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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4444
Reduction of dispersion using FBG in fiber optic communication
Sabapathi T 1, Muthu Ilamathi N 2, Divya A3
1 Associate Professor,ECE Dept., Mepco Schlenk Engineering College, Sivakasi, Tamilnadu, India
2B.E., Student Mepco Schlenk Engineering College, Sivakasi, Tamilnadu, India
3B.E., Student Mepco Schlenk Engineering College, Sivakasi, Tamilnadu, India
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract – Fiber optic transmissions are facing many
difficulties that limited its ability for long distances. One of
these difficulties is the degradation that occurs when an
optical signal passes through the optical fiber. The causes of
degradation are power attenuation, dispersion and
nonlinear effects. Degradation in the system has to be
minimized to support long haul transmission distance with
high capacity. The effect of the degradation is studied and
analyzed based on the BER and Eye Diagram obtained at
the speed of 10 Gbps. The losses on the transmitted signals
are eliminated by an optical amplifier. The results also
show that Chromatic dispersion is the most significant effect
of degradation phenomenon. Commonly used important
component to compensate the dispersion in optical
communication system is Fiber Bragg Grating. Reflection
and filtering are the main functions of Fiber Bragg Grating.
FBG has low cost filter for wavelength selection and low
insertion loss and wide bandwidth. The simulation of
transmission system will be analysed based on different
parameters by using OptiSystem 7.0 simulator.
Key Words: Fiber Bragg Grating, Degradation, Eye
Diagram, Chromatic dispersion, Long Haul transmission
1. INTRODUCTION
By using fiber optic communication the
information or data transmitted from one place to another
through an optical fiber. It is similar to an optical wire
made it as the most acceptable for the communication
channel. Three basic elements of optical communication
are fiber media, input light sources and detector as the
output. In optical communication the signal degradation is
the most important phenomenon. Signal degradation
includes power attenuation, pulse broadening, and fiber
non-linearities. Power attenuation is the loss of power
introduced by the fiber. The dispersion is also called as
spreading of pulses as they travel through the fiber, it
degrades the system performance by broadening of optical
pulses as they propagate inside the optical fiber. If their
parameter depends on the intensity an optical effect is
called as nonlinear, these effects depend on the
transmission length and there are two main nonlinear
categories Stimulated light Scattering and Nonlinear Phase
Modulation. The key component of optical communication
system is FBG and they are used as dispersion
compensator, filters and flatteners gain. FBG is very
attractive components because as well as being passive,
linear and compact, retain strong dispersion in both
reflection and transmission. The maximum compression
ratio is achieved by using Fiber Bragg Grating. The overall
losses non-linear effects and costs of optical transmission
system are increased by using DCF. FBG helps to
decreasing the system cost and also have lower insertion
loss. In fiber optic communication Wave Division
Multiplexing is a technology which multiplexes many
number of optical signals on a single optical fiber by using
different of light sources to carry different signals. OADM
is a device used in WDM system for multiplexing and
routing different channels of light into or out of a single
mode fiber [9]. Programmable version of OADM is called
as ROADM.For simulation the most suitable settings of the
system should be used which include input power (dBm),
fiber cable length (km) and attenuation coefficient (dB/km).
2 DISPERSION COMPENSATION
The dispersion or pulse broadening has to be
compensated as it may produce Inter symbol
interference and increase the Bit error rate. There
are various mechanisms for compensating the
dispersion.
