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International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016]
Infogain Publication (Infogainpublication.com) ISSN : 2454-1311
www.ijaems.com Page | 25
Simulation of Gain flattening 32 channels EDFA-
DWDM Optical System
Amit Patni, Durgesh Kumar
Department of ECE, Poornima college of Engineering, Jaipur, India
Abstract—The gain flatness of EDFA plays a very
critical role in DWDM system applications in all optical
network design. The main purpose of this paper is to
achieve gain flatness for 32 channels in order to equalize
amplitude gain of DWDM system. This system is
simulated using Opti system software to achieve gain
flatness of EDFA through variation of EDFA pump
power and input power of system. The gains are flattened
within 41±0.9 dB from Wavelength range 1546 to 1560
nm having noise figure less than 8dB, Optimized EDFA
fiber length of 6.245 m and frequency spacing between
channels is 0.4 nm simultaneously amplified in a EDFA of
single stage. The working model consists of WDM
transmitter , MUX, Pump laser, dual port WDM analyzer
and EDFA as key components
Keywords—EDFA(Er+3
doped fiber amplifier),
DWDM(Dense wavelength division multiplexing), Pump
power, Input power , NF(Noise figure)
I. INTRODUCTION
As now a days ,to facilitate high speed network services
we require large amount of bandwidth, so EDFA are used
extensively in WDM-DWDM technology which increases
the capacity of optical network with high speed without
affecting any cost. EDFA is an optical amplifier which
uses generally Er+3
doped optical fiber as a gain medium
to amplify an optical signal with multiplexed pump laser
and signal is amplified through interaction of doping ions
The main characteristic of it is that its operating
wavelength is 1.55µm as we know that this wavelength
related to third window of optical communication which
shows lowest attenuation comparatively to another optical
communication Transmitting window. The technical
characteristics of EDFA include Efficient pumping, Low
noise, High Gain, Low distortion and minimal inter
channel crosstalk High output power (this is not gain but
amount of possible output power) and most importantly it
amplifies the data channels with high data rates in optical
domain and in operating range of optical fibers. The gain
of optical system depends on the wavelength which can
effect system’s performance and due to unequal gain
spectrum of optical amplifiers, this can unbalance the
powers in the transmitted WDM channels so by
equalizing gain of amplifier we can achieve error free
detection of signals transmitted through optical link.
There are several methods through which optical flat
spectral gain can be designed such as by altering the
pump power, by controlling fiber length, by variation of
input power and by properly choosing optical notch filter
characteristics. In this paper, the gain flatness of EDFA is
achieved by variation of pump power and input power for
a fixed fiber length of 10 km and average output power of
more than 7dBm.
II. METHOD
Figure 1 shows the block diagram of EDFA-DWDM
System design which includes WDM transmitter, MUX,
Pump laser, dual port WDM analyzer , EDFA as key
components in the wavelength region of 1546-1560 nm
having single pumping power using wavelengths between
980-1480 nm. This model has been computed, simulated
and analyzed with varying parameters of gain and noise
figure. The gain flatness and system stability of 980 nm
pump laser wavelength has been obtained maximum
compared to 1480 nm wavelength.
Fig.1: Block diagram of EDFA-DWDM system design
with single pumping source
International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016]
Infogain Publication (Infogainpublication.com) ISSN : 2454-1311
www.ijaems.com Page | 26
III. BACKGROUND
EDFA are always a prime choice to use them as optical
amplifiers because of their capability to amplify signal in
optical domain without converting into electrical signal.
By using EDFA, the transmission distance and capacity
of optical system increases and their characteristic is to
provide flat gain over a range of frequencies.
In this context Paper [1] proposed a model that provides
flat gain of around 27dB for 16 channel WDM system
maintaining frequency spacing between channels to 0.8
nm by using Gain flattening filer(GFF).
In Paper [2] gains are flattened to around 24dB for 16
channel WDM system maintaining frequency spacing
between channels to 0.8 nm by studying variation of
Fiber length and pump power.
