Simulation of Corneal imaging properties for near objects

Purpose: Using raytracing simulation to study the effect of corneal imaging metrics for different aperture sizes as a function of object distances with different schematic model eyes. Methods: This raytracing simulation determined the best focus (with the least root-mean-square (rms) ray scatter) an...

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Bibliographic Details
Main Authors: Cayless, A. (Author), Eppig, T. (Author), Gatzioufas, Z. (Author), Hoffmann, P. (Author), Langenbucher, A. (Author), Szentmáry, N. (Author), Wendelstein, J. (Author)
Format: Article
Language:English
Published: John Wiley and Sons Inc 2021
Subjects:
Online Access:View Fulltext in Publisher
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008 220427s2021 CNT 000 0 und d
020 |a 02755408 (ISSN) 
245 1 0 |a Simulation of Corneal imaging properties for near objects 
260 0 |b John Wiley and Sons Inc  |c 2021 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1111/opo.12861 
520 3 |a Purpose: Using raytracing simulation to study the effect of corneal imaging metrics for different aperture sizes as a function of object distances with different schematic model eyes. Methods: This raytracing simulation determined the best focus (with the least root-mean-square (rms) ray scatter) and the best wavefront focus (with least rms wavefront error) for four schematic model eyes (Liou-Brennan (LBME), Atchison (ATCHME), Gullstrand (GULLME) and Navarro (NAVME)) with 4 aperture sizes (2–5 mm) and 30 object distances in a logscale from 10 cm to 10 m plus infinity. For each configuration, 10,000 rays were traced through the cornea, and the aperture stop was located at the lens front apex plane as described in the model eyes. The wavefront was decomposed into Zernike components to extract the spherical aberration term. Results: The focal distance with respect to the corneal front apex increases from around 31 mm for objects at infinity to around 40 mm for objects at 10 cm. The best (wavefront) focus was systematically closer to the cornea compared with the paraxial focus, and the overestimation of focal length with the paraxial focus was larger for large aperture sizes and small object distances. The rms ray scatter and wavefront error were both systematically larger with large aperture and small object sizes. At best focus the rms wavefront error was systematically larger, and the rms ray scatter was systematically smaller compared to the best wavefront focus. Spherical aberration varied more with GULLME than with LBME or NAVME, and increased strongly at smaller object distances. Conclusions: The imaging properties of the cornea, especially spherical aberration, increase strongly as the object distance decreases. This effect should be considered, especially when considering aberration correcting lenses for near vision such as multifocal or enhanced depth of focus lenses. © 2021 The Authors. Ophthalmic and Physiological Optics published by John Wiley & Sons Ltd on behalf of College of Optometrists 
650 0 4 |a article 
650 0 4 |a best focus 
650 0 4 |a computer simulation 
650 0 4 |a Computer Simulation 
650 0 4 |a cornea 
650 0 4 |a cornea 
650 0 4 |a Cornea 
650 0 4 |a corneal imaging properties 
650 0 4 |a Corneal Topography 
650 0 4 |a corneal wavefront aberration 
650 0 4 |a Corneal Wavefront Aberration 
650 0 4 |a decomposition 
650 0 4 |a diagnostic imaging 
650 0 4 |a eye refraction 
650 0 4 |a human 
650 0 4 |a Humans 
650 0 4 |a keratometry 
650 0 4 |a lens 
650 0 4 |a Lens, Crystalline 
650 0 4 |a myopia 
650 0 4 |a Myopia 
650 0 4 |a near vision 
650 0 4 |a Refraction, Ocular 
650 0 4 |a simulation 
650 0 4 |a spherical aberration model eye 
650 0 4 |a vision 
650 0 4 |a wavefront aberration 
700 1 |a Cayless, A.  |e author 
700 1 |a Eppig, T.  |e author 
700 1 |a Gatzioufas, Z.  |e author 
700 1 |a Hoffmann, P.  |e author 
700 1 |a Langenbucher, A.  |e author 
700 1 |a Szentmáry, N.  |e author 
700 1 |a Wendelstein, J.  |e author 
773 |t Ophthalmic and Physiological Optics