This is a follow-up to my earlier Quantum Speculations paper on detector-surface passivity. It assembles two classical surface effects—geometric micro-arc steering at real slit edges (R ≈ 50–300 nm) and self-organized charge-mound electrostatic steering—into one hypothesized five-step causal chain that can generate or modulate fringe-like angular bands under high coherence. The chain is strictly local to the slit edge and its near field (decay ≲ 1 µm); once a particle leaves that zone, free-space propagation is standard. The quantitative relations (channel law, dwell-time proxy, mound period/amplitude, deflection estimate) are provisional bookkeeping only. The 18 null tests in Appendix A are the procedure that would fix, reject, bound, or refine them—not a confirmation exercise for formulas already assumed true. The paper is offered as a calibration tool for high-coherence experiments: positive results would indicate measurable classical surface contributions at the classical–quantum interface; consistent nulls would tighten bounds on such effects. Comments and criticism are welcome.
This is a follow-up to my earlier Quantum Speculations paper on detector-surface passivity. It assembles two classical surface effects—geometric micro-arc steering at real slit edges (R ≈ 50–300 nm) and self-organized charge-mound electrostatic steering—into one hypothesized five-step causal chain that can generate or modulate fringe-like angular bands under high coherence. The chain is strictly local to the slit edge and its near field (decay ≲ 1 µm); once a particle leaves that zone, free-space propagation is standard. The quantitative relations (channel law, dwell-time proxy, mound period/amplitude, deflection estimate) are provisional bookkeeping only. The 18 null tests in Appendix A are the procedure that would fix, reject, bound, or refine them—not a confirmation exercise for formulas already assumed true. The paper is offered as a calibration tool for high-coherence experiments: positive results would indicate measurable classical surface contributions at the classical–quantum interface; consistent nulls would tighten bounds on such effects. Comments and criticism are welcome.
In electron and photon interference experiments, detectors often display fringe patterns and coarse banding whose detailed appearance varies with material, exposure history, coherence, flux, and vacuum conditions — raising questions about the assumption that detection screens are strictly passive recorders of incident intensity. Though previous experiments used every known rigorously controlled procedure to minimize surface interactions, the passivity of those surfaces has yet to be explicitly tested. This paper proposes a set of empirical tests to assess whether coherence-sensitive, detector-local dynamics — including charge redistribution, gradual structural deformation, local heating, reversible trap occupancy, and surface contamination — contribute measurably to observed interference patterns. Specifically, it introduces a speculative, classical mechanism — the Emergent Attractor Model (EAM) — in which mask-edge-seeded coherence correlations are amplified through a multi-field cascade of history-dependent processes on the detector surface, modulating local absorption probabilities over multiple timescales. The primary purpose of the model is to null test as many contributing variables as possible. In EAM, emergent attractors form on conductive surfaces under grazing incidence. A single surface (such as a mask edge) can generate visible fringes via self-organized lateral excitations. In double-slit configurations, both the mask edge and detector surface contribute, with the detector amplifying mask-seeded correlations through impact-driven multi-field feedback. The proposed model reproduces key features of both single- and double-slit patterns, including blurred envelopes with banding, high-contrast fringe trains, long-term evolution of pattern contrast, flux-dependent visibility, and vacuum/history effects, without invoking free-space wave interference at the screen. It offers a concrete, falsifiable framework for testing the Apparatus Passivity Assumption and exploring whether EAM-like dual-site effects are present in real systems. Several qualitative predictions and diagnostic experiments are outlined to probe material dependence, coherence sensitivity, exposure history, flux, vacuum conditions, and reset protocols. These tests aim not to revise quantum mechanics, but to clarify the role of the detector in shaping observed patterns — and to determine whether EAM-like effects are present in real systems. The surface is a physical object governed by condensed matter physics, and diagnosing its complexity might complement decades of existing work in quantum interference. EAM is one possible detector-side mechanism among many, and every null result could still be informative for understanding detector physics. We propose testing this speculative model so that it can be conclusively falsified. Regardless of the final outcome, the field wins. Correspondence: rauwolfa@gmail.com
The double-slit experiment combines three observational facts: interference fringes in the coherent regime, position-resolved detections, and continuous fringe suppression under which-path resolution. Standard quantum mechanics accommodates all three through postulates without deriving them from deeper structure. This paper shows that the standard far-field interference law and the coherence-to-which-path transition follow as structural corollaries of results established in Quantum Mechanics as the Boundary Algebra of a Non-Invertible Projection (doi:10.5281/zenodo.19535588) and its companion (doi:10.5281/zenodo.19571321). Two results suffice for the algebraic derivation: the Born rule as the canonical quadratic measure on Im(Π), and the kernel spinor as the Hilbert quadrature of the boundary field. A third result — measurement irreversibility as a kinematic consequence of the projection geometry — belongs to the physical interpretation of measurement and temporal ordering within the same framework. The paper derives the Fraunhofer intensity law I(x) ∝ |Ψ₁ + Ψ₂|² and the detector-overlap formula with fringe visibility V = |γ|, within the standard Fraunhofer approximation and without additional postulates. It does not claim a first-principles derivation of the full boundary propagator or of single-event arrival statistics. A companion numerical simulation implements all three coherence regimes. A self-contained appendix summarises the three imported results in compact form.
