Ray equation for a spatially variable uniaxial crystal and its use in the optical design of liquid-crystal lenses

2007 ◽  
Vol 24 (7) ◽  
pp. 2089 ◽  
Author(s):  
Charles Jenkins ◽  
Richard Bingham ◽  
Kenneth Moore ◽  
Gordon D. Love
2000 ◽  
Author(s):  
Xiling Zhu ◽  
Sheng Wu ◽  
Hai Jing ◽  
Xibin Shao ◽  
Zhihua Ling ◽  
...  

1993 ◽  
Author(s):  
Alan Purvis ◽  
N. J. Bailey ◽  
Gordon D. Love ◽  
John V. Major

Author(s):  
Guglielmo Rossi ◽  
Federico Landini ◽  
Teresa Salvatici ◽  
Marco Romoli ◽  
Maurizio Pancrazzi ◽  
...  

Crystals ◽  
2019 ◽  
Vol 9 (3) ◽  
pp. 122
Author(s):  
Yi-Chin Fang ◽  
Cheng Tsai ◽  
Da-Long Cheng

The main purpose of this paper is to explore a newly developed optical design, then to further improve the overhead lighting contrast in the laser projector module. In terms of the structural design of the projector, a liquid crystal lens array was used as the local dimming system for the light source, in order to achieve the objective, which was to significantly improve the contrast facility of the projection system. Second, in terms of the design of the light source, the output method for the light source was a laser light source employing arrays of micro-scanning. The main purpose was to compensate for the dim spots in the hole between the lenses in each unit of the liquid crystal when the liquid crystal lens array was locally dimmed, and thus significantly improving the contrast facility of the projection system. In terms of the software simulation, a liquid crystal lens array was used to simulate a pore size of 2.0 mm and focal lengths of 9 cm and 23 cm. The end effect gave good control and adjustment of the bright and dark areas during local dimming of the projector’s imaging chip components. For a single laser source, the maximum contrast for local dimming was about 128:1, 438:1, and 244:1, for the Red (R), Green (G), and Blue (B) optical paths, respectively. The light efficiency scores were approximately 20.91%, 20.05%, and 24.45%, for the R, G, and B optical paths, respectively. After compensation using a micro-scanning light source, the defect of having dim spots between the pores was remedied, and the light adjustment area became more uniform while the contrasts became smaller. The maximum contrasts were approximately 52:1, 122:1, and 110:1, for the R, G, and B optical paths, respectively. For the projector, when the liquid crystal lenses were not transmissive, the maximum uniformity scores were 82.25%, 87.15%, and 88.43%, for the R, G, and B optical paths, respectively.


2008 ◽  
Vol 41 (11) ◽  
pp. 115101 ◽  
Author(s):  
Kyung-Mi Kim ◽  
Seung-Hoon Ji ◽  
Joun-Ho Lee ◽  
Seung Hee Lee ◽  
Gi-Dong Lee

2009 ◽  
Vol 42 (5) ◽  
pp. 878-884 ◽  
Author(s):  
Leonas Dumitrascu ◽  
Irina Dumitrascu ◽  
Dana Ortansa Dorohoi

This paper presents a simplified data acquisition and analysis technique for use in determining the main refractive indices and thickness of a uniaxial anisotropic layer cut out parallel to the optical axis, by processing the conoscopic interference figures obtained using a polarizing microscope equipped with a CCD camera. For negative uniaxial crystals, the equations used permit the calculation of the optical sign of the studied material so it is not necessary to insert a quartz wedge into the conoscopic beam. The technique can also be applied to the study of liquid crystal layers in a planar orientation.


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