' configuration. Each of these lead to a runaway process and don't form a stable configuration.


    A Quantum Can Of Worms

    It is now several years after the discovery of QHD. It seems the whole Flatland physics community has started working on QHD. Many are working on practical problems and are involved in the computation of stable hexon patterns for geometries of interest. Others are investigating the implications of QHD at a more fundamental level. My friend Werner is mostly intrigued by the sum over all possibilities approach preventing hexons to be localized in one cell.  Key issue is the fact that while the hexon orbits make sense, the occurrence of a hexon at a particular cell is much more enigmatic. QHD predicts that if one attempts to measure the specific location of a hexon, randomness enters the picture. In fact, any cell with +1 or -1 amplitude has equal probability of the hexon showing up, and upon measurement one of these will emerge at random as the cell containing the hexon. I refer to this measurement phenomenon as the 'collapse of the hexon orbit'. Albert, probably the most famous Flatland physicist of all times, abhors this aspect of QHD. He insists that "God doesn't play dice". 
       
    Yet, no matter if Albert's God likes it or nor, fact of the matter is: QHD works. Each and every of its predictions that has been put to a test has been confirmed. Yet some aspects of QHD, such as orbit-splitting configurations, are difficult to digest for us Flatlanders. QHD see,s to describe a world for which we can make successful predictions, yet we can not really understand. What is 'understanding' anyway? I prefer to be pragmatic on this issue. I think I can safely say that nobody 'understands' quantum hexodynamics. The advise I give to my fellow flatlanders therefore is: do not keep saying to yourself, if you can possibly avoid it, "But how can it be like that?" because you will get down the drain, into a blind alley from which nobody has yet escaped. Nobody knows how it can be like that.

    I just wonder: have you, Spaceland physicists, also landed on a QHD-like theory to describe your microscopic world? And if so, are you bothered about its philosophical implications?  


    -Richard P. Flatman-


    Notes

    * Memoirs published in Spaceland in 1884 under the title "Flatland: A Romance of Many Dimensions".
    ** It just came to my attention that two Spacelanders recently won a prestigious science prize for nothing more than mimicking our world in a Spaceland lab. Although my initial reaction was one of disappointment (I had assumed your higher dimensional science was well beyond our si ple world), I now realize this opens exiting possibilities for you Spacelanders to create your own versions of Flatland that may even evolve its own life forms!      
    *** Despite huge efforts that culminated in the building of the Large Hexon Collider (LHC), no one ever witnessed a hexon splitting up in more fundamental elementary particles.    

    Comments

    Surely you are joking, Mr. Flatman!

    Joking aside, what a nice little toy model to explain some key aspects of quantum physics. No complex numbers, no operators, no Hilbert spaces, no eigenvalues. Just a lattice billiard. Chapeau!

    vongehr
    An inspiring post again. I always thought a (quantum) cellular automaton is a very attractive way to think about many phenomena, be they in relativity or in quantum physics, or even in the realms of evolutionary theory and the theory of mind. However, there are two main problems: The first is that any such hidden variables model is incapable of reproducing quantum entanglement, which is the actual hall mark of quantum physics (all else, quantization and uncertainty, say, can be modeled by a hidden hot ether with topological quantizations, for example). You can try, and if you get your hexagons to show true entanglement (EPR style), you will be my all time hero! Secondly, the main problem with such models is not even quantum, but the mere fact of that you cannot get the gray hexagons in any other way but by having some god put them there. The green, red and yellow ones are fine, but try to get the gray ones made out of green and red ones, and the thing becomes much less attractive. Both problems are basically the same: we desire a much too localized dynamics. The world may be 2D quantum, but it must be a very distributed, non-local affair.
    Johannes Koelman
    "if you get your hexagons to show true entanglement (EPR style), you will be my all time hero!" Keep in mind the QHD model is a one-particle model. No doubt there are possibilities to extend it to multiple particle models, but I doubt that would lead to anything simple and attractive. ".. any such hidden variables model .." You may call QHD many things (a semi-classical model, a lattice Schrodinger model, etc.), but calling it a hidden variable theory is incorrect. There are no 'hidden variables' or 'pilot waves' anywhere in the model. QHD simply contains no variable other than the hexon amplitude (cell color). No difference here with 'true quantum mechanics'. "try to get the gray ones made out of green and red ones, and the thing becomes much less attractive" True, also in this respect QHD is not different from standard textbook QM (ever tried to create the potential well discussed in chapter three of your first QM textbook out of the trapped particles?). You may think of the gray cells as occupied by an ultra-heavy variant of the hexons (heavyons?), but I prefer to keep the model description strictly single-particle, and to think of the gray cells as 'god-given' excluded areas.
    vongehr
    "hidden variables" was the wrong expression - I should have formulated that better - I wanted to stress the deterministic underlying substrate with locally acting (nearest neighbors) rules. Cellular automata make me immediately think of the particles in the end being pseudo particles made from collective behavior of many underlying cells. Since you call your model a "one-particle model", you may be thinking of something else. The points I made are maybe only valid for my narrow interpretation of where cellular models are supposed to lead to (e.g. some such computation on a holographic screen maybe). In QM, the potential wall you refer to is acceptable as somehow be consisting of mutually self trapping (pseudo) particles, especially if attractive forces are given. The gray hexagons however, attractive forces and so on, making them emerge from an underlying cellular substrate with locally acting rules, that is what may be a problem in principle. The impossibility of getting entanglement from such a "real hidden substrate" may well be one and the same problem. Non-locality is the one aspect that seems to destroy all these nice looking comprehensible toy models.
    Hfarmer
    Cool article.   Do you think that having some blocked spaces in side some of your hexon traps could be due to some sort of 2D gravity like effect?  As if those blocked cells somehow attract hexons?
    Science advances as much by mistakes as by plans.
    Johannes Koelman
    An interesting thought, Hontas. I have to think a bit more about this. But don't read too much into this model. In essence it is nothing more than a rough discretization (in space and time) of a single-particle Schrodinger equation.
    Pachu
    How a step happen ? Its time related ? 
    Its synchronized (all cells do the step at the same time) ?
    Have you a computer simulation for this model ? (looks easy to make)
    The first gif shows several colors, how you model allow this behavoir ?

