Effect of third-order dispersion on subpicosecond pulse propagation in photonic-crystal waveguides

2006 ◽  
Vol 89 (13) ◽  
pp. 131101 ◽  
Author(s):  
Yu Tanaka ◽  
Haruhiko Kuwatsuka ◽  
Hitoshi Kawashima ◽  
Naoki Ikeda ◽  
Yoshimasa Sugimoto ◽  
...  
2010 ◽  
Vol 35 (18) ◽  
pp. 3084 ◽  
Author(s):  
Vladimir I. Kruglov ◽  
Claude Aguergaray ◽  
John D. Harvey

2013 ◽  
Vol 23 ◽  
pp. 40-44 ◽  
Author(s):  
O. Shulika ◽  
I. Sukhoivanov ◽  
S. Iakushev ◽  
I. Guryev ◽  
J. Andrade Lucio ◽  
...  

This paper presents the design of all-normal dispersion photonic-crystal fiber optimized for pulse-preserving supercontinuum generation near 800 nm. The supercontinuum generation is analyzed numerically addressing the role of pump pulse energy and the pump wavelength deviation from the zeroth point of third-order dispersion. We have also shown that supercontinuum generated in designed ANDi-PCF from a few nanojoule 100 fs pulses can be efficiently compressed down to a sub-10-fs pulse with a simple quadratic compressor.


2009 ◽  
Vol 36 (9) ◽  
pp. 2295-2299
Author(s):  
雷大军 Lei Dajun ◽  
杨华 Yang Hua ◽  
文双春 Wen Shuangchun ◽  
董辉 Dong Hui ◽  
张景贵 Zhang Jinggui ◽  
...  

2014 ◽  
Vol 938 ◽  
pp. 316-321
Author(s):  
E. Gunasundari ◽  
K. Senthilnathan ◽  
S. Sivabalan ◽  
K. Nakkeeran ◽  
P. Ramesh Babu

In this paper, we propose a new type of optical waveguide called silicon nanowire embedded equai-angular spiral photonic crystal fiber (SN-SPCF) using fully vectorial finite element method, where closely arranged arrays of air holes act as cladding and nanosize silicon material at the centre acts as core. We show that the proposed nanowire embedded PCF of 400 nm core diameter exhibits high anomalous group velocity dispersion (-3148 ps2/km), small third order dispersion (-8.6591 ps3/km) and high nonlinearity (443.2 W-1m-1) at 1550 nm wavelength. Soliton-effect pulse compression of femtosecond pulses in a silicon nanowire-spiral photonic crystal fiber at 1550 nm is numerically studied. We demonstrate a pulse compression of 75 fs input pulse to about 4 fs by the simultaneous actions of both linear effects (a large anomalous group velocity dispersion and a small third order dispersion) and the nonlinear effect (an effective high nonlinearity).


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