The double-slit experiment is often framed as evidence that microscopic objects are “both waves and particles,” or that a wavefunction “collapses” upon measurement. This paper gives a QMU-native, apparatus-centric explanation in the Aether Physics Model (APM) by separating the experiment into three operational layers: (1) Transport layer (space): Light is treated as a conserved transport content, denoted here as ligt, distributed over expanding photon fronts. The measurable quantity in space is the delivered areal density (intensity) lint(ν;r). Interference is asserted at this transport layer: two outgoing channels can superpose and form stable bright and dark regions in lint at the screen plane before any detection event occurs. (2) Boundary layer (aperture): The slit-mask is modeled as a transfer operator T acting on the incident delivery density:lintout(ν;r)=Tlintin(ν;r).For a double slit, the outgoing density is produced by two transfer channels, T1 and T2, whose superposition yields an intensity-level interference formlinttot(P)=lint1(P)+lint2(P)+2lint1(P)lint2(P)cosΔϕ(P).The phase difference is written in QMU-normalized form using the chronovibration identity and the dimensionless cadence:c=FqλC,ν∗=Fqν,λ=ν∗λC,so thatΔϕ(P)=2πλΔℓ(P)=2πν∗λCΔℓ(P).In the far-field approximation with slit separation d, screen distance L, and transverse coordinate x, Δℓ(x)≈dx/L, givingΔϕ(x)≈2πν∗LdλCx.This emphasizes that the fringe map is a geometric count in units of λC scaled by the dimensionless cadence ν∗. (3) Detection layer (matter): Detection is a discrete resonance gate event in matter, not a continuous “field readout.” The receiver is represented by a binary acceptance functionG(ν∗,alignment)∈{0,1},and the event-rate density follows the gated effective drivelinteff(r)=∫G(ν∗,alignment)R(ν∗)lint(ν;r)dν,N˙e(r)∝linteff(r).Single-particle hits therefore build the fringe pattern because discrete events sample a pre-existing transport interference pattern in lint. Coherence window and a falsifiable fringe condition The paper introduces a receiver coherence window τg and its QMU-normalized form τg∗=Fqτg. This produces a detector gate coherence lengthLg=cτg=λCτg∗,and a direct, falsifiable interference conditionΔℓ(P)≲λCτg∗.A key operational refinement is the \emph{minimum law} for the observed visibility rolloff length:Lrolloff≈min(Lc,Lg),where Lc is a transport coherence length set by source bandwidth / wavefront quality, and Lg is the detector’s gate coherence length. This predicts two distinct regimes and a detector-dependent saturation plateau when Lc is increased beyond Lg. Which-path marking as controlled timing-jitter injection Which-path devices are treated as measurable degradations (timing/phase jitter, alignment scrambling, or mode partitioning), not metaphysical collapse. A minimal quantitative model treats marking as injecting an RMS delay σt between channels, with QMU-normalized jitter σt∗=Fqσt. For Gaussian jitter, the visibility obeysV=V0exp[−2π2(ν∗)2(σt∗)2],yielding a clean functional form for tunable weak-to-strong marking protocols. Slit-edge participation and QMU surface knobs (including qsfo) To make boundary participation experimentally reportable, the slit transfer operator is decomposed asT=Tgeom+Tsurf,where Tsurf captures mask material / coating / roughness / polarization-sensitive surface channels. The paper introduces QMU-native surface oscillation knobs:qsfo:=λCc3=λC2Fq3,qsfi:=c3λC=qsfo1,and defines a dimensionless surface-participation ratioΠsurf:=Ωsurfqsfi,so that “edge effects” are reported as measured QMU parameters rather than qualitative caveats. What this upload contains This Zenodo upload includes the full paper (PDF) written in the QADI template style, with: (i) a transport/boundary/detection decomposition, (ii) QMU-normalized fringe geometry, (iii) a detector-dependent coherence-window prediction (τg∗ and Lg), (iv) the minimum-law saturation test, (v) a timing-jitter which-path reduction law, and (vi) QMU surface-mode reporting via qsfo/qsfi. The appendix provides SI bridges and explicitly states that numerical anchors are reported using the MKS (SI) version of the QMU conversion tables. Suggested citation Thomson III, D. W. The Double-Slit Experiment in the Aether Physics Model (APM): Transfer Operators, Gate Coherence, and QMU Predictions. DOI: 10.5281/zenodo.18446424 Zenodo (Version 1.0).
