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Kinematic Evolution and the Omega Naught Parameter: A Semi-Classical Analysis of Particle Trajectories and Quantization

Ankush Bhattacharyya

Published Apr 14, 2026• 0 citations
Publisher

Abstract

This monograph provides an in-depth analysis of particle kinematics through the lens of a newly proposed semi-classical parameter, Omega Naught. Rather than treating quantum and classical regimes as disparate entities, this work explores the transitionary "granularity" of motion that emerges when reconciling de Broglie’s wave-particle duality with Newtonian force relations. The analysis utilizes the derivation of the v^3 = K*a relation as a primary kinematic signature to test the validity of the Omega Naught framework. Furthermore, the study demonstrates the robustness of this model by applying it to Bohr’s quantization of the Hydrogen atom, showing that such quantum states emerge naturally as geometric consequences of the underlying kinematic constraints. By documenting boundary conditions and velocity-acceleration dynamics over extensive theoretical derivations, this paper establishes Omega Naught as a critical scaling constant for predicting system behavior in the semi-classical regime. The results offer a unified perspective on quantization as an extension of fundamental kinematic evolution.

DOI
10.5281/zenodo.19572292

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The Kinematics of Quantum Space A Classical Proof of Orbital Stability and Trajectory Continuity (Part II)

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Abstract The Kinematics of Quantum Space: A Classical Proof of Orbital Stability and Trajectory Continuity (Part II) Building upon the dense, discrete, nonlocal medium defined in Part I (Quantum Space, density ratio ρ = 6.54×10¹²), we prove that the electron in a hydrogen atom follows a strictly deterministic, continuous, and classical trajectory. No probabilistic interpretation, wave function collapse, or irreducible uncertainty is required. 1. Orbital velocity – six independent derivations Starting from the Bohr radius (a₀ = 5.291772×10⁻¹¹ m) and the electron mass (mₑ = 9.109384×10⁻³¹ kg), we derive the ground state orbital velocity through six independent physical paths: Galilean kinematics (v = s/t) Bohr quantization condition (mₑ v a₀ = ħ) Fine‑structure constant (v = α c, α = 1/137.036) Kinetic energy (ionization energy 13.6 eV) Coulomb–centripetal force balance Direct experimental transit time (attosecond measurements) All six converge identically to: v=e22ϵ0h=αc≈2.188×106 m/sv=2ϵ0he2=αc≈2.188×106m/s The electron is a real satellite of the nucleus, not a probability cloud. 2. Orbital stability – zero radiation from destructive interference The classical objection (Larmor's formula predicts radiative collapse within ≈47 ps) assumes a point charge. For a standing wave charge distribution satisfying 2πr = nλ (Bohr condition), we compute the Liénard–Wiechert potentials and the far‑field Poynting vector explicitly: S=1μ0Erad×Brad=0,Ptotal=∮S⋅dA=0S=μ01Erad×Brad=0,Ptotal=∮S⋅dA=0 The ground state does not radiate. Energy is locked in the standing wave. Radiation occurs only during transitions (n→m), exactly as observed in atomic spectroscopy. 3. Quantum jump as a vertical ballistic throw – continuity proven The transition n=1 → n=2 (energy ΔE = 10.2 eV) is treated as a classical vertical throw in an effective constant acceleration field g_q: gq=FCoulomb(a0)me=kee2mea02≈9.043×1022 m/s2gq=meFCoulomb(a0)=mea02kee2≈9.043×1022m/s2 Jump height: h = r₂ - r₁ = 1.5875×10⁻¹⁰ mEffective initial velocity (constant‑g approximation): v₀ ≈ 5.36×10⁶ m/sTime of ascent: t_up = v₀/g_q ≈ 59 asTotal flight time: t_total = 118 as The position function y(t) = v₀ t - ½ g_q t² is continuous and differentiable (C¹ class). The illusion of an instantaneous "quantum jump" arises solely because t_total is shorter than the temporal resolution of most instruments (Δt_instr ≫ 118 as). The trajectory exists – we are simply not fast enough to see it. 4. Spin as toroidal vortex kinematics – no superluminal speed Spin (S_z = ±½ħ) is not a rigid sphere rotation. We model the electron as a toroidal charge distribution with major radius R. The no‑superluminal condition v = ωR < c yields a lower radius bound: Rmin=ℏ2mec≈1.93×10−13 mRmin=2mecℏ≈1.93×10−13m This is physically reasonable (≈300× smaller than the Bohr radius). Quantization to ±½ħ follows from resonance stability: only prograde (+) and retrograde (–) synchronous rotations are stable, analogous to the Moon (synchronous) and Venus (retrograde). 5. 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Keywords: orbital stability, Larmor paradox, destructive interference, Poynting vector, quantum jump as ballistic throw, attosecond transit time, toroidal spin, Compton scattering measurement, Bell inequalities reinterpretation, classical determinism, falsifiable predictions, scale inversion. PACS: 03.65.Sq (Semiclassical theories), 03.65.Ta (Foundations), 31.15.xk (Classical treatments of atomic structure), 32.80.t (Atomic transitions), 42.50.Ct (Quantum optics, measurement).MSC: 81Q05 (Closed and approximate solutions), 70F05 (Two‑body problem, Kepler), 78A35 (Motion of charged particles), 83A05 (Special relativity).arXiv: quant-ph, physics.class-ph, physics.atom-ph.