2.1 Fiber Bragg Grating (FBG):
Fiber Bragg grating constructed in a short segment
of optical fiber is a distributed Bragg reflector it will reflect
the particular wavelength and the remaining wavelength
will be transmitted as shown in Fig. 2.1. The refractive
index of the fiber core is achieved by producing a periodic
variations, it creates a wavelength-specific dielectric
mirror. Chirped Fiber Bragg Grating is one of most
important components for chromatic dispersion
compensation. Fiber Bragg Grating is commonly used and
low cost filter for wavelength selection. Fiber Bragg
Grating has a several applications to improve the
standard and reduce the costs in optical networks[1]. The
operation of FBG is reflection and filtering techniques and
they have a high efficiency and low losses. Chromatic
dispersion can be reduced with the help of Fiber Bragg
Grating. To compensate chromatic dispersion in a
communication system, the final expected effect is
compressed in incident pulse. Fiber Bragg Grating act as a
single mode it will expose the core to the periodic pattern
of intense UV light. The exposure will increase the
refractive index so that refractive index is permanently
increased. So that exposure pattern will produce fixed
index modulation called as a grating. Due to the changes in
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4445
the periodic refraction, a small reflected light rays will be
produced. Then, the small reflected light rays will be
combined into a large reflected light rays. When the grating
period is approximately half the input light wavelength
which is called Bragg’s wavelength. The other light (except
the Bragg’s light) will be able to see. The longer
wavelength light move slowly than the shorter wavelength
light because of pulse broadening. Because of high data
rates and fiber lengths, the pulses in a data stream will
tends to be overlap. Like that, fiber dispersion limits the
higher data that can be transmitted through a fiber optic
cable.
Fig 2.1: Dispersion compensation
mechanism
The use of Fiber Bragg Grating shown in Figure 2.1
is to compensate the chromatic dispersion in an optical
fiber communication. The transit times of different
wavelengths in a pulse regulate the grating serves as a
particular optical delay line. So that they are
approximately equal. The faster wave lengths are travel at
a longer distance and the shorter wave lengths are travel at
a shorter distance [3].
Fig 2: Dispersion compensation using FBG
3 Dispersion Compensation Fiber (DCF):
In recent years there has been a lot of work on
dispersion-compensating fibers (DCFs), which are being
used extensively for enhancing the installed 1310 nm
optimized optical fiber links for operation at 1550 nm.
The first step will be designing and simulation of the pre,
post and symmetric dispersion compensation. This will be
done by using OptiSystem software version 7.0. First we
completely study about the software will be done. The
OptiSystem software is user friendly to work, flexible, and
fast and the OptiSystem components library consists many
components that can be measured from design of real
devices. The parameters such as bit rate, fiber length,
sensitivity and dispersion parameters will be varied to
achieve best BER by using model design in OptiSystem
software. By using the OptiSystem software the
Comparison analysis of systems will be done. The BER
analyser is used to analyse the BER and eye diagrams. We
will discuss three dispersion compensation techniques in
this research paper to compensate fiber dispersion, there
are pre-, post-, and symmetrical compensation. In this
simulations, NRZ modulation formats are used and
receiver sensitivity for 2.5 Gbps is -28 dBm and for 10
Gbps -25 dBm.
3.1 . Pre DCF
The layout involving the pre DCF is shown in Fig. 3.1 and
the BER for various transmitted optical power is shown in
Table 3.1.
Fig 3.1: Pre DCF
The layout for Post DCF is shown in fig. 3.2. The layout for
Symmetrical DCF is shown in fig. 3.3.
Fig 3.2: Post DCF
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4446
Fig 3.3: Symmetrical DCF
Table 3.1 :Observation of BER for various
Transmitted power
Powe
r
(dBm
)
DCF
FBG
pre Post
symmetri
cal
0 1.149x10-10 8.189x10-11 2.3250-15
1.09x10-
24
1 7.804x10-11 5.564x10-11
3.368x10-
17
7.11x10-
26
2 5.579x10-11 3.581x10-11
5.239x10-
19
6.22x10-
27
3 3.75x10-11 2.216x10-11
1.029x10-
20
6.36x10-
28
4 2.589x10-11 1.245x10-11
2.843x10-
22
6.66x10-
29
5 1.581x10-11 6.239x10-12 1.58470-23 5.8410-30
4. OPTICAL ADD-DROP MULTIPLEXING
Optical add-drop multiplexer (OADM) is a device
used in WDM systems for various techniques as
multiplexing and routing the different channels of light
into or out of an optical network. Add and drop device has
the capacity to add one or more new wavelength channels
to an existing multi wavelength WDM signal. And it is used
to drop one or more channels, passing those signals to
another network path. An OADM has a various
specification, one of the important specific type is an
optical cross connects. An OADM consists of an optical
multiplexer and an optical demultiplexer and
reconfiguration is present in between the multiplexer and
demultiplexer and a set of ports are present for adding
and dropping signals. The OADM can be realized by
several ways.