In paper [3], the system is simulated to achieve gain
flatness of 16 channel EDFA-WDM through optimized
fiber length and pump power .The gains are flattened
between 24+0.3dB from 1546 to 1558 nm band of
wavelength and noise figure less than 6dB obtained.
Paper [4] describes the simulation models of EDFA Gain
of different Pump powers. Here, EDFA length of 10m
and pump power of 220mW gives the gain of 40.17dB ,
pump power of 620mW gives the gain of 44.3dB and
pump power of 1000mW gives the gain of 46 dB.
Paper [5] proposed a simulation model that provides
EDFA-WDM flattened gain to around 38dB and noise
figure<9dB for 16 channels by variation of fiber length
and pump power.
IV. RESULTS AND DISCUSSIONS
The pump power is different to be in range 100 mW and
510 mW, by varying the wavelength of each channels in
ranging between 1545-1560 nm, the corresponding gains
and noise figure data obtained from dual port WDM
analyzer(both are in dB) are plotted in figure 2 and
figure 3 respectively.
Figure 3 shows the variation of noise figure for different
pump powers. Here it is visualized that for low pump
power noise figure is high and chances of distortion in
signal increases. Table 1 shows the average values of
noise figure for different pump power values.
Fig.2: Variation of Gain along the wavelength for
different pump powers at a constant input power
Fig.3: Variation of Noise figure along the wavelength for
different pump powers at constant input power
Table 1. Average gain and noise figure values for
different pump powers
Pump
Power
200
mW
300
mW
400
mW
510
mW
Avg
Gain(dB)
37.657 39.448 40.666 41.665
Avg
NF(dB)
7.093 6.886 6.783 6.714
Figure 4 shows the variation of Gain for different input
powers. Here it is visualized that for low input power gain
Figure 2 shows that the EDFA gain increases as pump
power increases. The average gain values for different
pump powers are shown in Table 1. As we can see that
the highest flattened gain which is around 41 dB is
achieved for a pump power of 510mW with an optimized
fiber length of 6.245 m and most importantly the
frequency spacing between channels is reduced to 0.424
nm which is a quite effective step in order to save
bandwidth.
International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016]
Infogain Publication (Infogainpublication.com) ISSN : 2454-1311
www.ijaems.com Page | 27
is low and on increasing input power the amount of gain
flatness increases considerably.
Table 2: EDFA-DWDM Parameters
Fig. 4: Variation of Gain along the wavelength for
different input powers at a constant pump power
Figure 5 shows the variation of noise figure for different
input powers. Here it is visualized that for low input
power noise figure is high and on increasing input power
the amount of noise figure increases considerably.
Fig. 5: Variation of Noise figure along the wavelength for
different input powers at constant pump power
V. CONCLUSION
In this paper, flattened gain EDFA-DWDM system
designed for 32 channels in wavelength range from 1546-
1560 nm. and it is observed that population inversion of
Er+3
ions can be controlled by properly choosing the
injected pump power of CW laser and doping of Er+3
to
EDFA. It is found that the optimized Er+3
doped fiber
length is 6.245 m whereas the optimum pump power is
510mW to flat the gain within 41+0.9dB for 0.424 nm
frequency spacing between transmitting channels. The
output power at EDFA 7.9188 dB and an average noise
figure is 6.714686dB.It is also found that this system also
provides maximum EDFA gain at lowest attenuation
wavelength of optical fiber i.e 1.55µm.
REFERENCES
[1] Deepika Verma and Santosh Meena, ‘Flattening the
Gain in 16 Channel EDFA-WDM System By Gain
Flattening Filter’, 2014 Sixth International
Conference on Computational Intelligence and
Communication Networks, IEEE,174-177
[2] Farah Diana Binti Mahad and Abu Sahmah Bin
Mohd Supa, ‘EDFA Gain Optimization for WDM
System’, ELEKTRIKA, VOL. 11, NO. 1, 2009, 34-
37
[3] P. NagaSiva Kumar, A. Sangeetha, ‘Gain Flatness of
EDFA in WDM Systems’, International conference
on Communication and Signal Processing, April 3-5,
2013, India,IEEE,713-716
[4] S. Semmalar, Poonkuzhali, P.Devi, ‘Optimized Gain
EDFA of different Lengths with aninfluence of
Pump Power’, 2011 IEEE,90-95
[5] M.A Othman, M.M.I smail, H.A. sulaiman, M.H.
