scholarly journals Design of Ring-Core Few-mode-EDFA with the Enhanced Saturation Input Signal Power and Low Differential Modal Gain

2021 ◽  
pp. 1-1
Author(s):  
Yihong Fang ◽  
Yan Zeng ◽  
Yuwen Qin ◽  
Ou Xu ◽  
Jianping Li ◽  
...  
2017 ◽  
Vol 178 ◽  
pp. 289-292 ◽  
Author(s):  
A. Crespo-Yepes ◽  
E. Barajas ◽  
J. Martin-Martinez ◽  
D. Mateo ◽  
X. Aragones ◽  
...  

2015 ◽  
Vol 74 (8) ◽  
Author(s):  
M. T. Ahmad ◽  
A. A. Latiff ◽  
Z. Zakaria ◽  
Z. Jusoh ◽  
H. Ahmad ◽  
...  

The amplification and lasing characteristics of the newly developed Thulium-Ytterbium co-doped fiber (TYDF) are investigated. It is obtained that both TYDF amplifier and laser operate at 1950 nm region. The maximum gain of 22.4 dB is obtained for 1942 nm signal when the 980 nm multimode pump power, TYDF length and input signal power are fixed at 1.2 W, 5 m and -20 dBm, respectively. At 5 m long of TYDF, the laser produces two prominent lines at 1960 nm and 1965 nm with peak powers of 2.8 dBm and 3.1 dBm, respectively due to the nonlinear polarization rotation (NPR) effect in the cavity.


2017 ◽  
Vol 38 (3) ◽  
Author(s):  
Aruna Rani ◽  
Sanjeev Dewra

AbstractThis paper investigates the performance of an optical system based on optimized semiconductor optical amplifier (SOA) at 160 Gbps with 0.8 nm channel spacing. Transmission distances up to 280 km at –30 dBm input signal power and up to 247 km at –32 dBm input signal power with acceptable bit error rate (BER) and


F1000Research ◽  
2021 ◽  
Vol 10 ◽  
pp. 251
Author(s):  
Siti Azlida Ibrahim ◽  
Amilia Mansoor ◽  
Tuan Ainin Sofea Tuan Mohd Marzuki ◽  
Nasr Y. M. Omar ◽  
Hairul Azhar Abdul Rashid

Background: One way to reduce the length of the gain medium in Erbium-Doped Fiber Amplifier (EDFA) is by doping the fiber core with a high concentration of Erbium. However, this method caused ion clustering effects, which limits the EDFA’s efficiency.  In this research, the use of Gallium as a new co-dopant in erbium-doped silica fiber is explored. Methods: The new fiber, namely Gallium co-doped Erbium fiber (Ga-EDF), is used as a gain medium in an optical fiber amplifier setup. A 2-meter length of the Ga-EDF fiber was used in a single pass configuration with a forward pumping scheme at 150 mW pump power. The Ga-EDF amplifier's gain and noise figure while pumping at 980 nm and 1480 nm were compared. The amplifier's performance was evaluated as the input signal power varied between -30 dBm to 3 dB, over the wavelength range of 1520 nm to 1580 nm. Results: The 980 nm-pumped Ga-EDF amplifier achieved the maximum small-signal gain of 22.45 dB and the corresponding noise figure of 5.71 dB at the input signal wavelength of 1535 nm. Meanwhile, the 1480 nm-pumped Ga-EDF amplifier attained the maximum small-signal gain of 20.83 dB and the corresponding noise figure of 5.09 dB at the input signal wavelength of 1550 nm. At the input signal power below -20 dBm and the wavelength range 1520 nm to 1547 nm, the Ga-EDF performs better when pumped at 980 nm. Their performance is comparable at the input signal wavelength range between 1547 nm to 1580 nm. At the input signal power above -20 dBm, the 1480 nm-pumped Ga-EDF outperformed the 980 nm-pumped amplifier. Conclusions: The overall performance indicates that the gain saturation point of the 1480 nm-pumped amplifier is higher than the 980 nm-pumped.


2021 ◽  
Author(s):  
Irfan Alp Gurkaynak ◽  
Mohammed Kamil Salh Al-Mashhadani ◽  
Mudhafar Hussein Ali ◽  
Thamer Fahad Al-Mashhadani ◽  
Abdullah Erkam Gunduz ◽  
...  

Abstract A Widely flatness gain bandwidth with double pass parallel hybrid fiber amplifier is experimentally demonstrated in this study. The proposed design combines serial erbium–Raman fiber amplifier in one branch and Raman fiber amplifier in the second branch. Multiple Raman pump units with a maximum power of 800 mW (250 mW of 1410 nm, 225 mW of 1480 nm, and 325 mW of 1495 nm) are utilized. Pump recycling technique is applied to achieve acceptable pumping efficiency. A maximum flatness gain bandwidth of 80 nm (1525–1605 nm) and average gain level of 22.5 dB are obtained at a small input signal power of -25 dBm and optimum pump power values. By comparison, a wider flatness gain of 90 nm (1520–1610 nm) and average gain level of 11.5 dB are achieved at a large input signal power of -5 dBm.


2015 ◽  
Vol 815 ◽  
pp. 348-352 ◽  
Author(s):  
M. Safuan Zainudin ◽  
N.A.M. Ahmad Hambali ◽  
Goh Chee Seong ◽  
M. Shakirin Abu Hurera ◽  
N. Roshidah ◽  
...  

The development was conducted with three configurations of L-Band EDFA, L-Band EDFA utilising Single FBG and Dual Stage L-Band EDFA utilising Dual FBG. The configurations utilising the FBG using 35 meter M-12 Fibercore EDF as the gain medium to amplify the input signal power in the L-band region. The gain enhancement has shown by the Dual Stage L-Band EDFA utilising Dual FBG by injecting low input signal power of -10 dBm. The flat amplitude of OSNR at 33.358 dB was produced at injected wavelength from 1570 nm to 1605 nm.


2015 ◽  
Vol 6 ◽  
pp. 1221-1228 ◽  
Author(s):  
Almir Wirth Lima ◽  
João Cesar Moura Mota ◽  
Antonio Sergio Bezerra Sombra

We simulated and analyzed in detail the behavior of ultrashort optical pulses, which are typically used in telecommunications, propagating through graphene-based nanoribbon waveguides. In this work, we showed the changes that occur in the Gaussian and hyperbolic secant input pulses due to the attenuation, high-order dispersive effects and nonlinear effects. We concluded that it is possible to control the shape of the output pulses with the value of the input signal power and the chemical potential of the graphene nanoribbon. We believe that the obtained results will be highly relevant since they can be applied to other nanophotonic devices, for example, filters, modulators, antennas, switches and other devices.


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