Extended gapped branch required for an envelope
Final equation 5.1.22 is the dispersion equality of the selected second-order gapped continuum channel. ka₀≪1 limits microscopic applicability; higher lattice terms are separate. B is real symmetric positive definite.
Based on the final manuscript · Chapter 5
Final equation 5.1.22 is the dispersion equality of the selected second-order gapped continuum channel. ka₀≪1 limits microscopic applicability; higher lattice terms are separate. B is real symmetric positive definite.
Chapter reference: Ch. 5 (5.1.22) · ASD-BOOK-ddbade997b45
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Ch. 5 (5.1.22)
Final equation 5.1.22 is the dispersion equality of the selected second-order gapped continuum channel. ka₀≪1 limits microscopic applicability; higher lattice terms are separate. B is real symmetric positive definite.
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: p1770 · p1803 · p1826 · p1833 · p1837 · p1841
Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e
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Previous source, retained as history
QM-0accdcbe7725 · Ch. 5 (5.1.22)
Dependencies
No preceding equation is recorded in this index. Consult the source topic for definitions, geometry and model scope.
Uses of this equation
Subsequent equationConditional second-order channel equationASD-WEB-QM-011Subsequent equationTruncation error in a uniform source-free limitASD-WEB-QM-016DocumentHow Does a Spatial Field Yield an Effective Wave Equation?