FINDING: Quantum tunneling is a wave-mechanical penetration of finite barriers, not a classical "jump"; recent QFT work shows "impossible" nonlocal measurements are possible but non-ideal, revealing a fundamental trade-off in measurement theory. | MATH: Transmission coefficient \(T ≈ e-2κ L\), \(κ = √2m(V_0-E)/\); for a rectangular barrier, \(T = [1 + V_0^2 ^2(κ L)/4E(V_0-E)]⁻¹\). In QFT, the "impossible measurement" problem is resolved by recognizing that ideal projective measurements violate microcausality; the trade-off is quantified by a non-ideal measurement parameter \(ε\) such that signaling error \(∝ ε^2\), with \(ε → 0\) only in the non-relativistic limit. | CONNECTION: The exponential decay \(e-2κ L\) is a pure decay constant — no golden ratio appears in the standard barrier solution. However, the *critical* barrier width where tunneling probability drops to \(1/φ\) (≈0.618) occurs at \ Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
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