The OADM layout with 4 channels is shown in Fig.
4.1. The evaluation of BER in different channels for various
power levels is shown in Table 4.1.
Fig 4.1: OADM with 4-channels
Table 4.1 Observation: BER in different channels
POWER
(dBm)
BER
Channel 1
Channel
2
Channel 3
Channel
4
0 0.000474 0.00036 4.668x10-5 4.082x10-5
1 1.642x10-5 8.665x10-6 4.893x10-7 3.318x10-7
2 8.640x10-8 7.460x10-8 7.172x10-10
1.675x10-
10
3
2.735x10-
11
1.958x10-
11
8.740x10-15
1.013x10-
15
4
8.925x10-
17
1.076x10-
16
2.363x10-22
6.961x10-
24
3. CONCLUSIONS
We have analyzed the dispersion compensation
using Fiber Bragg Grating (FBG) and DCF at different
transmission power. The transmission systems have been
analyzed on the basic of different parameters. By
simulating a communication system and using the
acceptable settings of the system which include input
power (dBm), fiber length (km), grating Length (mm) and
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4447
dispersion parameters. We design a OADM system to
improve the efficiency of WDM system. All the results are
analyzed by using OPTISYSTEM 7.0 software. From the
result we found FBG is the best dispersion compensator
compared to DCF.
REFERENCES
S. O. Mohammadi, Saeed Mozzaffari and M. Mahdi Shahidi,
“Simulation of a transmission system to compensate
dispersion in an optical fiber by chirp gratings.”
International Journal of the Physical Sciences, Vol.
6(32), pp. 7354 - 7360, 2 December, 2011.
Sachin dev, Col. (Dr.) Suresh Kumar, “Dispersion
Compensation in Optical Fiber Communication using
Bragg Grating” International Journal of Engineering
Technology Science and Research, Volume 3, Issue 9
September 2016.
Mohamed A. A. Elmaleeh, Fadal Alla G.S. Gamar, Amin B. A.
Mustafa, “Minimization of signal degradation in single
mode fibre optic link” International Journal of Latest
Research in Science and Technology, Volume 3, Issue
5: Page No 95-102. September-October 2014.
Dar, A. B., Jha, R. K., “ Design and comparative performance
analysis of different chirping profiles of tanh apodized
fiber Bragg grating and comparison with the
dispersion compensation fiber for long-haul
transmission system” J. Mod. Opt. 64(6), 555–566
(2017).
Y. Yu, P. D. Townsend, J. Zhao, "Equalization of dispersion-
induced crosstalk in optical offset-QAM OFDM
systems", IEEE Photon. Technol. Lett., vol. 28, no. 7,
pp. 782-785, Apr. 2016.
Bibhu Prasad , Dr. K. C. Patra, Dr. N.K Barpanda
“Performance Analysis of Fiber Optical
Communication using Fiber Bragg Grating as
Dispersion Compensator” IJAREEIE Vol. 5, Issue 4,
April 2016.
Y. Zhou, Y. Shao, Z. Wang, C. Li, J. Zhou, and W. Ma,
“Research on Dispersion Compensation of 40 GB/s
Optical Duo-Binary Coded Transmission System,”
Optics and Photonics Journal, Vol. 6, pp. 190 - 195,
August 2016.
R. Mishra, N.K. Shukla, and C.K. Dwivedi, “A Comparative
Performance Analysis of Optical Fiber System with
FBG Compensated SMF for High Data Rate,” Imperial
Journal of Interdisciplinary Research, Vol.2, no7, 2016.
Sily S. Kumar and P. Keerthana, “Simulation of RoF Using
Wavelength Selective OADM” International Journal of
Research Studies in Science, Engineering and
Technology Volume 2, Issue 9, PP 16-22, September
2015.
