Fresnel propagation of a one-dimensional transverse aperture

B=I, nearly monoenergetic, thin aperture and paraxial approximation; common longitudinal and time phases are suppressed.

Theory · EFFECTIVE MODELEquation version 1.0.0

Based on the final manuscript · Chapter 5

ASD-WEB-QM-019

\psi(L,Y)=\frac1{\sqrt{i\lambda L}}\int_{-\infty}^{\infty}T(y)\psi_{\rm in}(y)\exp\!\left[\frac{ik(Y-y)^2}{2L}\right]dy,\qquad\lambda=2\pi/k

B=I, nearly monoenergetic, thin aperture and paraxial approximation; common longitudinal and time phases are suppressed.
Chapter reference: Ch. 5 (5.3.1)–(5.3.3) · ASD-BOOK-ddbade997b45

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Ch. 5 (5.3.1)–(5.3.3)

B=I, nearly monoenergetic, thin aperture and paraxial approximation; common longitudinal and time phases are suppressed.

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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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QM-0accdcbe7725 · Ch. 5 (5.3.1)–(5.3.3)

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