A Microlens Array on Curved Substrates by 3D Micro Projection and Reflow Process

Author(s):  
Hao Zhang ◽  
Lei Li ◽  
David L. McCray ◽  
Donggang Yao ◽  
Allen Y. Yi

Microlens arrays are becoming increasingly important because of their widespread applications in optical, electronic, and energy fields. Currently, microlens array fabrication processes are mainly developed on planar substrates. For nonplanar substrates, existing fabrication methods suffer from various disadvantages. This is largely due to the inherent technical complexity of 3D microstructure fabrication processes. In this work, an innovative 3D fabrication method for microlens arrays on curved surfaces is introduced. To fabricate the microlens array, a PMMA microlens array on a curved surface was used as the projection microlens array. A thick layer of positive tone photoresist SPR 220 was spin coated on a curved, titanium-coated aluminum substrate. A pre-designed pattern was projected onto the photoresist by using a home built exposure system. The development process resulted in micro cylinders on the curved substrate. A thermal reflow process was then performed on the cylinder array, forming a microlens array. Experiments were conducted to evaluate the factors that affect the shapes of the microlenses. These factors include film thickness variation, exposure and development variation, slope of the substrate, height to width ratio and heating time in thermal reflow process. Finally microlenses were tested by using a Twyman-Green interferometer.

2004 ◽  
Vol 14 (8) ◽  
pp. 1197-1204 ◽  
Author(s):  
Hsiharng Yang ◽  
Ching-Kong Chao ◽  
Mau-Kuo Wei ◽  
Che-Ping Lin

2019 ◽  
Vol 27 (3) ◽  
pp. 3439 ◽  
Author(s):  
S. G. Heo ◽  
D. Jang ◽  
H.-J. Koo ◽  
H. Yoon

2014 ◽  
Vol 38 (1) ◽  
pp. 85-92 ◽  
Author(s):  
Tsung-Hung Lin ◽  
Shih-Yu Hung ◽  
Chien-Hsin Hung ◽  
Ming-Ho Shen ◽  
Ching-Kong Chao ◽  
...  

Author(s):  
Yang Chen ◽  
Allen Y. Yi ◽  
Donggan Yao ◽  
Fritz Klocke ◽  
Guido Pongs

This fabrication process includes three major steps, i.e., fabrication of glassy carbon molds with arrays of micro size holes, glass compression molding to create micro cylinders on glass substrate, and reheating to form microlens arrays. As compared to traditional polymer microlens arrays, glass microlens arrays are more reliable and therefore could be used in more critical applications. In this research, microlens arrays with different surface geometries were successfully fabricated on P-SK57 (Tg = 493 °C) glass substrate using a combination of compression molding and thermal reflow process. The major parameters that influence the final lens shape, including reheating temperature and holding time, were studied to establish a suitable fabrication process. A numerical simulation method was developed to evaluate the fabrication process.


2003 ◽  
Vol 13 (5) ◽  
pp. 775-781 ◽  
Author(s):  
Che-Ping Lin ◽  
Hsiharng Yang ◽  
Ching-Kong Chao

2009 ◽  
Vol 86 (11) ◽  
pp. 2255-2261 ◽  
Author(s):  
E. Roy ◽  
B. Voisin ◽  
J.-F. Gravel ◽  
R. Peytavi ◽  
D. Boudreau ◽  
...  

Author(s):  
Jhy-Cherng Tsai ◽  
Yong-Sung Hsu

Microlens and its mold fabricated by thermal reflow using photoresist have been widely used for forming patterns in different scales. When the photoresist solidifies from melting condition, for example by the reflow process, its profile is formed based on the balance between surface tension and gravity. This research is aimed to investigate the influence of surface tension and gravity on the profile of microlens in thermal reflow process. Theoretical analysis based on the interaction between surface tension and gravity of liquid droplet is first investigated. The result showed that the height to diameter ratio (h/D), or the sag ratio, of the liquid droplet is affected by the Bond number (Bo), a number defined as the ratio of gravity to surface tension. The sag ratio is not sensitive to Bo when Bo is small but the ratio decreases as Bo increases if Bo is over the critical number. Based on the analysis, the critical number for the AZ4620 photoresist on a silicon substrate is 1, corresponding to the critical radius of droplet R = 2,500μm. When the size of the droplet is less then the critical size, the profile is mainly controlled by the surface tension and thus the sag ratio is about the same regardless the size. The profile, in contrast, is highly affected by the gravity if the size of the droplet is larger then the critical size. The sag ratio decreases exponentially with respect to Bo in this case. Experiments are also designed and conducted to verify the analysis. Experimental result showed that the sag ratio of the photoresist reduces to 0.065 from 0.095 when Bo increases from 0.0048 to 0.192. The results showed that the trend is consistent to the theoretical model.


2012 ◽  
Vol 179 ◽  
pp. 242-250 ◽  
Author(s):  
Hao Zhang ◽  
Lei Li ◽  
David L. McCray ◽  
Donggang Yao ◽  
Allen Y. Yi

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