[10]Dwaipayan Dey and Neha, “Compensation in Optical
Fiber WDM System Using Different Compensation
Techniques” International Journal of Advanced
Research
in Computer Science and Software Engineering, Vol.4,
Issue 5, May 2014.

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  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4444 Reduction of dispersion using FBG in fiber optic communication Sabapathi T 1, Muthu Ilamathi N 2, Divya A3 1 Associate Professor,ECE Dept., Mepco Schlenk Engineering College, Sivakasi, Tamilnadu, India 2B.E., Student Mepco Schlenk Engineering College, Sivakasi, Tamilnadu, India 3B.E., Student Mepco Schlenk Engineering College, Sivakasi, Tamilnadu, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract – Fiber optic transmissions are facing many difficulties that limited its ability for long distances. One of these difficulties is the degradation that occurs when an optical signal passes through the optical fiber. The causes of degradation are power attenuation, dispersion and nonlinear effects. Degradation in the system has to be minimized to support long haul transmission distance with high capacity. The effect of the degradation is studied and analyzed based on the BER and Eye Diagram obtained at the speed of 10 Gbps. The losses on the transmitted signals are eliminated by an optical amplifier. The results also show that Chromatic dispersion is the most significant effect of degradation phenomenon. Commonly used important component to compensate the dispersion in optical communication system is Fiber Bragg Grating. Reflection and filtering are the main functions of Fiber Bragg Grating. FBG has low cost filter for wavelength selection and low insertion loss and wide bandwidth. The simulation of transmission system will be analysed based on different parameters by using OptiSystem 7.0 simulator. Key Words: Fiber Bragg Grating, Degradation, Eye Diagram, Chromatic dispersion, Long Haul transmission 1. INTRODUCTION By using fiber optic communication the information or data transmitted from one place to another through an optical fiber. It is similar to an optical wire made it as the most acceptable for the communication channel. Three basic elements of optical communication are fiber media, input light sources and detector as the output. In optical communication the signal degradation is the most important phenomenon. Signal degradation includes power attenuation, pulse broadening, and fiber non-linearities. Power attenuation is the loss of power introduced by the fiber. The dispersion is also called as spreading of pulses as they travel through the fiber, it degrades the system performance by broadening of optical pulses as they propagate inside the optical fiber. If their parameter depends on the intensity an optical effect is called as nonlinear, these effects depend on the transmission length and there are two main nonlinear categories Stimulated light Scattering and Nonlinear Phase Modulation. The key component of optical communication system is FBG and they are used as dispersion compensator, filters and flatteners gain. FBG is very attractive components because as well as being passive, linear and compact, retain strong dispersion in both reflection and transmission. The maximum compression ratio is achieved by using Fiber Bragg Grating. The overall losses non-linear effects and costs of optical transmission system are increased by using DCF. FBG helps to decreasing the system cost and also have lower insertion loss. In fiber optic communication Wave Division Multiplexing is a technology which multiplexes many number of optical signals on a single optical fiber by using different of light sources to carry different signals. OADM is a device used in WDM system for multiplexing and routing different channels of light into or out of a single mode fiber [9]. Programmable version of OADM is called as ROADM.For simulation the most suitable settings of the system should be used which include input power (dBm), fiber cable length (km) and attenuation coefficient (dB/km). 2 DISPERSION COMPENSATION The dispersion or pulse broadening has to be compensated as it may produce Inter symbol interference and increase the Bit error rate. There are various mechanisms for compensating the dispersion. 