Quantum tunneling as evanescent wavefunction decay, not classical pass-through — E8 Intelligence Research

FINDING: Quantum tunneling is the exponential attenuation of a wavefunction through a classically forbidden barrier; transmission is governed by an evanescent decay, not a classical "pass-through." MATH: - Time-independent Schrödinger: −(ħ²/2m)ψ″ + V(x)ψ = Eψ - Rectangular barrier (E < V₀), transmission: T ≈ 16(E/V₀)(1−E/V₀)·e^(−2κa), where κ = √(2m(V₀−E))/ħ - Decay length: 1/κ = ħ/√(2m(V₀−E)); WKB general form: T ≈ exp(−2∫√(2m(V(x)−E))/ħ dx) - Resonant (E > V₀) transmission peaks at k·a = nπ (Fabry–Pérot-like standing-wave condition) CONNECTION: The exponential decay e^(−2κa) is a pure geometric-scaling law — transmission is multiplicatively invariant under barrier-width translation (T(a+a′) = T(a)·T(a′)/T(0)), i.e. a log-linear (additive-in-exponent) structure. Resonant peaks sit at integer multiples of π in phase (k·a = nπ), a base-π lattice condition analogous to standing-wave/root-system quantization. No direct 0.618/1.618 ratio appears in the tunneling coefficient itself; the go Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-01
DOI
https://doi.org/10.5281/zenodo.23853391
Primary Topic
Quantum Mechanics and Applications
Type
preprint
Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
preprint

Quantum tunneling as evanescent wavefunction decay, not classical pass-through — E8 Intelligence Research

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

Quantum tunneling as evanescent wavefunction decay, not classical pass-through — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Quantum tunneling is the exponential attenuation of a wavefunction through a classically forbidden barrier; transmission is governed by an evanescent decay, not a classical "pass-through." MATH: - Time-independent Schrödinger: −(ħ²/2m)ψ″ + V(x)ψ = Eψ - Rectangular barrier (E < V₀), transmission: T ≈ 16(E/V₀)(1−E/V₀)·e^(−2κa), where κ = √(2m(V₀−E))/ħ - Decay length: 1/κ = ħ/√(2m(V₀−E)); WKB general form: T ≈ exp(−2∫√(2m(V(x)−E))/ħ dx) - Resonant (E > V₀) transmission peaks at k·a = nπ (Fabry–Pérot-like standing-wave condition) CONNECTION: The exponential decay e^(−2κa) is a pure geometric-scaling law — transmission is multiplicatively invariant under barrier-width translation (T(a+a′) = T(a)·T(a′)/T(0)), i.e. a log-linear (additive-in-exponent) structure. Resonant peaks sit at integer multiples of π in phase (k·a = nπ), a base-π lattice condition analogous to standing-wave/root-system quantization. No direct 0.618/1.618 ratio appears in the tunneling coefficient itself; the go 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
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.

Laika access coming soon