High Sensitivity Differential Refractometer by Evanescent Wave in a Thin Dielectric Waveguide

Author(s):  
Rafael A. Ribeiro ◽  
Sérgio C. Zilio
2020 ◽  
Vol 307 ◽  
pp. 84-89
Author(s):  
Aisyah Hanim Surani ◽  
Affa Rozana Abdul Rashid ◽  
N. Arsad ◽  
Amna Afiqah Nasution Hakim

An optimized study of tapered polymer optical fiber (POF) for measurement of different concentration of ethanol in deionized water (0.5%-3.5%) is proposed and demonstrated. This sensor operated based on evanescent wave absorption principle. The cladding of PMMA based POF is removed using organic solvents which can be used to create tapered POF. The unclad length around 1 cm and 3 cm as well as the waist diameters of POF in the range of 5 mm and 8 mm were compared for their efficiency as an ethanol sensor based on power output ratio values. Tapered POF with smaller waist diameter and longer tapered length showed higher sensitivity as ethanol sensor. Therefore, by tailoring the length and tapered diameter of POF, high sensitivity of ethanol sensor can be fabricated.


2020 ◽  
Author(s):  
Yanjun Hu ◽  
Abdul Ghaffar ◽  
Yulong Hou ◽  
Wenyi Liu ◽  
Fei Li ◽  
...  

Abstract A novel high sensitivity relative humidity (RH) sensor was proposed by using micro structure plastic optical fiber (POF) based on the surface plasmon resonance (SPR) effect and the evanescent wave (EW) loss. The micro structure was fabricated on the POF and coated with a gold layer and agarose, adopting the sputtering and dip-coating technique. These construction effects on the attenuation of power caused by the SPR effect and the EW loss were used to perform RH detections. The agarose’s different refractive indexes (RIs) caused fluctuations in the transmission power when the humidity increased. The demonstrated experimental results showed that the proposed sensor achieved a linear response from 20% RH to 80% RH with a high sensitivity of 0.595µW/%. The proposed sensor had the advantages of fast response and recovery. Furthermore, the temperature dependence and the repeatability test of the sensor were also performed.


2014 ◽  
Vol 39 (19) ◽  
pp. 5725 ◽  
Author(s):  
S. Avino ◽  
C. Richmond ◽  
A. Giorgini ◽  
P. Malara ◽  
R. Zullo ◽  
...  

2016 ◽  
Vol 85 ◽  
pp. 876-882 ◽  
Author(s):  
Nianbing Zhong ◽  
Mingfu Zhao ◽  
Lianchao Zhong ◽  
Qiang Liao ◽  
Xun Zhu ◽  
...  

2008 ◽  
Vol 18 (01) ◽  
pp. 167-177 ◽  
Author(s):  
A. DHAWAN ◽  
M. D. GERHOLD ◽  
J. F. MUTH

Surface plasmon and evanescent wave sensors are attractive for chemical and biological sensing applications. They can work in aqueous media and when used in conjunction with the appropriate surface chemistry they can have high specificity and high sensitivity. However, most surface plasmon sensors are relatively complex as they are based on the use of attenuated total internal reflection to excite surface plasmon resonance in a thin gold film and require light to be incident at the appropriate angle and polarization. Other surface plasmon and optical affinity sensors have used the evanescent waves in planar waveguides to interact with the environment. These devices are sensitive but, have strict optical coupling requirements and are difficult to fabricate. In optical fiber evanescent wave sensors the interaction with the surrounding environment is usually obtained by tapering an optical fiber, which significantly weakens the structure, or by just utilizing the end of the optical fiber. In this paper, in-line optical fiber structures are presented that are mechanically robust, and provide a large interaction length for high sensitivity. They are compatible with standard chemistries for optical affinity sensing of biological compounds.


2017 ◽  
Vol 91 ◽  
pp. 623-628 ◽  
Author(s):  
Xin Xin ◽  
Nianbing Zhong ◽  
Qiang Liao ◽  
Yanyan Cen ◽  
Ruohua Wu ◽  
...  

1992 ◽  
Vol 7 (1) ◽  
pp. 39-48 ◽  
Author(s):  
Irene M. Walczak ◽  
Walter F. Love ◽  
Thomas A. Cook ◽  
Rudolf E. Slovacek

1955 ◽  
Vol 8 (2) ◽  
pp. 212 ◽  
Author(s):  
PG Guest

A graphical method is given for correcting the smoothing effect which arises when a celestial distribution of brightness temperature is scanned with an aerial beam. The method is much simpler to apply than previous methods which have been used and is no l


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