Optics, electromagnetic theory Wave optics and diffraction Object
Airy disk
Builds on Fraunhofer diffractionBessel function of the first kind
Description
Let a plane monochromatic wave of wavelength and wavenumber fall normally on a circular aperture of radius . Let be the Bessel function of the first kind of order , and let be the intensity on the axis. In the Fraunhofer regime, the intensity at angle from the axis is The pattern is a bright central disk surrounded by fainter rings. The Airy disk is the central bright disk, bounded by the first dark ring. This ring lies at the first positive zero of , that is, at
Remarks
The formula comes from the Fourier transform of the indicator function of a disk: in polar coordinates its angular integral gives , and . Since as , the expression is normalised so that . About of the light lies inside the Airy disk. The size of the Airy disk sets the resolving power of a telescope or microscope with a circular aperture. In the Rayleigh criterion, two point sources are just resolved when the centre of one Airy pattern falls on the first dark ring of the other.
Reading path
To understand this page from the ground up, read these 14 pages in order. The foundations come first.
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- no evidence level
- Bessel function of the first kind concept
- Fourier transform concept
- Green's function concept
- Helmholtz equation concept
- Paraxial approximation concept
- Refractive index concept
- Wave equation concept
- Physical optics definition
- Fresnel number definition
- Kirchhoff's diffraction formula statement
- Rayleigh–Sommerfeld diffraction statement
- Fresnel diffraction definition
- Fraunhofer diffraction definition
- Airy disk object
Where this leads
1 page builds on this one.
Further reading
About this page
| Tag | DB435TBQJT |
|---|---|
| URI | m2://DB435TBQJT |
| Kind | object |
| Writing | W0 stub |
| MSC | 78A45, 33C10 |
| Uses | Fraunhofer diffraction, Bessel function of the first kind |
| Same as | |
| Changed | 3 November 2026 |
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