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INTERNATIONAL RESEARCH JOURNAL OF ENGINEERING AND TECHNOLOGY (IRJET) E-ISSN: 2395 -0056
VOLUME: 04 ISSUE: 03 | MAR -2017 WWW.IRJET.NET P-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 385
Performance Analysis and Power Optimization for Optical Link Using
Different Modulation Techniques
Mansi Kalaria 1, Viral Mehta2, Ami Lavingia3
1Electronics & Communication Dept., SVBIT, Gujarat, India
2 Electronics & Communication Dept., SVBIT, Gujarat, India
3 Electronics & Communication Dept., SALTIER, Gujarat, India
-----------------------------------------------------------------------------***----------------------------------------------------------------------------
Abstract—Challenge faced by today's telecommunication
network is the increasing demand of bandwidth and data
rates. This rapid increase in data traffic in communication
system has accelerated the development of high capacity
optical fiber links, and the main barriers across these links
are the dispersion and various nonlinear effects. Even the
transmission limit is influenced due to distinctive scattering
issues and power attenuation existing in optical fiber. In this
paper optical fiber link at different transmission distance
upto 300km is studied using two different modulation
schemes. Paper shows the comparative analysis of two
modulation schemes Non-Return to Zero (NRZ) and Return
to Zero (RZ) for an optical network. The performance
analysis is done on the basis of BER, Q-factor and Eye
Diagram. Performance of link weakens as the transmission
distance increases. It is observed that RZ gives better
performance compared to NRZ modulation.
Keywords—Optical link; RZ; NRZ; Optisystem
I. INTRODUCTION
In single channel transmission the RZ coded transmission
achieves high performance because SPM can be
compensated with fiber dispersion effects. In this modern
time, the increasing traffic demands require larger
bandwidth for high data rate communication. The high
data rate transmission requires an increase in input launch
power. In this paper, performance analysis of an optical
communication system for 40 Gbps single mode
transmission is done. When we deal with high data rate
optical communication systems using SMF, the RZ
transmission is suited well than NRZ because RZ has more
compressed pulse version as compared to NRZ. EDFA
optical amplifiers are used for the amplification of optical
signals at various lengths of SMF. The transmission
distance is limited by dispersion and non linear effects. In
order to abolish dispersion effect, dispersion
compensating fiber (DCF) is used in channel of an optical
communication system.
The rest of the paper is organized as follows. Section 2
presents the architecture of simulated optical high speed
system. And a 40 Gbps optical link is constructed and
simulated by using Optisystem. In Section 3, the
performance of the 40 Gbps single span optical network is
analyzed. Finally, we conclude the paper in Section 4.
II. DESIGN AND SIMULATION SETUP
Proposed algorithm consists of a transmitter section with
different modulation schemes (RZ and NRZ), optical fiber,
receiver section and a BER analyzer to analyze the output
result. The transmitter section consists of pseudo random
bit sequence generator, optical source and Mach Zender
modulator.
In transmission channel single mode fiber and dispersion
compensating fiber along with optical amplifier is used.
The length of the optical Single Mode Fiber (SMF) is varied
and in accordance with the length of Dispersion
Compensating Fiber (DCF) will vary respectively according
to the equation
DSMF x LSMF = -DDCF x LDCF
Where,
DSMF = Dispersion Coefficient of Single Mode Fiber
LSMF = Length of Single Mode Fiber
DDCF = Dispersion Coefficient of Dispersion Compensating
Fiber
LDCF = Length of Dispersion Compensating Fiber
Out of the three DCF compensation techniques, we have
simulated our link using symmetric dispersion
compensation configuration.
In receiver section PIN photodetector for converting optical
signal to electrical signal is used followed by band pass
filter.
In order to analyze the impact of nonlinearities on the
optical fiber communication system, the transmission
length of the optical system is varied. The result is analyzed
using BER analyzer.
The simulation parameters are given as follows:
Parameters Value
Bit Rate 40 Gbps
Modulation Format RZ, NRZ
Transmission Distance 50 km x n spans (n=2,4,6)
INTERNATIONAL RESEARCH JOURNAL OF ENGINEERING AND TECHNOLOGY (IRJET) E-ISSN: 2395 -0056
VOLUME: 04 ISSUE: 03 | MAR -2017 WWW.IRJET.NET P-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 386
(km)
Length of SMF 50 km
Length of DCF 10 km
Dispersion coefficient of
SMF
17ps/nm/km
Dispersion coefficient of
DCF
-85ps/nm/km
DCF Scheme Symmetric
III. RESULTS
In this paper, we have simulated an optical link at 40 Gbps
bit rate using two different modulation schemes namely
Retutrn-to-Zero (RZ) and Non-Return-to-Zero(NRZ). The
distance is varied from 100 km to 300km to analyze the
performance to the link in terms of Q-factor, BER and eye
diagram.
Figure 1 shows the eye diagram of optical link using RZ and
NRZ modulation for 100 km fiber length.
