Fresnel Diffraction
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Fresnel diffraction (also called near-field diffraction) is the diffraction pattern observed when the source or observation screen is at a finite distance from the diffracting aperture.
Fresnel Approximation
The Fresnel approximation uses a quadratic phase approximation:
$$ \gamma_z \approx 1 - \frac{1}{2}(\gamma_x^2 + \gamma_y^2) $$valid when $\gamma_x \ll 1$ and $\gamma_y \ll 1$ (small angles).
Fresnel Condition
The Fresnel approximation is valid when:
$$ z \ll \frac{a^4}{\lambda^3} $$where $z$ is the propagation distance, $a$ is the aperture size, and $\lambda$ is the wavelength.
Key Properties
- Pattern changes shape with propagation distance
- More complex than Fraunhofer diffraction
- Involves Fresnel integrals or quadratic phase factors
Related Topics
- Fraunhofer diffraction (far-field limit)
- Fresnel zones
- Fresnel zone plate