    Hope your answer not to be: go study QM  :-b
    Johannes Koelman
    "How a step happen ? Its time related ? Its synchronized (all cells do the step at the same time) ?" The steps are synchronized. And yes, this represents time progressing in finite portions. "Have you a computer simulation for this model ? (looks easy to make)" Yes, I have made a simple spreadsheet to experiment with this model. But one can easily do without. "The first gif shows several colors, how you model allow this behavoir ?" The first figure depicts a conceptual situation, that is not part of the model. Consider it an artist impression.
    rholley
    Didn’t Zenon Epipediges, quite a while ago, raise some interesting questions about paradoxes of motion in this sort of system?
    Robert H. Olley / Quondam Physics Department / University of Reading / England
    Amateur Astronomer
    I like this article because it tends to build up a physical system from the smallest components in ways that can be tested against mathematical consistency and physical data. Non-locality is not a part of the example because the picture has no field like a gravity source in one corner stretching the hexagons out of shape along the connecting diagonal. If Johannes had chosen to give a different example the non-locality would simply be propagated by cells that are not exactly symmetrical about every axis, where the distortion changes with distance from the distorting source. Excluding some cells marked in gray is not a problem at all. Remember that in the physical sciences variables are often described for convenience of measurement in partial differential equations where some other parameters are deliberately held constant for the purpose of expressing a special case. It is fairly easy to extend the example with momentum to exclude cells in the center of an orbit, or an exclusion principle of adjacent orbits to exclude cells on the outside of an orbit. All of these things are just a slightly more complicated model that is not necessary for the concept Johannes presented. Both principles can also be developed as consequences of competing actions from inside and outside the separate orbits. I’ve seen similar models over the past 40 years. Some were made of circles. Others were made of triangles. It is possible to think of all of those things interacting dynamically where the hexagons represent an average state in the absence of force fields. The model can get as complicated as necessary to remove any objection. This model needs to be reconciled with existing science that treats every point in space as an oscillator. Both classical optics and quantum mechanics depend on the oscillator models. Johannes gave pictures that really do allow such reconciliation by not showing a zero state of polarization between the positive and negative polarities. The result is one of the little jokes that Johannes always plays on us. From the picture we can’t tell which direction the orbits are rotating, clockwise or anti-clockwise. The same picture can be an oscillator that rotates back and forth, but then there would be a potential energy state variable in each cell that Johannes isn’t ready to show us just yet. If the model was expanded to have a choice of dynamic or potential energy states in each cell, then there would be enough elements to define a partition function for the energy that is variable with localized stress. It leads to local conditions described by local variables and local measurements, where there is energy contained in a field of oscillators with a frequency variable and an amplitude variable that can be defined as functions of the stresses and unstressed states. These types of models offer a path forward to resolve the 50 year stalemate of QFT and GR without fighting a strongly contested battle over the Dirac Sea Of Energy and the Cosmological Constant. If my example of a gravity source is replaced by an electric charge in the same corner, then the Reissner Nordström metric says the diagonal is compressed instead of being stretched. Remember electric charges are never found with out a rest mass. So the complete metric is predicting a competition of gravity with electric fields for curvature of space. The relative strength gradient for each field favors gravity at a distance and electric fields near the source. Somewhere in between the near and far fields there is a balanced region containing a lot of energy with a small cosmological constant. It’s called the vacuum partition theory. It gets more interesting when magnetic fields are added. That’s a bit too complicated for this page. It is found on the recent pages about variable fine structure. I won’t try to describe the picture with magnetic poles of different polarity on opposite ends of the diagonal. New data from Astronomers is suggestion the familiar metrics need to be rewritten. By now I hope the readers have decided that the example Johannes gave is more than a toy, even if it fun to work with. Paradoxes arise from false assumptions that can be removed in this case by making the model a bit more complicated. Models of this type have always been resisted because they resolve a long lasting argument. A lot of people prefer to have the argument instead of a resolution.
    A brave attempt to link Gravity and QFT through Rindler observers with just the right title:

    Physics from information
    http://arxiv.org/abs/1011.1657

    This is an ongoing review on my conjecture that information processing at causal horizons is the key ingredient of all physics. Assuming that information is fundamental and the information propagates with finite velocity, one can find that main physical laws such as Newton's second law and Einstein equation simply describe the energy-information relation (dE=TdS) for matter or space time crossing a causal horizon with temperature T for observers. Quantum mechanics arises from ignorance of the observers about matter crossing the horizon, which explains why superluminal communication is impossible even with quantum entanglement. This approach also explains the origin of Jacobson's thermodynamic formalism of Einstein gravity and Verlinde's entropic gravity. When applied to a cosmic causal horizon, the conjecture reproduces the observed dark energy and demands the zero cosmological constant.