Envelope boundary problem for a rectangular barrier
0<E<V₀, equal masses, B=I and barrier width a; ψ and ψ′ are continuous across finite steps.
Based on the final manuscript · Chapter 5
0<E<V₀, equal masses, B=I and barrier width a; ψ and ψ′ are continuous across finite steps.
Chapter reference: Ch. 5 (5.3.28)–(5.3.31) · ASD-BOOK-ddbade997b45
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Ch. 5 (5.3.28)–(5.3.31)
0<E<V₀, equal masses, B=I and barrier width a; ψ and ψ′ are continuous across finite steps.
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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Previous source, retained as history
QM-0accdcbe7725 · Ch. 5 (5.3.28)–(5.3.31)
Dependencies
algebraSchrödinger-type effective envelopeASD-WEB-QM-015Uses of this equation
Subsequent equationBarrier transmission coefficient and conserved fluxASD-WEB-QM-031Subsequent equationWKB structure in a variable-coefficient forbidden regionASD-WEB-QM-033DocumentTunneling: Effective Transmission and Core Transport