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dc.contributor.authorDíaz, José Antonio
dc.contributor.authorMahajan, Virendra N.
dc.date.accessioned2018-01-31T18:58:06Z
dc.date.available2018-01-31T18:58:06Z
dc.date.issued2017-08-23
dc.identifier.citationJosé Antonio Díaz, Virendra N. Mahajan, "Diffraction and geometrical optical transfer functions: calculation time comparison", Proc. SPIE 10375, Current Developments in Lens Design and Optical Engineering XVIII, 103750D (23 August 2017); doi: 10.1117/12.2275377; http://dx.doi.org/10.1117/12.2275377en
dc.identifier.issn0277-786X
dc.identifier.doi10.1117/12.2275377
dc.identifier.urihttp://hdl.handle.net/10150/626488
dc.description.abstractIn a recent paper, we compared the diffraction and geometrical optical transfer functions (OTFs) of an optical imaging system, and showed that the GOTF approximates the DOTF within 10% when a primary aberration is about two waves or larger [Appl. Opt., 55, 3241-3250 (2016)]. In this paper, we determine and compare the times to calculate the DOTF by autocorrelation or digital autocorrelation of the pupil function, and by a Fourier transform (FT) of the point-spread function (PSF); and the GOTF by a FT of the geometrical PSF and its approximation, the spot diagram. Our starting point for calculating the DOTF is the wave aberrations of the system in its pupil plane, and the ray aberrations in the image plane for the GOTF. The numerical results for primary aberrations and a typical imaging system show that the direct integrations are slow, but the calculation of the DOTF by a FT of the PSF is generally faster than the GOTF calculation by a FT of the spot diagram.
dc.language.isoenen
dc.publisherSPIE-INT SOC OPTICAL ENGINEERINGen
dc.relation.urlhttps://www.spiedigitallibrary.org/conference-proceedings-of-spie/10375/2275377/Diffraction-and-geometrical-optical-transfer-functions-calculation-time-comparison/10.1117/12.2275377.fullen
dc.rights© 2017 SPIE.en
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/
dc.subjectOptical transfer functionen
dc.subjectaberrationsen
dc.subjectgeometrical OTFen
dc.subjectdiffraction OTFen
dc.subjectimagingen
dc.titleDiffraction and geometrical optical transfer functions: calculation time comparisonen
dc.typeArticleen
dc.identifier.eissn1996-756X
dc.contributor.departmentUniv Arizona, Coll Opt Scien
dc.identifier.journalCURRENT DEVELOPMENTS IN LENS DESIGN AND OPTICAL ENGINEERING XVIIIen
dc.description.collectioninformationThis item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.en
dc.eprint.versionFinal published versionen
refterms.dateFOA2018-09-12T01:11:07Z
html.description.abstractIn a recent paper, we compared the diffraction and geometrical optical transfer functions (OTFs) of an optical imaging system, and showed that the GOTF approximates the DOTF within 10% when a primary aberration is about two waves or larger [Appl. Opt., 55, 3241-3250 (2016)]. In this paper, we determine and compare the times to calculate the DOTF by autocorrelation or digital autocorrelation of the pupil function, and by a Fourier transform (FT) of the point-spread function (PSF); and the GOTF by a FT of the geometrical PSF and its approximation, the spot diagram. Our starting point for calculating the DOTF is the wave aberrations of the system in its pupil plane, and the ray aberrations in the image plane for the GOTF. The numerical results for primary aberrations and a typical imaging system show that the direct integrations are slow, but the calculation of the DOTF by a FT of the PSF is generally faster than the GOTF calculation by a FT of the spot diagram.


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