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Frontiers of Optoelectronics

Front Optoelec    2013, Vol. 6 Issue (3) : 297-302     DOI: 10.1007/s12200-013-0336-8
RESEARCH ARTICLE |
Highly nonlinear enhanced-core photonic crystal fiber with low dispersion for wavelength conversion based on four-wave mixing
Yashar E. MONFARED(), A. MOJTAHEDINIA, A. R. MALEKI JAVAN, A. R. MONAJATI KASHANI
Department of Electrical Engineering, Shahre-rey Branch, Islamic Azad University, Tehran 1815163111, Iran
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Abstract

In this paper, a new structure of highly nonlinear low dispersion photonic crystal fiber (HN-PCF) by elliptical concentration of GeO2 in the PCF core has been proposed. Using finite difference time domain (FDTD) method, we have analyzed the dispersion properties and effective mode area in the HN-PCF. Simulative results show that the dispersion variation is within±0.65 ps/(nm?km) in C-band, especially 0.24 ps/(nm?km) in 1.55 μm wavelength. Effective area and nonlinear coefficient are 1.764 μm2 and 72.6 W-1?km-1 respectively at 1.55 μm wavelength. The proposed PCF demonstrates high nonlinear coefficient, ultra small effective mode area and nearly-zero flattened dispersion characteristics over C-band, which can have important application in all-optical wavelength conversion based on four wave mixing (FWM).

Keywords dispersion      effective area      four wave mixing (FWM)      wavelength conversion      photonic crystal fiber (PCF)     
Corresponding Authors: MONFARED Yashar E.,Email:y.monfared@ieee.org   
Issue Date: 05 September 2013
 Cite this article:   
Yashar E. MONFARED,A. MOJTAHEDINIA,A. R. MALEKI JAVAN, et al. Highly nonlinear enhanced-core photonic crystal fiber with low dispersion for wavelength conversion based on four-wave mixing[J]. Front Optoelec, 2013, 6(3): 297-302.
 URL:  
http://journal.hep.com.cn/foe/EN/10.1007/s12200-013-0336-8
http://journal.hep.com.cn/foe/EN/Y2013/V6/I3/297
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Yashar E. MONFARED
A. MOJTAHEDINIA
A. R. MALEKI JAVAN
A. R. MONAJATI KASHANI
Fig.1  Cross section of HN-PCF with holes diameter , holes pitch, width , and height of ellipse of the germano-silicate high index core
Fig.2  Fundamental guided mode of HN-PCF with = 0.9 μm, = 2.3 μm, = 0.6 μm and = 2.2 μm in operation wavelength = 1.55 μm
Fig.3  Dispersion curves of HN-PCF with = 2.3 μm, = 0.6 μm and = 2.2 μm as function of wavelength
Fig.4  Nonlinear coefficient curves of HN-PCF with = 2.3 μm, = 0.6 μm and = 2.2 μm as function of wavelength
Fig.5  Dispersion curves of HN-PCF with = 0.7 μm and = 2.3 μm as function of wavelength
Fig.6  Effective area of HN-PCF with = 0.6 μm, = 2.2 μm and = 2.3 μm as function of wavelength
propertyC-HNPCFR-HNPCFOur HN-PCF
effective area3.5 μm22 μm21.76 μm2
dispersion3.2 ps/(nm?km)0.7 ps/(nm?km)0.24 ps/(nm?km)
n22.507 × 10-203 × 10-203.16 × 10-20
nonlinear coefficient29 W-1?km-160.5 W-1?km-172.6 W-1?km-1
Tab.1  Optical properties of fibers at = 1.55 μm wavelength
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