Math 2.0

Optics, electromagnetic theory Definition

Seidel aberrations

Builds on Optical aberrationParaxial approximation

Definition

Consider an optical system that is rotationally symmetric about its axis. Let hh be the normalised height of the object point above the axis. Let (ρ,θ)(\rho, \theta) be normalised polar coordinates in the exit pupil, with θ\theta measured from the direction of hh. By the symmetry, the wave aberration WW is a function of h2h^2, ρ2\rho^2 and hρcos⁡θh \rho \cos\theta, and it has an expansion W=∑Wklm hkρlcos⁡mθ.W = \sum W_{klm} \, h^k \rho^l \cos^m \theta . The terms of total degree k+l=4k + l = 4 are the primary or Seidel aberrations:

  1. spherical aberration W040ρ4W_{040} \rho^4;
  2. coma W131hρ3cos⁡θW_{131} h \rho^3 \cos\theta;
  3. astigmatism W222h2ρ2cos⁡2θW_{222} h^2 \rho^2 \cos^2\theta;
  4. field curvature W220h2ρ2W_{220} h^2 \rho^2;
  5. distortion W311h3ρcos⁡θW_{311} h^3 \rho \cos\theta.

Remarks

The terms of degree 22 are a change of focus W020ρ2W_{020}\rho^2 and a tilt W111hρcos⁡θW_{111} h\rho\cos\theta. They only move the ideal image, so they are not counted as aberrations of the image quality. A spherical mirror imaging a point on its axis has only spherical aberration among the five, since h=0h = 0 kills the other four terms. A system with only a distortion term W311W_{311} forms sharp images, so distortion is an aberration of position, not of sharpness. In terms of ray aberrations the Seidel terms are of third order in the aperture and field, so they are also called third-order aberrations. The coefficients are often written as the Seidel sums SI,…,SVS_{\mathrm{I}}, \dots, S_{\mathrm{V}}, computed surface by surface from paraxial ray data.

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  1. Optical aberration concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Optical_aberration
About this page
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Kinddefinition
WritingW0 stub
MSC78A05
DefinesSeidel aberrations
UsesOptical aberration, Paraxial approximation
Changed3 November 2026

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