EQUATION REGISTRY

Above-barrier and threshold checks

qa=nπ gives above-barrier perfect transmission; it is not double-barrier quasibound resonance.

Theory · EFFECTIVE MODELEquation version 1.0.0

Based on the final manuscript · Chapter 5

ASD-WEB-QM-032
E>V0: T=[1+V02sin⁡2(qa)4E(E−V0)]−1, q=2m0(E−V0)/ℏ;E=V0: T=[1+m0V0a22ℏ2]−1E>V_0:\ T=\left[1+\frac{V_0^2\sin^2(qa)}{4E(E-V_0)}\right]^{-1},\ q=\sqrt{2m_0(E-V_0)}/\hbar;\quad E=V_0:\ T=\left[1+\frac{m_0V_0a^2}{2\hbar^2}\right]^{-1}

qa=nπ gives above-barrier perfect transmission; it is not double-barrier quasibound resonance.
Chapter reference: Ch. 5 (5.3.36) and its threshold limit · ASD-BOOK-ddbade997b45

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Ch. 5 (5.3.36) and its threshold limit

qa=nπ gives above-barrier perfect transmission; it is not double-barrier quasibound resonance.

Conditions retained in this adoption

  • Selected channel and stated initial/boundary conditions; action/energy matching retained
  • Continuum, slow-envelope and detector approximations kept at their respective levels

Source locators: p1984 · p1993 · p1995 · p1997 · p2000 · p2008 · p2012

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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QM-0accdcbe7725 · Ch. 5 (5.3.36) and its threshold limit

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