Misran, M.A.M said,’EDFA-WDM optical network
analysis’,International journal of Electronics and
computer science engineering,1894-1904.
Parameters Values(Units)
Number of Channels 32
WDM transmitter frequency 1546 nm
WDM transmitter freq. spacing 0.4 nm
WDM Bandwidth 10GHz
Modulation type NRZ
EDFA optimized length 6.245 m
EDFA core radius 2.2µm
Er+3
ion density 1.425e+025 m-3
Numerical aperture 0.24
International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016]
Infogain Publication (Infogainpublication.com) ISSN : 2454-1311
www.ijaems.com Page | 28
[6] Warsha Balani, Mniash Saxena, “Simulation and
Analysiis of GFF at WDM MUX Bandwidth of
13GHz”, International journal of Computational
Intelligence and Informatics, Vol.2 No ,January-
March 2013.
[7] Y. Sun, A. K. Srivastava, J. Zhou, and J. W. Sulhoff,
“Optical fibre amplifiers for WDM optical
networks”, Bell Labs. Tech. J., vol. 4, pp.187-206,
1999.
[8] Inderpreet Kaur and Neena Gupta, “A Novel
Approach for Performance of DWDM Systems
Using TDFAEDFA Configuration”, International
Journal of Electronics and Communication
Technology, Vol.1, Issue 1, December 2010.
[9] Kamalbir Kaur, Kulwinder Singh, “Performance
analysis of 16- channel WDM system using Erbium
Doped Fiber Amplifier”, International Journal of
Engineering and Innovative Technology (IJEIT)
Volume 3, Issue 6, December 2013
[10]Warsha Balani, Mniash Saxena, “Simulation and
Analysiis of GFF at WDM MUX Bandwidth of
13GHz”, International journal of Computational
Intelligence and Informatics, Vol.2 No ,January-
March 2013.

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5 Simulation of Gain flattening 32 channels EDFA-DWDM Optical System

  • 1. International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016] Infogain Publication (Infogainpublication.com) ISSN : 2454-1311 www.ijaems.com Page | 25 Simulation of Gain flattening 32 channels EDFA- DWDM Optical System Amit Patni, Durgesh Kumar Department of ECE, Poornima college of Engineering, Jaipur, India Abstract—The gain flatness of EDFA plays a very critical role in DWDM system applications in all optical network design. The main purpose of this paper is to achieve gain flatness for 32 channels in order to equalize amplitude gain of DWDM system. This system is simulated using Opti system software to achieve gain flatness of EDFA through variation of EDFA pump power and input power of system. The gains are flattened within 41±0.9 dB from Wavelength range 1546 to 1560 nm having noise figure less than 8dB, Optimized EDFA fiber length of 6.245 m and frequency spacing between channels is 0.4 nm simultaneously amplified in a EDFA of single stage. The working model consists of WDM transmitter , MUX, Pump laser, dual port WDM analyzer and EDFA as key components Keywords—EDFA(Er+3 doped fiber amplifier), DWDM(Dense wavelength division multiplexing), Pump power, Input power , NF(Noise figure) I. INTRODUCTION As now a days ,to facilitate high speed network services we require large amount of bandwidth, so EDFA are used extensively in WDM-DWDM technology which increases the capacity of optical network with high speed without affecting any cost. EDFA is an optical amplifier which uses generally Er+3 doped optical fiber as a gain medium to amplify an optical signal with multiplexed pump laser and signal is amplified through interaction of doping ions The main characteristic of it is that its operating wavelength is 1.55µm as we know that this wavelength related to third window of optical communication which shows lowest attenuation comparatively to another optical communication Transmitting window. The technical characteristics of EDFA include Efficient pumping, Low noise, High Gain, Low distortion and minimal inter channel crosstalk High output power (this is not gain but amount of possible output power) and most importantly it amplifies the data channels with high data rates in optical domain and in operating range of optical fibers. The gain of optical system depends on the wavelength which can effect system’s performance and due to unequal gain spectrum of optical amplifiers, this can unbalance the powers in the transmitted WDM channels so by equalizing