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This site is a continuation of earlier versions, started the late 1990’s as an outlet for curiosity as to the relationship between Albert Einstein’s Special Theory of Relativity, and Quantum Mechanics (QM).

Overview: Quantum Mechanics with a Game Engine

Conventional quantum interpretations seek to form a correspondence between interference phenomena characteristic of classical wave phenomena and the equations of quantum mechanics, thereby leading to various concepts such as of wave-particle duality, decoherence, and multiple realities.

In brief, when particles (e.g. atoms, electrons, molecules) are fired through a suitable grating, they form scattering patterns where particle densities exactly match the intensity of a wave interference pattern.  A simple formula (the de Broglie equation) connects particle momentum to a wavelength that would result in the observed pattern should the wave undergo interference.

Taken together with the fact that particles are localised and discrete, it seems reasonable to suppose that the mechanism of wave interference must be taking place but must somehow be concealed from direct observation, and accordingly various interpretations share common threads.

  • That there are distinct classical and quantum domains, the quantum domain is characterised by wave-like behaviour and interference, whereas in the classical domain particles are localised and discrete.
  • The equations of quantum theory are quite literally describing wave interference.
  • The job of an interpretation is to explain how a non-local and distributed wave interference process can be reconciled with the fact that particles are always detected as discrete local entities. The wave process must be concealed from direct observation.

Differing attempts to reconcile the continuous and non-local features of wave interference with the discrete interactions characteristic of quantum mechanics – tend to be regarded as the only possible options.

Whether it is a multiverse where all possible realities exist simultaneously or an ephemeral ‘wave function’ that crosses space and time only to ‘collapse’ or ‘decohere’ on measurement down to one single outcome from a continuous spatial distribution of possible outcomes, the job of these added mechanisms (collapse/multiple realities) is to link continuous wave-like probability distributions back to singular discrete events, by invoking a hidden, but classical, wave-like interference process.

In essence, the conundrum over apparently counter-intuitive effects, such as ‘wavefunction collapse’ and ‘multiple realities’ (which I would argue are ad-hoc mechanisms, not actually there in quantum mechanics itself), results from the need to add these ad-hoc devices to rescue the idea that wave-particle duality explains how quantum mechanics works.

One avenue that could be worth following is to explore William Duane’s 1923 hypothesis for crystal diffraction, where quantum scattering is modeled using discrete momentum exchanges between and incident particle and a scattering object.

Duane showed how Einstein’s work on the photomodelledc effect provides a model for quantised exchange of momentum that can be applied to the diffraction of X-rays by crystals. This model allows the problem to be treated as a discrete particle scattering problem.  In effect, Duane derived the same scattering relationships that were derived by Bragg’s wave model, “based on quantum ideas without reference to interference laws.” (www.pcontent/9/5/15nas.org/8).

Duane’s work was extended by Gregory Breit (www.pnas.org/content/9/7/238) to explain how diffraction through gratings and slits can also be analyzed using discrete momentum transfers.

At first appearance, Duane’s work might appear to be at variance with the mathematical representations in contemporary quantum theory, because of the notion that interference is crucial then leading to an expectation that the incident particles should somehow (at least transiently) act like classical waves in order to generate an interference pattern.

In effect, the conventional approach (where the incident particle is supplying the ‘waves’ that undergo an interference process) implicitly leads to the idea that the incident particle must the key element, both at scattering and detection.

In contrast, Duane’s analysis of crystal scattering shows that the scattering can also be explained if the scattering is governed by a set of permitted quantized reactions that are a property of the crystal structure, and furthermore, are completely independent of the type of incident particle or its velocity and energy.

By employing standard quantum theory to calculate the possible reactions of an extended object, Duane’s approach looks to provide a better fit to the mathematical formalism of contemporary quantum mechanics than the tortuous rationalisations of wave-particle duality, where the incident particle is thought to mysteriously ‘explore’ the scattering object as a classical wave, then recombine via collapse or ‘decoherence’.

Duane’s work shows how scattering by crystals and gratings (with Breit, including the notorious ‘double slit’) can be straightforwardly modeled by treating the reactions of the scattering object as being constrained to a quantized set of possible reactions while the incident particles are treated as localized entities that obey the rules of energy and momentum conservation.

Unlike fully deterministic classical mechanics, Duane’s model requires quantized momentum transfers that depend on the state and structure of the scattering object and this dependency injects the required uncertainty in outcomes to be consistent with quantum constraints on determining particle position at the time of interaction.  The major difference is that while the position cannot be measured (which requires some form of additional interaction), in Duane’s model the particles can have definite positions and trajectories, they just cannot be observed without disrupting the outcome of the experiment.

Because Duane’s model keeps the incident particle as a discrete entity throughout, a simple model can be constructed with particles following definite trajectories before and after the interaction. As can be seen in the simulation, the ability of this simple model to reproduce Laue scattering patterns is striking in both simplicity and beauty.

I am in the process of building a small Web-based game that people can use to explore the workings of this type of model. This is in the early stages of being ported to a web environment, the explanations and user interface are very much under construction. Nevertheless, feel free to explore.

Game engine simulation of quantized scattering at a grating.(An initial test of a WebGL version of these simulations is available here.)

At this point, the function of the test is to determine the feasibility of developing an educational example that shows how Duane’s model works to provide an alternative to de Broglie’s idea of wave-particle duality)

In essence, taking Duane’s approach involves shifting our view as to what the mathematical equations of quantum theory represent without throwing the ‘baby out with the bathwater’. The primary shift in viewpoint is to challenge the conventional view that the equations completely represent the behavior of incident particles that individually explore all avenues through a classically passive scattering object, and then later magically turn up as discrete localized objects on detection.

Despite the radical differences between interpretations based on interference/wave-particle duality, (e.g. ‘pilot wave’/collapse’/’multiple realities’), these interpretations have a common basis. All contain attempts to couple observed scattering patterns to the same type of interference processes that classical waves undergo. As if there is a one-to-one correspondence between the mathematical tools of quantum theory and the interference of classical waves.

In contrast, Duane showed that if one treats the possible momentum reactions that an extended object can make as being a discrete and quantized, then the set of reactions that are required to reproduce the observed crystal scattering can be tied to the crystal geometry using the same quantum rules that Niels Bohr had deduced for the angular momentum of atomic orbital