(a)
(b)
Figure 1: Eye Diagram (a) NRZ (b) RZ
Figure 2 shows the eye diagram of optical link using RZ and
NRZ modulation for 200 km fiber length.
(a)
(b)
Figure 2: Eye Diagram (a) NRZ (b) RZ
Figure 3 shows the eye diagram of optical link using RZ and
NRZ modulation for 300 km fiber length.
(a)
(b)
Figure 3: Eye Diagram (a) NRZ (b) RZ
Table 1 shows Q-factor value for NRZ and RZ fat varied
fiber length.
INTERNATIONAL RESEARCH JOURNAL OF ENGINEERING AND TECHNOLOGY (IRJET) E-ISSN: 2395 -0056
VOLUME: 04 ISSUE: 03 | MAR -2017 WWW.IRJET.NET P-ISSN: 2395-0072
© 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 387
TABLE 1: Q-Factor
Modulation
Distance
100 km 200 km 300 km
NRZ 43.1771 13.3985 6.19741
RZ 64.9336 40.5856 28.2801
IV. CONCLUSION
In this paper single span optical link with various
modulation schemes namely NRZ and RZ at different
transmission distance is simulated. From the obtained
result, it is found that RZ modulation format shows the
better performance than other formats.
REFERENCES
[1] G. Eason, B. Noble, and I.N. Sneddon, “On certain
integrals of Lipschitz-Hankel type involving products
of Bessel functions,” Phil. Trans. Roy. Soc. London, vol.
A247, pp. 529-551, April 1955. (references)
[2] J. Clerk Maxwell, A Treatise on Electricity and
Magnetism, 3rd ed., vol. 2. Oxford: Clarendon, 1892,
pp.68-73.
[3] I.S. Jacobs and C.P. Bean, “Fine particles, thin films and
exchange anisotropy,” in Magnetism, vol. III, G.T. Rado
and H. Suhl, Eds. New York: Academic, 1963, pp. 271-
350.
[4] K. Elissa, “Title of paper if known,” unpublished.
[5] R. Nicole, “Title of paper with only first word
capitalized,” J. Name Stand. Abbrev., in press.
[6] Y. Yorozu, M. Hirano, K. Oka, and Y. Tagawa, “Electron
spectroscopy studies on magneto-optical media and
plastic substrate interface,” IEEE Transl. J. Magn. Japan,
vol. 2, pp. 740-741, August 1987 [Digests 9th Annual
Conf. Magnetics Japan, p. 301, 1982]

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Performance Analysis and Power Optimization for Optical Link Using Different Modulation Techniques

  • 1. INTERNATIONAL RESEARCH JOURNAL OF ENGINEERING AND TECHNOLOGY (IRJET) E-ISSN: 2395 -0056 VOLUME: 04 ISSUE: 03 | MAR -2017 WWW.IRJET.NET P-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 385 Performance Analysis and Power Optimization for Optical Link Using Different Modulation Techniques Mansi Kalaria 1, Viral Mehta2, Ami Lavingia3 1Electronics & Communication Dept., SVBIT, Gujarat, India 2 Electronics & Communication Dept., SVBIT, Gujarat, India 3 Electronics & Communication Dept., SALTIER, Gujarat, India -----------------------------------------------------------------------------***---------------------------------------------------------------------------- Abstract—Challenge faced by today's telecommunication network is the increasing demand of bandwidth and data rates. This rapid increase in data traffic in communication system has accelerated the development of high capacity optical fiber links, and the main barriers across these links are the dispersion and various nonlinear effects. Even the transmission limit is influenced due to distinctive scattering issues and power attenuation existing in optical fiber. In this paper optical fiber link at different transmission distance upto 300km is studied using two different modulation schemes. Paper shows the comparative analysis of two modulation schemes Non-Return to Zero (NRZ) and Return to Zero (RZ) for an optical network. The performance analysis is done on the basis of BER, Q-factor and Eye Diagram. Performance of link weakens as the transmission distance increases. It is observed that RZ gives better performance compared to NRZ modulation. Keywords—Optical link; RZ; NRZ; Optisystem I. INTRODUCTION In single channel transmission the RZ coded transmission achieves high performance because SPM can be compensated with fiber dispersion effects. In this modern time, the increasing traffic demands require larger bandwidth for high data rate communication. The high data rate transmission requires an increase in input launch power. In this paper, performance analysis of an optical communication system for 40 Gbps single mode transmission is done. When we deal with high data rate optical communication systems using SMF, the RZ transmission is suited well than NRZ because RZ has more compressed pulse version as compared to NRZ. EDFA optical amplifiers are used for the amplification of optical signals at various lengths of SMF. The transmission distance is limited by dispersion and non linear effects. In order to abolish dispersion