CONVECTION AND RADIATION EFFECTS IN HOLLOW, COMPOUND OPTICAL FIBERS

Author(s):  
Juan I. Ramos
1988 ◽  
Author(s):  
Peter B. Lyons ◽  
C A. Barnes ◽  
E J. Friebele ◽  
R Gilbert ◽  
R Greenwell ◽  
...  

2018 ◽  
Vol 216 (3) ◽  
pp. 1800485 ◽  
Author(s):  
Antonino Alessi ◽  
Angela Guttilla ◽  
Sylvain Girard ◽  
Simonpietro Agnello ◽  
Marco Cannas ◽  
...  

2008 ◽  
Author(s):  
Sylvain Girard ◽  
Youcef Ouerdane ◽  
Claude Marcandella ◽  
Thierry Robin ◽  
Aziz Boukenter ◽  
...  

1998 ◽  
Author(s):  
Jan Troska ◽  
Jeremy Batten ◽  
Karl A. Gill ◽  
Francois Vasey

1986 ◽  
Vol 25 (Part 1, No. 3) ◽  
pp. 464-468 ◽  
Author(s):  
Kaya Nagasawa ◽  
Yutaka Hoshi ◽  
Yoshimichi Ohki ◽  
Kichinosuke Yahagi

1993 ◽  
Vol 32 ◽  
pp. 436-440 ◽  
Author(s):  
L. Gherardi ◽  
P. Marelli ◽  
A. Serra ◽  
G. Viezzoli

Sensors ◽  
2021 ◽  
Vol 21 (24) ◽  
pp. 8193
Author(s):  
Sohel Rana ◽  
Austin Fleming ◽  
Nirmala Kandadai ◽  
Harish Subbaraman

Neutron and gamma irradiation is known to compact silica, resulting in macroscopic changes in refractive index (RI) and geometric structure. The change in RI and linear compaction in a radiation environment is caused by three well-known mechanisms: (i) radiation-induced attenuation (RIA), (ii) radiation-induced compaction (RIC), and (iii) radiation-induced emission (RIE). These macroscopic changes induce errors in monitoring physical parameters such as temperature, pressure, and strain in optical fiber-based sensors, which limit their application in radiation environments. We present a cascaded Fabry–Perot interferometer (FPI) technique to measure macroscopic properties, such as radiation-induced change in RI and length compaction in real time to actively account for sensor drift. The proposed cascaded FPI consists of two cavities: the first cavity is an air cavity, and the second is a silica cavity. The length compaction from the air cavity is used to deduce the RI change within the silica cavity. We utilize fast Fourier transform (FFT) algorithm and two bandpass filters for the signal extraction of each cavity. Inclusion of such a simple cascaded FPI structure will enable accurate determination of physical parameters under the test.


2007 ◽  
Vol 54 (6) ◽  
pp. 2598-2603 ◽  
Author(s):  
B. Tortech ◽  
A. Gusarov ◽  
M. Van Uffelen ◽  
J. Bisutti ◽  
S. Girard ◽  
...  

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