Ultra-flattened negative dispersion for residual dispersion compensation using soft glass equiangular spiral photonic crystal fiber

2016 ◽  
Vol 63 (17) ◽  
pp. 1681-1687 ◽  
Author(s):  
Md. Imran Hasan ◽  
R. R. Mahmud ◽  
Monir Morshed ◽  
Md. Rabiul Hasan
2019 ◽  
Vol 40 (4) ◽  
pp. 401-410 ◽  
Author(s):  
Md. Ibadul Islam ◽  
Kawsar Ahmed ◽  
Shuvo Sen ◽  
Bikash Kumar Paul ◽  
Md. Shadidul Islam ◽  
...  

Abstract A photonic crystal fiber in square lattice architecture is numerically investigated and proposed for broadband dispersion compensation in optical transmission system. Simulation results reveal that it is possible to obtain an ultra-high negative dispersion of about −571.7 to −1889.7 (ps/nm.km) in the wavelength range of 1340 nm to 1640 nm. Experimentally it is demonstrated that the design fiber covers a high birefringence of order 4.74×10‒3 at the wavelength of 1550 nm. Here, numerical investigation of guiding properties and geometrical properties of the proposed PCF are conducted using the finite element method (FEM) with perfectly match layers. Moreover, it is established more firmly that the proposed fiber successfully compensates the chromatic dispersion of standard single mode in entire band of interest. Our result is attractive due to successfully achieve ultra-high negative dispersion that is more promisor than the prior best results.


2010 ◽  
Author(s):  
Manish Tiwari ◽  
Arti Agrawal ◽  
Vijay Janyani ◽  
B. M. Azizur Rahman

2020 ◽  
Vol 41 (4) ◽  
pp. 371-383 ◽  
Author(s):  
Saleha Fatema ◽  
Rubaya Absar ◽  
Mohammad Istiaque Reja ◽  
Jobaida Akhtar

AbstractThe effect of core infiltration in the optical properties of Photonic Crystal Fiber (PCF) is investigated. The soft glass rod infiltration provides greater refractive index contrast between the core and the cladding. This modification improves the optical properties significantly. Four structures of photonic crystal fiber (Hexagonal, Octagonal, Decagonal and Elliptical) are investigated and a comparative study has been made to observe the difference in the optical properties due to the infiltration. It is observed that, by introducing this infiltration the birefringence is improved up to the order of $10^{-1}$ and a very high negative dispersion coefficient of 7744ps/(km.nm) can be achieved. The birefringence is increased $4.82\times10^{6}$ times in the hexagonal PCF, $5.38\times10^{5}$ times in octagonal PCF, 546 times in decagonal PCF and about 8 times in the elliptical PCF at operating wavelength due to the core infiltration. The positive dispersion of the fiber is eliminated and a very high negative dispersion co-efficient of 7744ps/(km.nm) is achieved in hexagonal PCF, a relatively flattened dispersion is obtained in other cases due to infiltration at operating wavelength. The nonlinearity is increased about 73 times in case of hexagonal PCF and in other cases it is increased about 2 times. The confinement loss is reduced up to the order of $10^{-11}$ due to the infiltration at the operating wavelength of 1550 nm. Another comparative study shows that the introduced fibers outperform most of the recent works with a more simple structure, which reduce fabrication complexity. The numerical investigation of the structures is conducted using full vector finite element method.


2014 ◽  
Vol 2014 ◽  
pp. 1-6 ◽  
Author(s):  
S. Revathi ◽  
Srinivasa Rao Inbathini ◽  
Rizwan Ali Saifudeen

We propose and design a spiral photonic crystal fiber with elliptical air holes for achieving high birefringence, large nonlinearity, and negative dispersion. The structure is designed using chalcogenide glass (As2S3) for different ellipticity ratios of air holes in the cladding and the effect on various properties is observed. The proposed structure has birefringence of the order 10−2, nonlinearity of 26739.42 W−1 m−1, and dispersion of −1136.69 at 0.85 μm. An accurate numerical approach based on finite element method is used for the design and simulation of the structure. Due to high birefringence and negative dispersion, the proposed structure can be used for polarization control and dispersion compensation, respectively.


2009 ◽  
Vol 21 (22) ◽  
pp. 1722-1724 ◽  
Author(s):  
A. Agrawal ◽  
N. Kejalakshmy ◽  
B.M.A. Rahman ◽  
K.T.V. Grattan

Optik ◽  
2020 ◽  
Vol 218 ◽  
pp. 164997 ◽  
Author(s):  
Anurag Upadhyay ◽  
Shivam Singh ◽  
Y.K. Prajapati ◽  
Rajeev Tripathi

Sign in / Sign up

Export Citation Format

Share Document