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Bohmian mechanics is endowed with an ontological package that supposedly allows to solve the main interpretational problems of quantum mechanics. We are concerned in this work by the emergence of classicality from the quantum mechanical substrate. We will argue that although being superficially attractive, the de Broglie-Bohm interpretation does not shed new light on the quantum-to-classical transition. This is due to nature of the dynamical law of Bohmian mechanics by which the particles follow the streamlines of the probability flow. As a consequence, Bohmian trajectories can be highly non-classical even when the wavefunction propagates along classical trajectories, as happens in semiclassical systems. In order to account for classical dynamics, Bohmian mechanics needs non-spreading and non-interfering wave packets: this is achieved for practical purposes by having recourse to decoherence and dense measurements. However one then faces the usual fundamental problems associated with the meaning of reduced density matrices. Moreover the specific assets of the de Broglie-Bohm interpretation – in particular the existence of point-like particles pursuing well-defined trajectories – would play no role in accounting for the emergence of classical dynamics.

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de Broglie’s concept of particles as sources of phase is extended to the analysis of systems in which the potential is not constant. The treatment assumes that the phase information propagates as waves according to classical electrodynamics including reflection with phase changes from potential energy barriers. The energies and weighting functions in such cases are obtained by comparison of the phase of the accelerated particle relative to the phases of reflections from the change in potential. Application to the chemically interesting systems of the harmonic oscillator and hydrogen atom are considered using the time evolution of the relative phases of the reflected de Broglie phase waves, whereby the weighting functions are obtained from the distance dependence of the phase differences between the reflections and the source. This is accomplished conveniently by taking time derivatives of the relative de Broglie phases and considering the periodicity of the motion. Optimum trajectories are determined by minimization of the action 2i(mv2-r∂V/∂r)/ħγ which depends on the potential V and the velocity v. The treatment leads to the Newtonian force law for circular orbits and affords the same energies as derived using the Schrödinger equation.

