Surface Plasmon Resonance Bio-Sensor with Full Field Phase Detection

2008 ◽  
Vol 381-382 ◽  
pp. 349-352
Author(s):  
Ju Yi Lee ◽  
T.K. Chou ◽  
H.C. Shih ◽  
Cheng Chih Hsu

A full field phase detection system for surface plasmon resonance (SPR) bio-sensor is presented. The phase difference variation between s and p polarization resulting from the SPR was detected by the polarization interferometry. In the polarization interferometry, the light reflected from the SPR sensor was divided into four phase quardrature parts by polarization components. By means of an algorithm similar to phase shifting interferometry, the phase distribution of SPR bio-sensor was obtained. We have successfully detected the phase difference variation with 0.07º resolution within 1×1 mm2 full field range. The corresponding detection limit of the refractive index change is about 1×10-7.

2018 ◽  
Vol 26 (16) ◽  
pp. 20975 ◽  
Author(s):  
Iltai (Isaac) Kim ◽  
Sokwon Paik ◽  
Yang Bae Jeon ◽  
Jae Sung Park ◽  
Hyunjung Kim ◽  
...  

2021 ◽  
Vol 3 ◽  
Author(s):  
Hiromasa Shimizu ◽  
Takahiro Ogura ◽  
Takumi Maeda ◽  
Shogo Suzuki

We show here the design, fabrication, and characterization of a wedge-shaped Au thin film with an enhanced figure of merit (FOM). This is achieved by using a reflectivity change in an attenuated total reflection (ATR) setup by slightly modulating the wavenumber of the surface plasmon polariton by means of the varying thickness of the Au thin film. The wedge-shaped Au thin film is equivalent to multiple surface plasmon resonance (SPR) transducers integrated in a single chip and was fabricated by an electron-beam evaporation process with the position of the shutter controlled during the deposition. The FOM, defined as the difference between the maximum and minimum values of the normalized reflectivity change (ΔR/R) divided by the corresponding difference of the incident angles, was 8.0-times larger than that based on the reflectivity R. Also, we demonstrated that the wedge-shaped Au thin film was able to detect ethanol gas at a concentration of 0.2%, corresponding to a refractive index change of 2 × 10−5, without any surface functionalization. Since the sensing signal can be obtained with a single image from the wedge-shaped Au thin film without precise thickness control of the metal thickness, no other materials or modulation equipment is necessary, and the sensing chip can be employed in simple and highly sensitive systems.


2015 ◽  
Vol 42 (6) ◽  
pp. 0608009
Author(s):  
王斌 Wang Bin ◽  
荆振国 Jing Zhenguo ◽  
彭伟 Peng Wei ◽  
刘云 Liu Yun

2000 ◽  
Vol 46 (1) ◽  
pp. 55-62 ◽  
Author(s):  
Sung-Hoon Kim ◽  
Kyeong-Sik Ock ◽  
Jung-Hyuk Im ◽  
Jae-Ho Kim ◽  
Kwang-Nak Koh ◽  
...  

2007 ◽  
Author(s):  
C.-H. Lin ◽  
Y.-D. Su ◽  
C.-H. Huang ◽  
K.-C. Cho ◽  
S.-J. Chen

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