This manuscript presents a deterministic boundary-phase model of the double-slit experiment. In this framework, particles follow continuous, definite trajectories while interference arises from structured curvature induced by slit boundary microstructure. The wavefunction is treated as a mathematical representation of a real boundary-generated field rather than a physical matter wave.The model preserves established interference results while introducing a falsifiable experimental prediction: coherent fringe displacement scaling with engineered slit roughness. For a baseline electron configuration (100 eV beam energy, 1 m screen distance, 1 µm slit separation), a measurable 2 µm fringe shift requires a relative phase offset of approximately 0.10 radians, corresponding to the coupling condition β_eff(δ/r) ≈ 0.10.A quantitative δ-sweep prediction is provided along with explicit experimental control requirements necessary to distinguish coherent boundary-phase displacement from conventional scattering or electrostatic effects. If the predicted scaling is observed under controlled conditions, the double-slit paradox can be resolved deterministically without invoking intrinsic randomness or wavefunction collapse.This work is presented as a falsifiable experimental proposal in quantum foundations and electron interferometry.
Standard interpretations of the quantum double-slit experiment rely on non-local wave-function collapse, single-particle self-interference across multiple apertures simultaneously, or retrocausal mechanisms. In this paper, I propose a strictly local, causal thought experiment in which individual quanta propagate as spatially extended, cohesive wavepackets carrying localized forward momentum. In my framework, a single wavepacket traverses only one aperture at a time by undergoing rotational boundary-wall scattering at the slit edges, while transferring its momentum to a single impact point on the detector screen and embedding a temporary spatial phase imprint ("skid mark") into the local quantum surface. Subsequent quanta of identical wavelength absorb and interact with the immediately preceding surface imprint, modifying their peak-and-trough trajectory distribution and overwriting the surface state in a strictly one-by-one sequential (Markovian) relay. Furthermore, I preemptively address key theoretical objections—including special-relativistic speed-of-light constraints, classical momentum transfer mechanics, non-local entanglement signaling paradoxes, planetary motion in local reference frames, and multi-wavelength cross-talk—demonstrating a self-consistent local-realist framework.
Standard interpretations of the quantum double-slit experiment rely on non-local wave-function collapse, single-particle self-interference across multiple apertures simultaneously, or retrocausal mechanisms. In this paper, I propose a strictly local, causal thought experiment in which individual quanta propagate as spatially extended, cohesive wavepackets carrying localized forward momentum. In my framework, a single wavepacket traverses only one aperture at a time by undergoing rotational boundary-wall scattering at the slit edges, while transferring its momentum to a single impact point on the detector screen and embedding a temporary spatial phase imprint ("skid mark") into the local quantum surface. Subsequent quanta of identical wavelength absorb and interact with the immediately preceding surface imprint, modifying their peak-and-trough trajectory distribution and overwriting the surface state in a strictly one-by-one sequential (Markovian) relay. Furthermore, I preemptively address key theoretical objections—including special-relativistic speed-of-light constraints, classical momentum transfer mechanics, non-local entanglement signaling paradoxes, planetary motion in local reference frames, and multi-wavelength cross-talk—demonstrating a self-consistent local-realist framework.