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Sheldon Goldstein, Ward Struyve

Non-relativistic de Broglie–Bohm theory describes particles moving under the guidance of the wave function. In de Broglieʼs original formulation, the particle dynamics is given by a first-order differential equation. In Bohmʼs reformulation, it is given by Newtonʼs law of motion with an extra potential that depends on the wave function—the quantum potential—together with a constraint on the possible velocities. It was recently argued, mainly by numerical simulations, that relaxing this velocity constraint leads to a physically untenable theory. We provide further evidence for this by showing that for various wave functions the particles tend to escape the wave packet. In particular, we show that for a central classical potential and bound energy eigenstates the particle motion is often unbounded. This work seems particularly relevant for ways of simulating wave function evolution based on Bohmʼs formulation of the de Broglie–Bohm theory. Namely, the simulations may become unstable due to deviations from the velocity constraint.

arXiv:1312.1990•Journal of Physics A Mathematical and Theoretical•Dec 11, 2014•18 citations
This monograph provides an in-depth analysis of particle kinematics through the lens of a newly proposed semi-classical parameter, Omega Naught. Rather than treating quantum and classical regimes as disparate entities, this work explores the transitionary "granularity" of motion that emerges when reconciling de Broglie’s wave-particle duality with Newtonian force relations. The analysis utilizes the derivation of the v^3 = K*a relation as a primary kinematic signature to test the validity of the Omega Naught framework. Furthermore, the study demonstrates the robustness of this model by applying it to Bohr’s quantization of the Hydrogen atom, showing that such quantum states emerge naturally as geometric consequences of the underlying kinematic constraints. By documenting boundary conditions and velocity-acceleration dynamics over extensive theoretical derivations, this paper establishes Omega Naught as a critical scaling constant for predicting system behavior in the semi-classical regime. The results offer a unified perspective on quantization as an extension of fundamental kinematic evolution.
Abstract The Kinematics of Quantum Space: A Classical Proof of Orbital Stability and Trajectory Continuity (Part II) Building upon the dense, discrete, nonlocal medium defined in Part I (Quantum Space, density ratio ρ = 6.54×10¹²), we prove that the electron in a hydrogen atom follows a strictly deterministic, continuous, and classical trajectory. No probabilistic interpretation, wave function collapse, or irreducible uncertainty is required. 1. Orbital velocity – six independent derivations Starting from the Bohr radius (a₀ = 5.291772×10⁻¹¹ m) and the electron mass (mₑ = 9.109384×10⁻³¹ kg), we derive the ground state orbital velocity through six independent physical paths: Galilean kinematics (v = s/t) Bohr quantization condition (mₑ v a₀ = ħ) Fine‑structure constant (v = α c, α = 1/137.036) Kinetic energy (ionization energy 13.6 eV) Coulomb–centripetal force balance Direct experimental transit time (attosecond measurements) All six converge identically to: v=e22ϵ0h=αc≈2.188×106 m/sv=2ϵ0he2=αc≈2.188×106m/s The electron is a real satellite of the nucleus, not a probability cloud. 2. Orbital stability – zero radiation from destructive interference The classical objection (Larmor's formula predicts radiative collapse within ≈47 ps) assumes a point charge. For a standing wave charge distribution satisfying 2πr = nλ (Bohr condition), we compute the Liénard–Wiechert potentials and the far‑field Poynting vector explicitly: S=1μ0Erad×Brad=0,Ptotal=∮S⋅dA=0S=μ01Erad×Brad=0,Ptotal=∮S⋅dA=0 The ground state does not radiate. Energy is locked in the standing wave. Radiation occurs only during transitions (n→m), exactly as observed in atomic spectroscopy. 