OP-QM-005 · Core–Field Coupling in Tunneling
For a one-dimensional stationary rectangular barrier with identical propagation parameters on both sides, the exact envelope boundary solution is established: the hyperbolic transmission form equals its exponential rational form, and reflection plus transmission equals one. A variable-coefficient barrier has a divergence-form equation, amplitude transport and first-order WKB expression. These solve specified effective-envelope propagation problems.
Based on the final manuscript · 第五章
NEEDS THEORY · Needs theory
Discuss this task01Established results
For a one-dimensional stationary rectangular barrier with identical propagation parameters on both sides, the exact envelope boundary solution is established: the hyperbolic transmission form equals its exponential rational form, and reflection plus transmission equals one. A variable-coefficient barrier has a divergence-form equation, amplitude transport and first-order WKB expression. These solve specified effective-envelope propagation problems.
Mathematical result
Exact boundary solution for equal exterior parameters, real potential and 0<E<V₀. z,D abbreviate 5.3.34; Rrefl is reflectance, not core radius. Complex exponential superposition carries flux.
Chapter reference: Ch. 5 (5.3.32)–(5.3.35) · ASD-BOOK-ddbade997b45
02Research still required
Evolve the finite core, accompanying field, barrier material and back reaction from one action. Track topology and energy exchange and compare core-crossing probability with the envelope flux ratio. Return to the second-order hyperbolic equation for rapidly changing boundaries; retain WKB slow-variation conditions and turning-point connections for variable barriers.
03The next reproducible deliverable
Deliver a joint initial-boundary evolution for a specified barrier, including conservation residuals, grid/boundary convergence, the model basis of core trajectories and statistical initial conditions. Reproduce the exact rectangular result and threshold limit before reporting departures from the effective description.
04Scope and research links
An equality defining a WKB expression does not make the true transmission of every barrier exact; nonzero evanescent-envelope flux alone does not prove nonlinear-core crossing.
tunneling · accompanying field · detection statistics · tunneling · accompanying field · detection statistics · quantum
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Adopted source, conditions and previous versions
第五章 §3.7—§3.9 式(5.3.28)—(5.3.39)
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Conditions retained in this adoption
- An equality defining a WKB expression does not make the true transmission of every barrier exact; nonzero evanescent-envelope flux alone does not prove nonlinear-core crossing.
Source locators: p1983 · p1988 · p1993 · p1995 · p1998 · p2000 · p2008 · p2009
Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e
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Previous source, retained as history
QM-0accdcbe7725 · Ch. 5 §§3.7–3.9
CH5-ca737ec4e327 · 第五章-出版整理稿.docxca737ec4e327d72c5507bbc8e00295b6e56029c7583ebad8e505cdb9c68c6262
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Revision history
第五章 · 第五章 §3.7—§3.9 式(5.3.28)—(5.3.39)
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Knowledge scopeASD: OP-QM-005 · Core–Field Coupling in Tunneling. OP-QM-005-EN. Version 1.0.0; 2026-10-24. https://asd-physics.org/en/open-problems/quantum/tunneling-core-coupling. 第五章 §3.7—§3.9 式(5.3.28)—(5.3.39). Source ASD-BOOK-ddbade997b45.
Continue with the assumptions, equations and sources.
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