Fiber Optic Refractometer Based on Leaky-Mode Interference of Bent Fiber

2015 ◽  
Vol 27 (1) ◽  
pp. 11-14 ◽  
Author(s):  
Xinpu Zhang ◽  
Wei Peng
2020 ◽  
Vol 28 (7) ◽  
pp. 9123 ◽  
Author(s):  
Zhihong Li ◽  
Qikai Bao ◽  
Jiayin Zhu ◽  
Xiukai Ruan ◽  
Yuxing Dai

2000 ◽  
Vol 6 (1) ◽  
pp. 83-90 ◽  
Author(s):  
Arun Kumar ◽  
Rajeev Jindal ◽  
Ravi K. Varshney ◽  
Sangeet K. Sharma

2015 ◽  
Vol 40 (7) ◽  
pp. 1468 ◽  
Author(s):  
G. Salceda-Delgado ◽  
A. Van Newkirk ◽  
J. E. Antonio-Lopez ◽  
A. Martinez-Rios ◽  
A. Schülzgen ◽  
...  

IEEE Access ◽  
2019 ◽  
Vol 7 ◽  
pp. 26641-26651 ◽  
Author(s):  
Zhihong Li ◽  
Zhuying Yu ◽  
Yubing Shen ◽  
Xiukai Ruan ◽  
Yuxing Dai

Author(s):  
J. M. Cowley ◽  
R. Glaisher ◽  
J. A. Lin ◽  
H.-J. Ou

Some of the most important applications of STEM depend on the variety of imaging and diffraction made possible by the versatility of the detector system and the serial nature, of the image acquisition. A special detector system, previously described, has been added to our STEM instrument to allow us to take full advantage of this versatility. In this, the diffraction pattern in the detector plane may be formed on either of two phosphor screens, one with P47 (very fast) phosphor and the other with P20 (high efficiency) phosphor. The light from the phosphor is conveyed through a fiber-optic rod to an image intensifier and TV system and may be photographed, recorded on videotape, or stored digitally on a frame store. The P47 screen has a hole through it to allow electrons to enter a Gatan EELS spectrometer. Recently a modified SEM detector has been added so that high resolution (10Å) imaging with secondary electrons may be used in conjunction with other modes.


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