A surface-emitting laser array with backside guiding holes for passive alignment to parallel optical fibers

1996 ◽  
Vol 8 (4) ◽  
pp. 494-496 ◽  
Author(s):  
K. Matsuda ◽  
T. Yoshida ◽  
T. Kobayashi ◽  
T. Chino
1997 ◽  
Vol 36 (Part 1, No. 3B) ◽  
pp. 1872-1875 ◽  
Author(s):  
Yasuhiro Kobayashi ◽  
Kenichi Matsuda ◽  
Toyoji Chino ◽  
Takayuki Yoshida ◽  
Kenzo Hatada

2011 ◽  
Vol 4 (5) ◽  
pp. 052104 ◽  
Author(s):  
Di Liu ◽  
Yongqiang Ning ◽  
Yugang Zeng ◽  
Li Qin ◽  
Yun Liu ◽  
...  

2018 ◽  
Vol 38 (5) ◽  
pp. 0514001
Author(s):  
吕朝晨 Lü Zhaochen ◽  
王青 Wang Qing ◽  
尧舜 Yao Shun ◽  
周广正 Zhou Guangzheng ◽  
于洪岩 Yu Hongyan ◽  
...  

2011 ◽  
Vol 38 (8) ◽  
pp. 0802011
Author(s):  
崔锦江 Cui Jinjiang ◽  
宁永强 Ning Yongqiang ◽  
姜琛昱 Jiang Chenyu ◽  
王帆 Wang Fan ◽  
施燕博 Shi Yanbo ◽  
...  

Author(s):  
Jeffery C. C. Lo ◽  
C. S. Yung ◽  
S. W. Ricky Lee ◽  
Steve H. K. Lee ◽  
J. S. Wu ◽  
...  

The alignment of optical fibers is very critical in optoelectronic packaging. A slight offset in any direction may severely affect the performance of the photonic device. Recently, passive alignment of optical fibers has attracted substantial attention due to its lower manufacturing cost and faster processing time when compared with active alignment. For conventional passive alignment, the position of each optical fiber is defined by the geometry of a V-groove. The epoxy is dispensed from the top of the V-groove and another cover plate is usually required to press the fiber against the walls of the V-groove. In the present study, a new technique for epoxy dispensing is developed. Instead of being applied from the top of the V-groove, some low viscosity epoxy is dispensed in a “canal” first. The epoxy fills an adjacent “reservoir” and then flows into the V-groove. Subsequently the epoxy flow runs through the gap between the optical fiber and the V-groove walls. It is observed that the flow of epoxy can align the optical fiber by the surface tension. Once the optical fiber is aligned and the epoxy is cured, more epoxy is applied in a glob-top manner to mechanical enhancement. In this paper, the configuration of the V-groove and associated features, the epoxy dispensing process, and the results of alignment are presented in details.


2001 ◽  
Vol 7 (S2) ◽  
pp. 1004-1005
Author(s):  
Motonobu Fujita ◽  
Makoto Naruse ◽  
Masatoshi Ishikawa

Here we show a confocal microscope system where a vertical-cavity surface-emitting laser (VCSEL) array is introduced for the parallel probing beams.A VCSEL array is a semiconductor laser device that emits circular beams vertically to the surface of the chip, which can directly be used as confocal laser microscope applications. The VCSEL device itself can be the parallel beam source of the confocal laser system, whereas in conventional Nipkow disc-based system, several lenses are required to form probing beams. Figure 1 shows the basic structure of VCSEL-based confocal microscope systems. Since there is typically no correlation between individual channels of VCSEL, there are no interferences among dense parallel beam arrays. Additionally, in the case of Nipkow disc system, the signal to noise ratio of the detected light is another problem: some of the light from the source laser reflects at the surface of the disc, which eventually could be detected by the sensor as noise. in the proposed system no such problem occurs as shown in Fig. 2(a). in addition, “all” optical beam from VCSEL is used as probing beam whereas most of the power is lost at the disc as compared in Fig. 2(b). in addition, pixel parallel illumination control is also achievable by controlling each channel of the VCSEL so that the dynamic range of the detected signal is maximized.


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