gain of amplifier we can achieve error free detection of signals transmitted through optical link. There are several methods through which optical flat spectral gain can be designed such as by altering the pump power, by controlling fiber length, by variation of input power and by properly choosing optical notch filter characteristics. In this paper, the gain flatness of EDFA is achieved by variation of pump power and input power for a fixed fiber length of 10 km and average output power of more than 7dBm. II. METHOD Figure 1 shows the block diagram of EDFA-DWDM System design which includes WDM transmitter, MUX, Pump laser, dual port WDM analyzer , EDFA as key components in the wavelength region of 1546-1560 nm having single pumping power using wavelengths between 980-1480 nm. This model has been computed, simulated and analyzed with varying parameters of gain and noise figure. The gain flatness and system stability of 980 nm pump laser wavelength has been obtained maximum compared to 1480 nm wavelength. Fig.1: Block diagram of EDFA-DWDM system design with single pumping source
  • 2. International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016] Infogain Publication (Infogainpublication.com) ISSN : 2454-1311 www.ijaems.com Page | 26 III. BACKGROUND EDFA are always a prime choice to use them as optical amplifiers because of their capability to amplify signal in optical domain without converting into electrical signal. By using EDFA, the transmission distance and capacity of optical system increases and their characteristic is to provide flat gain over a range of frequencies. In this context Paper [1] proposed a model that provides flat gain of around 27dB for 16 channel WDM system maintaining frequency spacing between channels to 0.8 nm by using Gain flattening filer(GFF). In Paper [2] gains are flattened to around 24dB for 16 channel WDM system maintaining frequency spacing between channels to 0.8 nm by studying variation of Fiber length and pump power. In paper [3], the system is simulated to achieve gain flatness of 16 channel EDFA-WDM through optimized fiber length and pump power .The gains are flattened between 24+0.3dB from 1546 to 1558 nm band of wavelength and noise figure less than 6dB obtained. Paper [4] describes the simulation models of EDFA Gain of different Pump powers. Here, EDFA length of 10m and pump power of 220mW gives the gain of 40.17dB , pump power of 620mW gives the gain of 44.3dB and pump power of 1000mW gives the gain of 46 dB. Paper [5] proposed a simulation model that provides EDFA-WDM flattened gain to around 38dB and noise figure<9dB for 16 channels by variation of fiber length and pump power. IV. RESULTS AND DISCUSSIONS The pump power is different to be in range 100 mW and 510 mW, by varying the wavelength of each channels in ranging between 1545-1560 nm, the corresponding gains and noise figure data obtained from dual port WDM analyzer(both are in dB) are plotted in figure 2 and figure 3 respectively. Figure 3 shows the variation of noise figure for different pump powers. Here it is visualized that for low pump power noise figure is high and chances of distortion in signal increases. Table 1 shows the average values of noise figure for different pump power values. Fig.2: Variation of Gain along the wavelength for different pump powers at a constant input power Fig.3: Variation of Noise figure along the wavelength for different pump powers at constant input power Table 1. Average gain and noise figure values for different pump powers Pump Power 200 mW 300 mW 400 mW 510 mW Avg Gain(dB) 37.657 39.448 40.666 41.665 Avg NF(dB) 7.093 6.886 6.783 6.714 Figure 4 shows the variation of Gain for different input powers. Here it is visualized that for low input power gain Figure 2 shows that the EDFA gain increases as pump power increases. The average gain values for different pump powers are shown in Table 1. As we can see that the highest flattened gain which is around 41 dB is achieved for a pump power of 510mW with an optimized fiber length of 6.245 m and most importantly the frequency spacing between channels is reduced to 0.424 nm which is a quite effective step in order to save bandwidth.
