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The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems

The ray-aberrations in axis-symmetrical systems are conventionally derived from wavefront functions or characteristic functions using classical approximate partial derivatives. However, the resulting aberrations typically have fifth-order errors, as described by Restrepo et al. (2017) [1]. According...

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Autor principal: Lin, Psang Dain
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Elsevier 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9474841/
https://www.ncbi.nlm.nih.gov/pubmed/36119862
http://dx.doi.org/10.1016/j.heliyon.2022.e10531
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author Lin, Psang Dain
author_facet Lin, Psang Dain
author_sort Lin, Psang Dain
collection PubMed
description The ray-aberrations in axis-symmetrical systems are conventionally derived from wavefront functions or characteristic functions using classical approximate partial derivatives. However, the resulting aberrations typically have fifth-order errors, as described by Restrepo et al. (2017) [1]. Accordingly, in the present study, the secondary ray-aberration coefficients for object placed at finite distance are determined using the fifth-order Taylor series expansion of a skew ray. Notably, the derived expressions are exact since they are determined without any approximations. It is found that some of the aberration coefficients are not constants, but are functions of the polar angle of the entrance pupil. It is additionally found that, once the required derivative matrices have been generated, determination of the secondary aberration coefficients is straightforward without iteration, and incurs only a low computational cost.
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spelling pubmed-94748412022-09-16 The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems Lin, Psang Dain Heliyon Research Article The ray-aberrations in axis-symmetrical systems are conventionally derived from wavefront functions or characteristic functions using classical approximate partial derivatives. However, the resulting aberrations typically have fifth-order errors, as described by Restrepo et al. (2017) [1]. Accordingly, in the present study, the secondary ray-aberration coefficients for object placed at finite distance are determined using the fifth-order Taylor series expansion of a skew ray. Notably, the derived expressions are exact since they are determined without any approximations. It is found that some of the aberration coefficients are not constants, but are functions of the polar angle of the entrance pupil. It is additionally found that, once the required derivative matrices have been generated, determination of the secondary aberration coefficients is straightforward without iteration, and incurs only a low computational cost. Elsevier 2022-09-06 /pmc/articles/PMC9474841/ /pubmed/36119862 http://dx.doi.org/10.1016/j.heliyon.2022.e10531 Text en © 2022 The Author(s) https://creativecommons.org/licenses/by-nc-nd/4.0/This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Research Article
Lin, Psang Dain
The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems
title The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems
title_full The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems
title_fullStr The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems
title_full_unstemmed The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems
title_short The determination of secondary ray-aberration coefficients for axis-symmetrical optical systems
title_sort determination of secondary ray-aberration coefficients for axis-symmetrical optical systems
topic Research Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9474841/
https://www.ncbi.nlm.nih.gov/pubmed/36119862
http://dx.doi.org/10.1016/j.heliyon.2022.e10531
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