Laser Guidance and Trapping of Mesoscale Particles in Hollow-Core Optical Fibers

1999 ◽  
Vol 82 (7) ◽  
pp. 1574-1577 ◽  
Author(s):  
Michael J. Renn ◽  
Robert Pastel ◽  
Heather J. Lewandowski
2021 ◽  
Author(s):  
Timur Ermatov ◽  
Marina Novoselova ◽  
Julia Skibina ◽  
Andrey Machnev ◽  
Dmitry Gorin ◽  
...  

Fibers ◽  
2019 ◽  
Vol 7 (5) ◽  
pp. 50 ◽  
Author(s):  
Walter Belardi

The possibility of guiding light in air has fascinated optical scientists and engineers since the dawn of optical fiber technology [...]


2014 ◽  
Vol 68 (6) ◽  
Author(s):  
Alexey V. Prokhorov ◽  
Maxim G. Gladush ◽  
Mikhail Yu. Gubin ◽  
Andrey Yu. Leksin ◽  
Sergey M. Arakelian

1984 ◽  
Vol 45 (7) ◽  
pp. 725-727 ◽  
Author(s):  
M. Watanabe ◽  
T. Hidaka ◽  
H. Tanino ◽  
K. Hoh ◽  
Y. Mitsuhashi

2019 ◽  
Vol 27 (7) ◽  
pp. 9868 ◽  
Author(s):  
Roman E. Noskov ◽  
Anastasia A. Zanishevskaya ◽  
Andrey A. Shuvalov ◽  
Sergei V. German ◽  
Olga A. Inozemtseva ◽  
...  

2020 ◽  
Vol 28 (4) ◽  
pp. 5423 ◽  
Author(s):  
Haihong Bao ◽  
Yingzhen Hong ◽  
Wei Jin ◽  
Hoi Lut Ho ◽  
Chao Wang ◽  
...  

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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