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The Mott Problem: a spherically symmetric emission that records as a straight track

James Norman Ibbotson

Published Nov 1, 2026• 0 citations
Publisher

Abstract

An alpha-emitting nucleus is spherically symmetric and has no preferred axis. Quantum mechanics therefore describes the emitted alpha particle as an outgoing spherical wave of uniform angular amplitude, . Yet every cloud-chamber photograph of such an emission records a single straight track. This is Mott's problem (1929), the measurement problem in its sharpest experimental form: an apparent contradiction between a symmetry and a photograph. This paper (i) states the problem precisely, (ii) reproduces Mott's resolution quantitatively from CODATA constants — the alpha de Broglie wavelength, the angular tolerance set by the size of the recording atom, the resulting sideways wander over a finite track, and a direct numerical simulation of the joint alpha–atom amplitude that recovers the closed-form width, and (iii) examines a candidate interpretive model drawn from the Temporal Dynamics Framework and reports, on that model's own quantitative assumptions, that it adds no measurable prediction to Mott's result. This last outcome is recorded as a null, and a numerical target for any future derivation is fixed: rad for a 5.407 MeV alpha in hydrogen, equivalently a lateral wander of 1.86 m over a 10 cm track. No result here improves on Mott (1929); the solution is his. The contribution of this paper is a fully numerical restatement of that solution and an explicit, falsifiable target that fixes what any interpretive model would have to reproduce. This record holds one paper on its own and is refreshed every couple of months. The complete deposit, 10.5281/zenodo.21788037, holds every paper with its code and data and is updated first; for the newest version of this paper, go there.