  • 3. International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016] Infogain Publication (Infogainpublication.com) ISSN : 2454-1311 www.ijaems.com Page | 27 is low and on increasing input power the amount of gain flatness increases considerably. Table 2: EDFA-DWDM Parameters Fig. 4: Variation of Gain along the wavelength for different input powers at a constant pump power Figure 5 shows the variation of noise figure for different input powers. Here it is visualized that for low input power noise figure is high and on increasing input power the amount of noise figure increases considerably. Fig. 5: Variation of Noise figure along the wavelength for different input powers at constant pump power V. CONCLUSION In this paper, flattened gain EDFA-DWDM system designed for 32 channels in wavelength range from 1546- 1560 nm. and it is observed that population inversion of Er+3 ions can be controlled by properly choosing the injected pump power of CW laser and doping of Er+3 to EDFA. It is found that the optimized Er+3 doped fiber length is 6.245 m whereas the optimum pump power is 510mW to flat the gain within 41+0.9dB for 0.424 nm frequency spacing between transmitting channels. The output power at EDFA 7.9188 dB and an average noise figure is 6.714686dB.It is also found that this system also provides maximum EDFA gain at lowest attenuation wavelength of optical fiber i.e 1.55µm. REFERENCES [1] Deepika Verma and Santosh Meena, ‘Flattening the Gain in 16 Channel EDFA-WDM System By Gain Flattening Filter’, 2014 Sixth International Conference on Computational Intelligence and Communication Networks, IEEE,174-177 [2] Farah Diana Binti Mahad and Abu Sahmah Bin Mohd Supa, ‘EDFA Gain Optimization for WDM System’, ELEKTRIKA, VOL. 11, NO. 1, 2009, 34- 37 [3] P. NagaSiva Kumar, A. Sangeetha, ‘Gain Flatness of EDFA in WDM Systems’, International conference on Communication and Signal Processing, April 3-5, 2013, India,IEEE,713-716 [4] S. Semmalar, Poonkuzhali, P.Devi, ‘Optimized Gain EDFA of different Lengths with aninfluence of Pump Power’, 2011 IEEE,90-95 [5] M.A Othman, M.M.I smail, H.A. sulaiman, M.H. Misran, M.A.M said,’EDFA-WDM optical network analysis’,International journal of Electronics and computer science engineering,1894-1904. Parameters Values(Units) Number of Channels 32 WDM transmitter frequency 1546 nm WDM transmitter freq. spacing 0.4 nm WDM Bandwidth 10GHz Modulation type NRZ EDFA optimized length 6.245 m EDFA core radius 2.2µm Er+3 ion density 1.425e+025 m-3 Numerical aperture 0.24
  • 4. International Journal of Advanced Engineering, Management and Science (IJAEMS) [Vol-2, Issue-3, March- 2016] Infogain Publication (Infogainpublication.com) ISSN : 2454-1311 www.ijaems.com Page | 28 [6] Warsha Balani, Mniash Saxena, “Simulation and Analysiis of GFF at WDM MUX Bandwidth of 13GHz”, International journal of Computational Intelligence and Informatics, Vol.2 No ,January- March 2013. [7] Y. Sun, A. K. Srivastava, J. Zhou, and J. W. Sulhoff, “Optical fibre amplifiers for WDM optical networks”, Bell Labs. Tech. J., vol. 4, pp.187-206, 1999. [8] Inderpreet Kaur and Neena Gupta, “A Novel Approach for Performance of DWDM Systems Using TDFAEDFA Configuration”, International Journal of Electronics and Communication Technology, Vol.1, Issue 1, December 2010. [9] Kamalbir Kaur, Kulwinder Singh, “Performance analysis of 16- channel WDM system using Erbium Doped Fiber Amplifier”, International Journal of Engineering and Innovative Technology (IJEIT) Volume 3, Issue 6, December 2013 [10]Warsha Balani, Mniash Saxena, “Simulation and Analysiis of GFF at WDM MUX Bandwidth of 13GHz”, International journal of Computational Intelligence and Informatics, Vol.2 No ,January- March 2013.