effect, dispersion compensating fiber (DCF) is used in channel of an optical communication system. The rest of the paper is organized as follows. Section 2 presents the architecture of simulated optical high speed system. And a 40 Gbps optical link is constructed and simulated by using Optisystem. In Section 3, the performance of the 40 Gbps single span optical network is analyzed. Finally, we conclude the paper in Section 4. II. DESIGN AND SIMULATION SETUP Proposed algorithm consists of a transmitter section with different modulation schemes (RZ and NRZ), optical fiber, receiver section and a BER analyzer to analyze the output result. The transmitter section consists of pseudo random bit sequence generator, optical source and Mach Zender modulator. In transmission channel single mode fiber and dispersion compensating fiber along with optical amplifier is used. The length of the optical Single Mode Fiber (SMF) is varied and in accordance with the length of Dispersion Compensating Fiber (DCF) will vary respectively according to the equation DSMF x LSMF = -DDCF x LDCF Where, DSMF = Dispersion Coefficient of Single Mode Fiber LSMF = Length of Single Mode Fiber DDCF = Dispersion Coefficient of Dispersion Compensating Fiber LDCF = Length of Dispersion Compensating Fiber Out of the three DCF compensation techniques, we have simulated our link using symmetric dispersion compensation configuration. In receiver section PIN photodetector for converting optical signal to electrical signal is used followed by band pass filter. In order to analyze the impact of nonlinearities on the optical fiber communication system, the transmission length of the optical system is varied. The result is analyzed using BER analyzer. The simulation parameters are given as follows: Parameters Value Bit Rate 40 Gbps Modulation Format RZ, NRZ Transmission Distance 50 km x n spans (n=2,4,6)
  • 2. INTERNATIONAL RESEARCH JOURNAL OF ENGINEERING AND TECHNOLOGY (IRJET) E-ISSN: 2395 -0056 VOLUME: 04 ISSUE: 03 | MAR -2017 WWW.IRJET.NET P-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 386 (km) Length of SMF 50 km Length of DCF 10 km Dispersion coefficient of SMF 17ps/nm/km Dispersion coefficient of DCF -85ps/nm/km DCF Scheme Symmetric III. RESULTS In this paper, we have simulated an optical link at 40 Gbps bit rate using two different modulation schemes namely Retutrn-to-Zero (RZ) and Non-Return-to-Zero(NRZ). The distance is varied from 100 km to 300km to analyze the performance to the link in terms of Q-factor, BER and eye diagram. Figure 1 shows the eye diagram of optical link using RZ and NRZ modulation for 100 km fiber length. (a) (b) Figure 1: Eye Diagram (a) NRZ (b) RZ Figure 2 shows the eye diagram of optical link using RZ and NRZ modulation for 200 km fiber length. (a) (b) Figure 2: Eye Diagram (a) NRZ (b) RZ Figure 3 shows the eye diagram of optical link using RZ and NRZ modulation for 300 km fiber length. (a) (b) Figure 3: Eye Diagram (a) NRZ (b) RZ Table 1 shows Q-factor value for NRZ and RZ fat varied fiber length.
  • 3. INTERNATIONAL RESEARCH JOURNAL OF ENGINEERING AND TECHNOLOGY (IRJET) E-ISSN: 2395 -0056 VOLUME: 04 ISSUE: 03 | MAR -2017 WWW.IRJET.NET P-ISSN: 2395-0072 © 2017, IRJET | Impact Factor value: 5.181 | ISO 9001:2008 Certified Journal | Page 387 TABLE 1: Q-Factor Modulation Distance 100 km 200 km 300 km NRZ 43.1771 13.3985 6.19741 RZ 64.9336 40.5856 28.2801 IV. CONCLUSION In this paper single span optical link with various modulation schemes namely NRZ and RZ at different transmission distance is simulated. From the obtained result, it is found that RZ modulation format shows the better performance than other formats. REFERENCES [1] G. Eason, B. Noble, and I.N. Sneddon, “On certain integrals of Lipschitz-Hankel type involving products of Bessel functions,” Phil. Trans. Roy. Soc. London, vol. A247, pp. 529-551, April 1955. (references) [2] J. Clerk Maxwell, A Treatise on Electricity and Magnetism, 3rd ed., vol. 2. Oxford: Clarendon, 1892, pp.68-73. [3] I.S. Jacobs and C.P. Bean, “Fine particles, thin films and exchange anisotropy,” in Magnetism, vol. III, G.T. Rado and H. Suhl, Eds. New York: Academic, 1963, pp. 271- 350. [4] K. Elissa, “Title of paper if known,” unpublished. [5] R. Nicole, “Title of paper with only first word capitalized,” J. Name Stand. Abbrev., in press. [6] Y. Yorozu, M. Hirano, K. Oka, and Y. Tagawa, “Electron spectroscopy studies on magneto-optical media and plastic substrate interface,” IEEE Transl. J. Magn. Japan, vol. 2, pp. 740-741, August 1987 [Digests 9th Annual Conf. Magnetics Japan, p. 301, 1982]