Modeling of plasmon-polariton refractive-index hollow core fiber sensors assisted by a fiber Bragg grating

2006 ◽  
Vol 24 (10) ◽  
pp. 3789-3796 ◽  
Author(s):  
Nemova ◽  
Kashyap
2014 ◽  
Author(s):  
Qiang Zhang ◽  
Tao Zhu ◽  
Fengyang Yin ◽  
Kin Seng Chiang ◽  
Ming Deng

2018 ◽  
Vol 38 (12) ◽  
pp. 1206007
Author(s):  
谭展 Tan Zhan ◽  
廖常锐 Liao Changrui ◽  
刘申 Liu Shen ◽  
侯茂祥 Hou Maoxiang ◽  
张哲 Zhang Zhe ◽  
...  

Author(s):  
Farah S. Al-Thahapy ◽  
Anwaar A. Al-Dergazly

In this project, four of fibers Bragg gratings were fabricated by injecting different volumes of liquids (star line Glass Mechanix optical adhesive material, olive oil diluted with ethanol) into the hollow core fiber. The amplitude splitting interferometric technique with a high resolution specially designed translation stage was used for the fabrication process. The fabrication was done using ultraviolet laser operated at wavelength 405nm. The fabricated Bragg length of the four fibers is equal to 3.8 cm. The results presented fiber Bragg grating (FBG) with successful fabrication at 653.3 nm Bragg reflected wavelength.


Photonics ◽  
2020 ◽  
Vol 7 (4) ◽  
pp. 111
Author(s):  
Haijin Chen ◽  
Xuehao Hu ◽  
Meifan He ◽  
Qianqing Yu ◽  
Zhenggang Lian ◽  
...  

We demonstrate a dual-core fiber-based Mach–Zehnder interferometer that could be used for precise detection of variations in refractive indices of gaseous samples. The fiber used here have a solid germanium-doped silica core and an air core that allows gases to flow through. Coherent laser beams are coupled to the two cores, respectively, and thus excite guiding modes thereby. Interferogram would be produced as the light transmitted from the dual cores interferes. Variations in refractive index of the hollow core lead to variations in phase difference between the modes in the two cores, thus shifting the interference fringes. The fringe shifts can be then interrogated by a photodiode together with a narrow slit in front. The resolution of the sensor was found to be ~1 × 10−8 RIU, that is comparable to the highest resolution obtained by other fiber sensors reported in previous literatures. Other advantages of our sensor include very low cost, high sensitivity, straightforward sensing mechanism, and ease of fabrication.


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