2.1 Fiber Bragg Grating (FBG): Fiber Bragg grating constructed in a short segment of optical fiber is a distributed Bragg reflector it will reflect the particular wavelength and the remaining wavelength will be transmitted as shown in Fig. 2.1. The refractive index of the fiber core is achieved by producing a periodic variations, it creates a wavelength-specific dielectric mirror. Chirped Fiber Bragg Grating is one of most important components for chromatic dispersion compensation. Fiber Bragg Grating is commonly used and low cost filter for wavelength selection. Fiber Bragg Grating has a several applications to improve the standard and reduce the costs in optical networks[1]. The operation of FBG is reflection and filtering techniques and they have a high efficiency and low losses. Chromatic dispersion can be reduced with the help of Fiber Bragg Grating. To compensate chromatic dispersion in a communication system, the final expected effect is compressed in incident pulse. Fiber Bragg Grating act as a single mode it will expose the core to the periodic pattern of intense UV light. The exposure will increase the refractive index so that refractive index is permanently increased. So that exposure pattern will produce fixed index modulation called as a grating. Due to the changes in
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4445 the periodic refraction, a small reflected light rays will be produced. Then, the small reflected light rays will be combined into a large reflected light rays. When the grating period is approximately half the input light wavelength which is called Bragg’s wavelength. The other light (except the Bragg’s light) will be able to see. The longer wavelength light move slowly than the shorter wavelength light because of pulse broadening. Because of high data rates and fiber lengths, the pulses in a data stream will tends to be overlap. Like that, fiber dispersion limits the higher data that can be transmitted through a fiber optic cable. Fig 2.1: Dispersion compensation mechanism The use of Fiber Bragg Grating shown in Figure 2.1 is to compensate the chromatic dispersion in an optical fiber communication. The transit times of different wavelengths in a pulse regulate the grating serves as a particular optical delay line. So that they are approximately equal. The faster wave lengths are travel at a longer distance and the shorter wave lengths are travel at a shorter distance [3]. Fig 2: Dispersion compensation using FBG 3 Dispersion Compensation Fiber (DCF): In recent years there has been a lot of work on dispersion-compensating fibers (DCFs), which are being used extensively for enhancing the installed 1310 nm optimized optical fiber links for operation at 1550 nm. The first step will be designing and simulation of the pre, post and symmetric dispersion compensation. This will be done by using OptiSystem software version 7.0. First we completely study about the software will be done. The OptiSystem software is user friendly to work, flexible, and fast and the OptiSystem components library consists many components that can be measured from design of real devices. The parameters such as bit rate, fiber length, sensitivity and dispersion parameters will be varied to achieve best BER by using model design in OptiSystem software. By using the OptiSystem software the Comparison analysis of systems will be done. The BER analyser is used to analyse the BER and eye diagrams. We will discuss three dispersion compensation techniques in this research paper to compensate fiber dispersion, there are pre-, post-, and symmetrical compensation. In this simulations, NRZ modulation formats are used and receiver sensitivity for 2.5 Gbps is -28 dBm and for 10 Gbps -25 dBm. 3.1 . Pre DCF The layout involving the pre DCF is shown in Fig. 3.1 and the BER for various transmitted optical power is shown in Table 3.1. Fig 3.1: Pre DCF The layout for Post DCF is shown in fig. 3.2. The layout for Symmetrical DCF is shown in fig. 3.3. Fig 3.2: Post DCF
