Wavelength dependence of bending loss in monomode optical fibers: effect of the fiber buffer coating

1990 ◽  
Vol 15 (17) ◽  
pp. 947 ◽  
Author(s):  
R. Morgan ◽  
J. S. Barton ◽  
P. G. Harper ◽  
J. D. C. Jones
2014 ◽  
Vol 5 (1) ◽  
Author(s):  
Svetislav Savović ◽  
Ana Simović ◽  
Aleksandar Djordjevich ◽  
Aco Janićijević

Power flow equation is used to calculate equilibrium mode distribution in W-type glass optical fibers. It has been shown how the coupling length for achieving the equilibrium mode distribution in W-type glass optical fibers varies with the depth and width of the intermediate layer and coupling strength for different widths of launch beam distribution. W-type optical fibers have shown effectiveness in reducing modal dispersion and bending loss.


Author(s):  
Sami D. Alaruri

In this chapter, the wavelength dependence of bend loss in a step-index multimode optical fiber (100 µm core diameter; fused silica) was investigated for fiber bend radii ranging between 2.0 and 4.5 mm using six laser excitation wavelengths, namely, 337.1, 470, 590, 632.8, 750, and 810 nm. The results obtained from fitting the bend loss measurements to Kao's model and utilizing MATLAB® indicate that bend loss is wavelength dependent and transmission loss in multimode optical fibers increases with the decrease in the fiber bend radius. Furthermore, the response of a microbend fiber-optic displacement sensor was characterized at 337.1, 470, 632.8, 750, and 810 nm. Measurements obtained from the microbend sensor indicate that the sensor output power is linear with the applied displacement and the sensor output is wavelength dependent. Lastly, references for industrial and biomedical applications of microbend fiber-optic sensors are provided. Finally, a brief description for the transmission loss mechanisms in optical fibers is given.


2007 ◽  
Vol 24 (10) ◽  
pp. 2610 ◽  
Author(s):  
Rutger W. Smink ◽  
Bastiaan P. de Hon ◽  
Anton G. Tijhuis

1983 ◽  
Author(s):  
N. Lagakos ◽  
D. S. Czaplak ◽  
J. H. Cole ◽  
J. A. Bucaro ◽  
E. L. Green

1997 ◽  
Vol 138 (1-3) ◽  
pp. 40-44 ◽  
Author(s):  
Toru Mizunami ◽  
Masato Hashimoto ◽  
Sanjay Gupta ◽  
Yasunao Uchida ◽  
Teruo Shimomura

Polymers ◽  
2018 ◽  
Vol 10 (8) ◽  
pp. 899 ◽  
Author(s):  
Hanna Stawska ◽  
Maciej Popenda ◽  
Elżbieta Bereś-Pawlik

In this paper, we present numerical studies of several different structures of anti-resonant, hollow core optical fibers. The cladding of these fibers is based on the Kagomé lattice concept, with some of the core-surrounding lattice cells removed. This modification, by creating additional, glass-free regions around the core, results in a significant improvement of some important optical fiber parameters, such as confinement loss (CL), bending loss (BL), and dispersion parameter (D). According to the conducted simulations (with fused silica glass being the structure’s material), CL were reduced from ~0.36 dB/m to ~0.16 dB/m (at 760 nm wavelength) in case of the structure with removed cells, and did not exceed the value of 1 dB/m across the 700–850 nm wavelength range. Additionally, proposed structure exhibits a remarkably low value of D—from 1.5 to 2.5 ps/(nm × km) at the 700–800 nm wavelength range, while the BL were estimated to be below 0.25 dB/m for bending radius of ~1.5 cm. CL and D were simulated, additionally, for structures made of acrylic glass polymethylmethacrylate, (PMMA), with similarly good results—DPMMA ∊ [2, 4] ps/(nm × km) and CLPMMA ≈ 0.13 dB/m (down from 0.41 dB/m), for the same spectral regions (700–800 nm bandwidth for D, and 760 nm wavelength for CL).


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