Quantum Tunneling vs. QFT Impossible Measurement: Distinct Nonlocal Issues — E8 Intelligence Research

FINDING: Quantum tunneling is a wave-mechanical transmission problem through a classically forbidden potential barrier, and the "impossible measurement" problem in QFT is a nonlocal joint-measurement consistency issue, not a transport phenomenon. | MATH: For a rectangular barrier of height V₀ > E and width a, the transmission coefficient in the thick-barrier (WKB) limit is T ≈ 16(E/V₀)(1−E/V₀)·exp(−2κa), where κ = √(2m(V₀−E))/ħ. The exact result comes from matching plane waves across the barrier: T = [1 + (V₀² sinh²(κa))/(4E(V₀−E))]⁻¹. Inside the barrier the wavefunction is ψ(x) ∝ e^(−κx) (evanescent decay, no oscillation). The "impossible measurement" paper (arXiv:2311.13644v2) concerns nonlocal joint measurements in QFT producing superluminal signaling if naively defined — a consistency constraint, not a tunneling rate. | CONNECTION: No geometric-harmony constants (0.382, 0.618, 0.786, 1.618, 2.618) appear in the tunneling equations. The only structural ratios are E/V₀ (energy fracti Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-29
DOI
https://doi.org/10.5281/zenodo.23755754
Primary Topic
Quantum Mechanics and Applications
Type
preprint
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Quantum Tunneling vs. QFT Impossible Measurement: Distinct Nonlocal Issues — E8 Intelligence Research

Andrew Stewart Caldin
10 links
Zenodo (CERN European Organization for Nuclear Research)
Quantum Mechanics and Applications
preprint

Quantum Tunneling vs. QFT Impossible Measurement: Distinct Nonlocal Issues — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Quantum tunneling is a wave-mechanical transmission problem through a classically forbidden potential barrier, and the "impossible measurement" problem in QFT is a nonlocal joint-measurement consistency issue, not a transport phenomenon. | MATH: For a rectangular barrier of height V₀ > E and width a, the transmission coefficient in the thick-barrier (WKB) limit is T ≈ 16(E/V₀)(1−E/V₀)·exp(−2κa), where κ = √(2m(V₀−E))/ħ. The exact result comes from matching plane waves across the barrier: T = [1 + (V₀² sinh²(κa))/(4E(V₀−E))]⁻¹. Inside the barrier the wavefunction is ψ(x) ∝ e^(−κx) (evanescent decay, no oscillation). The "impossible measurement" paper (arXiv:2311.13644v2) concerns nonlocal joint measurements in QFT producing superluminal signaling if naively defined — a consistency constraint, not a tunneling rate. | CONNECTION: No geometric-harmony constants (0.382, 0.618, 0.786, 1.618, 2.618) appear in the tunneling equations. The only structural ratios are E/V₀ (energy fracti Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Quantum Mechanics and Applications
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