Relative far-field intensity of two rectangular slits
a is slit width and d separation; coherent uniform illumination and D²/(λL)≪1. Web φ replaces manuscript observation angle θ, not wave phases; paraxial spacing remains approximate.
Based on the final manuscript · Chapter 5
a is slit width and d separation; coherent uniform illumination and D²/(λL)≪1. Web φ replaces manuscript observation angle θ, not wave phases; paraxial spacing remains approximate.
Chapter reference: Ch. 5 (5.3.4)–(5.3.6) · ASD-BOOK-ddbade997b45
Source and ID
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Return to premises and derivationAdopted source, conditions and previous versions
Ch. 5 (5.3.4)–(5.3.6)
a is slit width and d separation; coherent uniform illumination and D²/(λL)≪1. Web φ replaces manuscript observation angle θ, not wave phases; paraxial spacing remains approximate.
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: p1909 · p1918 · p1927 · p1933 · p1945
Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e
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Previous source, retained as history
QM-0accdcbe7725 · Ch. 5 (5.3.4)–(5.3.6)
Dependencies
algebraFresnel propagation of a one-dimensional transverse apertureASD-WEB-QM-019