3. Quantum jump as a vertical ballistic throw – continuity proven The transition n=1 → n=2 (energy ΔE = 10.2 eV) is treated as a classical vertical throw in an effective constant acceleration field g_q: gq=FCoulomb(a0)me=kee2mea02≈9.043×1022 m/s2gq=meFCoulomb(a0)=mea02kee2≈9.043×1022m/s2 Jump height: h = r₂ - r₁ = 1.5875×10⁻¹⁰ mEffective initial velocity (constant‑g approximation): v₀ ≈ 5.36×10⁶ m/sTime of ascent: t_up = v₀/g_q ≈ 59 asTotal flight time: t_total = 118 as The position function y(t) = v₀ t - ½ g_q t² is continuous and differentiable (C¹ class). The illusion of an instantaneous "quantum jump" arises solely because t_total is shorter than the temporal resolution of most instruments (Δt_instr ≫ 118 as). The trajectory exists – we are simply not fast enough to see it. 4. Spin as toroidal vortex kinematics – no superluminal speed Spin (S_z = ±½ħ) is not a rigid sphere rotation. We model the electron as a toroidal charge distribution with major radius R. The no‑superluminal condition v = ωR < c yields a lower radius bound: Rmin=ℏ2mec≈1.93×10−13 mRmin=2mecℏ≈1.93×10−13m This is physically reasonable (≈300× smaller than the Bohr radius). Quantization to ±½ħ follows from resonance stability: only prograde (+) and retrograde (–) synchronous rotations are stable, analogous to the Moon (synchronous) and Venus (retrograde). 5. Measurement as ballistic collision – Heisenberg is technical, not fundamental A typical measurement photon (λ = 0.1 nm, E ≈ 12.4 keV) carries momentum: pphoton=hλ≈6.626×10−24 kg⋅m/spphoton=λh≈6.626×10−24kg⋅m/s The electron's orbital momentum is: pelectron=mev≈1.993×10−24 kg⋅m/spelectron=mev≈1.993×10−24kg⋅m/s Ratio: p_photon / p_electron ≈ 3.33. The photon delivers more momentum than the electron possesses in its orbit. Measurement is not passive observation – it is a ballistic collision (Compton scattering). The post‑collision electron momentum is fully determinable if both the energy and scattering angle of the outgoing photon are measured precisely. "Uncertainty" is a technical deficiency of incomplete measurement, not a law of nature. 6. Five falsifiable predictions Electron transit time across one Bohr diameter: 48.4 ± 5 as (testable with attosecond spectroscopy). n=1 → n=2 transition duration: 100–120 as (continuous, not instantaneous). Heisenberg product Δx·Δp → 0 as detector precision → ∞ (no fundamental lower bound). Bell inequality violations decrease as measurement impulse strength decreases (weak measurement regime). Residual "quantum randomness" equals unmodeled environmental force noise; full force accounting restores classical determinism. 7. Conclusion All calculations use only standard constants and classical equations (Newton, Maxwell, Coulomb, Compton). No new postulates are introduced. The electron's path exists, is continuous, and follows deterministic mechanics. Quantum mysticism – wave function collapse, irreducible uncertainty, non‑locality as magic – is replaced by scale‑inverted classical physics operating within the dense geometry of Quantum Space defined in Part I. Keywords: orbital stability, Larmor paradox, destructive interference, Poynting vector, quantum jump as ballistic throw, attosecond transit time, toroidal spin, Compton scattering measurement, Bell inequalities reinterpretation, classical determinism, falsifiable predictions, scale inversion. PACS: 03.65.Sq (Semiclassical theories), 03.65.Ta (Foundations), 31.15.xk (Classical treatments of atomic structure), 32.80.t (Atomic transitions), 42.50.Ct (Quantum optics, measurement).MSC: 81Q05 (Closed and approximate solutions), 70F05 (Two‑body problem, Kepler), 78A35 (Motion of charged particles), 83A05 (Special relativity).arXiv: quant-ph, physics.class-ph, physics.atom-ph.
Bohmian mechanics is endowed with an ontological package that supposedly allows to solve the main interpretational problems of quantum mechanics. We are concerned in this work by the emergence of classicality from the quantum mechanical substrate. We will argue that although being superficially attractive, the de Broglie-Bohm interpretation does not shed new light on the quantum-to-classical transition. This is due to nature of the dynamical law of Bohmian mechanics by which the particles follow the streamlines of the probability flow. As a consequence, Bohmian trajectories can be highly non-classical even when the wavefunction propagates along classical trajectories, as happens in semiclassical systems. In order to account for classical dynamics, Bohmian mechanics needs non-spreading and non-interfering wave packets: this is achieved for practical purposes by having recourse to decoherence and dense measurements. However one then faces the usual fundamental problems associated with the meaning of reduced density matrices. Moreover the specific assets of the de Broglie-Bohm interpretation – in particular the existence of point-like particles pursuing well-defined trajectories – would play no role in accounting for the emergence of classical dynamics.