DOI
10.5281/zenodo.23848237

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An alpha-emitting nucleus is spherically symmetric and has no preferred axis. Quantum mechanics therefore describes the emitted alpha particle as an outgoing spherical wave of uniform angular amplitude, . Yet every cloud-chamber photograph of such an emission records a single straight track. This is Mott's problem (1929), the measurement problem in its sharpest experimental form: an apparent contradiction between a symmetry and a photograph. This paper (i) states the problem precisely, (ii) reproduces Mott's resolution quantitatively from CODATA constants — the alpha de Broglie wavelength, the angular tolerance set by the size of the recording atom, the resulting sideways wander over a finite track, and a direct numerical simulation of the joint alpha–atom amplitude that recovers the closed-form width, and (iii) examines a candidate interpretive model drawn from the Temporal Dynamics Framework and reports, on that model's own quantitative assumptions, that it adds no measurable prediction to Mott's result. This last outcome is recorded as a null, and a numerical target for any future derivation is fixed: rad for a 5.407 MeV alpha in hydrogen, equivalently a lateral wander of 1.86 m over a 10 cm track. No result here improves on Mott (1929); the solution is his. The contribution of this paper is a fully numerical restatement of that solution and an explicit, falsifiable target that fixes what any interpretive model would have to reproduce. This record holds one paper on its own and is refreshed every couple of months. The complete deposit, 10.5281/zenodo.21788037, holds every paper with its code and data and is updated first; for the newest version of this paper, go there.
The Mott problem asks: Is there a microphysical mechanism - based only on Schroedinger's equation - that explains why an alpha particle emitted in a spherically symmetric nuclear decay produces a non-spherically-symmetric single track in a cloud chamber? This is a variant of the more general quantum measurement problem. Earlier, I proposed such a mechanism, drawing on quantum-mechanical Coulomb scattering and the thermal behavior of supersaturated vapors. I found that the probability that a track originates at distance R from the decay source is proportional to 1/R^2, with a proportionality constant that I expressed in terms of more fundamental parameters but was unable to estimate at the time. I tested the 1/R^2 law opportunistically using cloud chamber video from the Internet. Here, I draw on chemical physics to independently estimate the proportionality constant. The estimate is within a factor 1-2 of a value extracted directly from the data.
The Mott problem concerns a long-standing paradox in quantum mechanics: although alpha-particle wavefunctions emitted from radioactive sources are spherically symmetric, cloud chambers consistently record straight-line tracks. Standard explanations rely on decoherence, probabilistic branching, or implicit classical assumptions, yet none fully resolve how directional trajectories emerge from an initially isotropic quantum state. This paper presents a geometric interpretation of the Mott problem within the Dimensional Evolution (DE) framework, in which wavefunction collapse is treated as a resonance- and identity-mediated geometric process rather than a purely probabilistic event. Measurement is modeled as a structured interaction between system and detector identity wells, producing directional collapse funnels that anchor sequential localization events. Trajectory formation is described as a process of coherent tether crystallization, whereby successive measurement interactions align collapse curvature along a stable resonant direction. Straight tracks arise not from classical particle paths, but from the geometric reinforcement of collapse orientation through detector–system coupling. Inverse-domain resonance matching replaces environment-driven decoherence as the primary mechanism governing localization. The DE approach resolves the Mott paradox without invoking hidden variables, many-worlds branching, or ad hoc classical transitions, and provides a unified geometric explanation for trajectory emergence in quantum measurement systems. Implications for quantum foundations, measurement theory, and experimental testability are discussed.
Abstract The Mott problem is a simpler version of the quantum measurement problem that asks: Is there a microscopic physical mechanism – based (explicitly or implicitly) only on Schroedinger’s equation – that explains why a single alpha particle emitted in a single spherically symmetric s-wave nuclear decay produces a manifestly nonspherically symmetric single track in a cloud chamber? I attempt here to generalize earlier work that formulated such a mechanism. The key ingredient there was identification of sites at which the cross section for ionization by a passing charged particle is near singular at ionization threshold. This near singularity arose from a Penning-like process involving molecular polarization in subcritical vapor clusters. Here, I argue that the same Mott problem question should be asked about Geiger counters. I then define a simple experiment to determine if ionization physics similar to the cloud chamber case takes place in the mica window of a Geiger counter and explains the collimation of wavefunctions that are spherically symmetric outside the counter into linear ion tracks inside. The experiment measures the count rate from a radioactive point source as a function of source-window separation. I have performed a proof of concept of this experiment; results are reported here and support the near-singular-ionization picture. These results are significant in their own right, and they may shed light on physical mechanisms underlying instances of the full quantum measurement problem. I illustrate this for the Stern–Gerlach experiment and a particular realization of superconducting qubits. I conclude by detailing further work required to flesh out these results more rigorously.
We present a resolution to the Mott problem (the apparent paradox of spherical quantum waves producing linear particle tracks) within the Fabric substrate framework. We propose that the wave function represents coherence patterns in a universal memory field M(x,t), and that particle detection corresponds to threshold-activated nucleation cascades in this substrate. The mechanism naturally explains track formation, straightness, and decoherence without invoking wave function collapse or many-worlds branching. We derive the nucleation dynamics, establish testable predictions distinguishing this interpretation from standard quantum mechanics, and connect the framework to agency and beauty as fundamental principles.
The Mott problem asks why a spherically symmetric quantum emission produces localized, linear ionization tracks rather than diffuse excitation. This paper presents an effective, interaction-level dynamical account of directional track formation based on local amplification, environmental response, and irreversible medium disturbance. The mechanism operates entirely within standard detector physics and does not invoke wavefunction collapse, observer dependence, or global selection principles. The analysis demonstrates how cumulative local interactions can dynamically consolidate a single persistent track, while explicitly showing that even a complete dynamical account does not explain the necessity of a unique outcome. That limitation is identified as a substantive result rather than a deficiency. The work is deliberately agnostic with respect to deeper ontological or constraint-based interpretations. Constraint-level closure of the Mott problem has been treated separately by the author in companion works.
This paper presents an ontological solution to the Mott problem, a foundational paradox in quantum mechanics concerning how a spherically symmetric wave function (e.g., from an alpha particle) produces a single, linear track in a classical detector. While Sir Nevill Mott's 1929 mathematical solution is complete, this work addresses the remaining philosophical unease by proposing a physical mechanism that selects a single classical path from an infinity of quantum possibilities. The solution is grounded in the KnoWellian Universe Theory (KUT), a framework built on procedural metaphysics. We posit that the formation of a particle track is not a wave function collapse but a KnoWellian Rendering Cascade—an irreversible, sequential transformation of potentiality into actuality. This process is governed by the KnoWellian Resonant Attractor Manifold (KRAM), a dynamic memory substrate of the cosmos. A modified Bohmian (pilot-wave) mechanic is proposed, where the particle's pilot-wave (identified as the Chaos Field in KUT) physically "etches" a directional "imprint" onto the local KRAM geometry upon the first rendering event (ionization). This imprint creates an attractor valley that makes subsequent rendering events along the same vector path overwhelmingly probable. The linear track is thus re-framed not as a "miraculous" alignment of probabilities but as a deterministic cascade causally guided by the memory of its own becoming. This framework provides a physical mechanism for the phase correlations in Mott's original solution and offers a new, testable foundation for understanding the quantum-to-classical transition.