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4446 Fig 3.3: Symmetrical DCF Table 3.1 :Observation of BER for various Transmitted power Powe r (dBm ) DCF FBG pre Post symmetri cal 0 1.149x10-10 8.189x10-11 2.3250-15 1.09x10- 24 1 7.804x10-11 5.564x10-11 3.368x10- 17 7.11x10- 26 2 5.579x10-11 3.581x10-11 5.239x10- 19 6.22x10- 27 3 3.75x10-11 2.216x10-11 1.029x10- 20 6.36x10- 28 4 2.589x10-11 1.245x10-11 2.843x10- 22 6.66x10- 29 5 1.581x10-11 6.239x10-12 1.58470-23 5.8410-30 4. OPTICAL ADD-DROP MULTIPLEXING Optical add-drop multiplexer (OADM) is a device used in WDM systems for various techniques as multiplexing and routing the different channels of light into or out of an optical network. Add and drop device has the capacity to add one or more new wavelength channels to an existing multi wavelength WDM signal. And it is used to drop one or more channels, passing those signals to another network path. An OADM has a various specification, one of the important specific type is an optical cross connects. An OADM consists of an optical multiplexer and an optical demultiplexer and reconfiguration is present in between the multiplexer and demultiplexer and a set of ports are present for adding and dropping signals. The OADM can be realized by several ways. The OADM layout with 4 channels is shown in Fig. 4.1. The evaluation of BER in different channels for various power levels is shown in Table 4.1. Fig 4.1: OADM with 4-channels Table 4.1 Observation: BER in different channels POWER (dBm) BER Channel 1 Channel 2 Channel 3 Channel 4 0 0.000474 0.00036 4.668x10-5 4.082x10-5 1 1.642x10-5 8.665x10-6 4.893x10-7 3.318x10-7 2 8.640x10-8 7.460x10-8 7.172x10-10 1.675x10- 10 3 2.735x10- 11 1.958x10- 11 8.740x10-15 1.013x10- 15 4 8.925x10- 17 1.076x10- 16 2.363x10-22 6.961x10- 24 3. CONCLUSIONS We have analyzed the dispersion compensation using Fiber Bragg Grating (FBG) and DCF at different transmission power. The transmission systems have been analyzed on the basic of different parameters. By simulating a communication system and using the acceptable settings of the system which include input power (dBm), fiber length (km), grating Length (mm) and
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072 © 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4447 dispersion parameters. We design a OADM system to improve the efficiency of WDM system. All the results are analyzed by using OPTISYSTEM 7.0 software. From the result we found FBG is the best dispersion compensator compared to DCF. REFERENCES S. O. Mohammadi, Saeed Mozzaffari and M. Mahdi Shahidi, “Simulation of a transmission system to compensate dispersion in an optical fiber by chirp gratings.” International Journal of the Physical Sciences, Vol. 6(32), pp. 7354 - 7360, 2 December, 2011. Sachin dev, Col. (Dr.) Suresh Kumar, “Dispersion Compensation in Optical Fiber Communication using Bragg Grating” International Journal of Engineering Technology Science and Research, Volume 3, Issue 9 September 2016. Mohamed A. A. Elmaleeh, Fadal Alla G.S. Gamar, Amin B. A. Mustafa, “Minimization of signal degradation in single mode fibre optic link” International Journal of Latest Research in Science and Technology, Volume 3, Issue 5: Page No 95-102. September-October 2014. Dar, A. B., Jha, R. K., “ Design and comparative performance analysis of different chirping profiles of tanh apodized fiber Bragg grating and comparison with the dispersion compensation fiber for long-haul transmission system” J. Mod. Opt. 64(6), 555–566 (2017). Y. Yu, P. D. Townsend, J. Zhao, "Equalization of dispersion- induced crosstalk in optical offset-QAM OFDM systems", IEEE Photon. Technol. Lett., vol. 28, no. 7, pp. 782-785, Apr. 2016. Bibhu Prasad , Dr. K. C. Patra, Dr. N.K Barpanda “Performance Analysis of Fiber Optical Communication using Fiber Bragg Grating as Dispersion Compensator” IJAREEIE Vol. 5, Issue 4, April 2016. Y. Zhou, Y. Shao, Z. Wang, C. Li, J. Zhou, and W. Ma, “Research on Dispersion Compensation of 40 GB/s Optical Duo-Binary Coded Transmission System,” Optics and Photonics Journal, Vol. 6, pp. 190 - 195, August 2016. R. Mishra, N.K. Shukla, and C.K. Dwivedi, “A Comparative Performance Analysis of Optical Fiber System with FBG Compensated SMF for High Data Rate,” Imperial Journal of Interdisciplinary Research, Vol.2, no7, 2016. Sily S. Kumar and P. Keerthana, “Simulation of RoF Using Wavelength Selective OADM” International Journal of Research Studies in Science, Engineering and Technology Volume 2, Issue 9, PP 16-22, September 2015. [10]Dwaipayan Dey and Neha, “Compensation in Optical Fiber WDM System Using Different Compensation Techniques” International Journal of Advanced Research in Computer Science and Software Engineering, Vol.4, Issue 5, May 2014.