Abstract In this work, we investigate the emergence of quantum structures within a purely geometric field framework based on a unified helical configuration. Building on the geometric foundations and limiting recovery principles established in the preceding papers of this series, we demonstrate that quantization arises as a consequence of topological and spectral constraints imposed on the underlying helical field, rather than being introduced as a fundamental postulate. We show that discrete spectral sectors naturally follow from global and local topological conditions on the field configuration space, leading to an intrinsic form of quantization without invoking canonical commutation relations or operator axioms. Effective quantum operators are constructed directly from geometric functionals of the helical field, yielding non-commutative structures as emergent features of constrained geometry. Within this setting, Planck’s constant appears as an effective parameter characterizing the spectral density of admissible configurations, rather than as a fundamental universal constant. The framework consistently recovers standard quantum kinematics in appropriate limiting regimes while remaining fully compatible with the classical and relativistic limits previously derived. This approach provides a coherent geometric interpretation of quantum discreteness, operator structure, and effective constants, thereby offering a unified perspective in which classical, relativistic, and quantum descriptions arise from a single geometric field without assuming independent foundational layers.
For nearly a century, the standard formulation of quantum mechanics has relied upon the probabilistic interpretation of physical states, fundamentally utilizing the wavefunction () to describe the position, momentum, and state of sub-atomic entities as a distribution of statistical likelihoods. The Copenhagen interpretation, which posits that physical systems do not possess definite properties prior to measurement, has served as the operational foundation of modern quantum physics. However, this stochastic abstraction has persistently generated profound epistemological and physical paradoxes, most notably the unresolved nature of wavefunction collapse and the mathematical friction encountered when attempting to unify quantum mechanics with the deterministic, continuous manifold of general relativity.
de Broglie’s concept of particles as sources of phase is extended to the analysis of systems in which the potential is not constant. The treatment assumes that the phase information propagates as waves according to classical electrodynamics including reflection with phase changes from potential energy barriers. The energies and weighting functions in such cases are obtained by comparison of the phase of the accelerated particle relative to the phases of reflections from the change in potential. Application to the chemically interesting systems of the harmonic oscillator and hydrogen atom are considered using the time evolution of the relative phases of the reflected de Broglie phase waves, whereby the weighting functions are obtained from the distance dependence of the phase differences between the reflections and the source. This is accomplished conveniently by taking time derivatives of the relative de Broglie phases and considering the periodicity of the motion. Optimum trajectories are determined by minimization of the action 2i(mv2-r∂V/∂r)/ħγ which depends on the potential V and the velocity v. The treatment leads to the Newtonian force law for circular orbits and affords the same energies as derived using the Schrödinger equation.
Non-relativistic de Broglie–Bohm theory describes particles moving under the guidance of the wave function. In de Broglieʼs original formulation, the particle dynamics is given by a first-order differential equation. In Bohmʼs reformulation, it is given by Newtonʼs law of motion with an extra potential that depends on the wave function—the quantum potential—together with a constraint on the possible velocities. It was recently argued, mainly by numerical simulations, that relaxing this velocity constraint leads to a physically untenable theory. We provide further evidence for this by showing that for various wave functions the particles tend to escape the wave packet. In particular, we show that for a central classical potential and bound energy eigenstates the particle motion is often unbounded. This work seems particularly relevant for ways of simulating wave function evolution based on Bohmʼs formulation of the de Broglie–Bohm theory. Namely, the simulations may become unstable due to deviations from the velocity constraint.