Supercontinuum generation in all-solid photonic crystal fibers with a low index subwavelength inclusion in the core

Laser Physics ◽  
2013 ◽  
Vol 23 (8) ◽  
pp. 085104 ◽  
Author(s):  
J Pniewski ◽  
R Kasztelanic ◽  
D Pysz ◽  
R Stepien ◽  
R Buczynski
2020 ◽  
Vol 12 (4) ◽  
pp. 106
Author(s):  
Bao Tran Le Tran ◽  
Thuy Nguyen Thi ◽  
Ngoc Vo Thi Minh ◽  
Trung Le Canh ◽  
Minh Le Van ◽  
...  

In this paper, we propose three solid-core photonic crystal fibers based on silica, with hexagonal, circular and square lattices as a cladding, composed of 8 rings of air-holes surrounding the core, infiltrated with ethanol. Using a commercial software we simulated the light propagation in these structures. The size of the air-holes was from 1 µm to 4 µm. We have shown that the fibers with the hexagonal lattices are optimal for supercontinuum generation since their dispersion characteristics are flat and the smallest.


Sensors ◽  
2021 ◽  
Vol 21 (1) ◽  
pp. 284
Author(s):  
Bowei Wan ◽  
Lianqing Zhu ◽  
Xin Ma ◽  
Tianshu Li ◽  
Jian Zhang

Due to their flexible structure and excellent optical characteristics hollow-core photonic crystal fibers (HC-PCFs) are used in many fields, such as active optical devices, communications, and optical fiber sensing. In this paper, to analyze the characteristics of HC-PCFs, we carried out finite element analysis and analyzed the design for the band gap cladding structure of HC-PCFs. First, the characteristics of HC19-1550 and HC-1550-02 in the C-band were simulated. Subsequently, the structural optimization of the seven-cell HC-1550-02 and variations in characteristics of the optimized HC-1550-02 in the wavelength range 1250–1850 nm were investigated. The simulation results revealed that the optimal number of cladding layers is eight, the optimal core radius is 1.8 times the spacing of adjacent air holes, and the optimal-relative thickness of the core quartz-ring is 2.0. In addition, the low confinement loss bandwidth of the optimized structure is 225 nm. Under the transmission bandwidth of the optimized structure, the core optical power is above 98%, the confinement loss is below 9.0 × 10−3 dB/m, the variation range of the effective mode field area does not exceed 10 μm2, and the relative sensitivity is above 0.9570. The designed sensor exhibits an ultra-high relative sensitivity and almost zero confinement loss, making it highly suitable for high-sensitivity gas or liquid sensing.


2015 ◽  
Author(s):  
Gregory A. Helmininack ◽  
Derek D. Gladysiewski ◽  
Feng Zhou ◽  
Ken Hershman ◽  
Ben Campbell ◽  
...  

2009 ◽  
Vol 34 (23) ◽  
pp. 3631 ◽  
Author(s):  
A. Kudlinski ◽  
G. Bouwmans ◽  
O. Vanvincq ◽  
Y. Quiquempois ◽  
A. Le Rouge ◽  
...  

Optik ◽  
2016 ◽  
Vol 127 (22) ◽  
pp. 10981-10990 ◽  
Author(s):  
A. Barrientos-García ◽  
Igor A. Sukhoivanov ◽  
J.A. Andrade-Lucio ◽  
J.C. Hernandez-Garcia ◽  
G. Ramos-Ortiz ◽  
...  

Laser Physics ◽  
2019 ◽  
Vol 29 (11) ◽  
pp. 115102
Author(s):  
Vu Tran Quoc ◽  
Doan Quoc Khoa ◽  
Bien Chu Van ◽  
Hieu Le Van

2011 ◽  
Vol 19 (27) ◽  
pp. 26672 ◽  
Author(s):  
Pernille Klarskov ◽  
Antti Isomäki ◽  
Kim P. Hansen ◽  
Peter E. Andersen

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