Description of gradient-index crystalline lens by a first-order optical system

2005 ◽  
Vol 7 (3) ◽  
pp. 103-110 ◽  
Author(s):  
M V Pérez ◽  
C Bao ◽  
M T Flores-Arias ◽  
M A Rama ◽  
C Gómez-Reino
2012 ◽  
Vol 71 (2) ◽  
Author(s):  
W. F. Harris

The ray transference is central to the understanding of the first-order optical character of an optical system including the visual optical system of the eye.  It can be calculated for dioptric and catadioptric systems from a knowledge of curvatures, tilts and spacing of surfaces in the system provided the material between successive surfaces has a uniform index of refraction.  However the index of the natural lens of the eye is not uniform but varies with position.  There is a need, therefore, for a method of calculating the transference of systems containing such gradient-index elements.  As a first step this paper shows that the transference of elements in which the index varies radially can be obtained directly from published formulae.  The transferences of radial-gradient systems are examined.  Expressions are derived for several properties including the power, the front- and back-surface powers and the locations of the cardinal points.  Equations are obtained for rays through such systems and for the locations of images of object points through them.  Numerical examples are presented in the appen-dix. (S Afr Optom 2012 71(2) 57-63)


2009 ◽  
Vol 11 (12) ◽  
pp. 125301
Author(s):  
M T Flores-Arias ◽  
A Díaz del Rio ◽  
C Bao-Varela ◽  
M V Pérez ◽  
C Gómez-Reino

2017 ◽  
Vol 66 (4) ◽  
pp. 044201
Author(s):  
Tan Nai-Yue ◽  
Xu Zhong-Jie ◽  
Wei Ke ◽  
Zhang Yue ◽  
Wang Rui

2020 ◽  
Vol 49 (1) ◽  
pp. 111001-111001
Author(s):  
姜东旭 Dong-xu JIANG ◽  
孙宝玉 Bao-yu SUN ◽  
李迎春 Ying-chun LI ◽  
林洁琼 Jie-qiong LIN ◽  
王冬雪 Dong-xue WANG ◽  
...  

1. The object of this investigation is to establish a formula for the longitudinal spherical aberration of rays which traverse a symmetrical optical system in an axial plane that shall be capable of fairly easy computation for any combination of lenses, and at the same time shall be accurate to the second order and free from certain important difficulties of convergency which occur in certain neighbourhoods when we attempt to use for the longitudinal aberration the method of aberration of successive orders. From the point of view of the optical designer, the usual theory of aberrations, which, for all practical purposes, is largely restricted to the first order, is known to give an unsatisfactory approximation. In practice, the designer adopts a semi-empirical method of tracing a number of rays through the system by means of the trigonometrical equations, a method which is laborious and lengthy, and which can at best give only incomplete informa­tion and very limited guidance for effecting improvements.


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