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IOSR Journal of Electronics and Communication Engineering (IOSR-JECE)
e-ISSN: 2278-2834,p- ISSN: 2278-8735.Volume 6, Issue 6 (Jul. - Aug. 2013), PP 19-23
www.iosrjournals.org
www.iosrjournals.org 19 | Page
Performance Analysis of Dispersion Compensation in Long Haul
Optical Fiber with DCF
Saurabh Kumar1
, Prof. A. K. Jaiswal2
, Er. Mukesh Kumar3
, Er. Rohini Saxena4
1
(M.Tech Student of ECE, SSET/ SHIATS, Allahabad, India)
2
(Prof. & Head of ECE, SSET/ SHIATS, Allahabad, India)
3,4
(Assistant Prof. of ECE, SSET/ SHIATS, Allahabad, India)
Abstract : In this paper, We investigate post, pre and symmetrical/mix dispersion compensation methods for 40
Gb/s non-return to zero link using standard and dispersion compensated fiber through FBG compensator to
optimize high data rate optical transmission. The influence of dispersion of FBG compensator and increases in
the power of CW laser has been studied to evaluate the performance of optical communication systems. The
simulation model of the WDM based on the Optisystem 11.0 is presented according to the above principle. The
simulation results are validated by analysing the Q-factor and Bit error rate (BER) in the numerical simulator.
It is found that post compensation performance is best and the input fiber power is taken as 5-10dB, the
corresponding BER performance is better.
Keywords - BER, Dispersion compensation, Q-factor, WDM.
I. Introduction
When optical signals are transmitted over optical links, different wavelength components of the optical
signals will generally experience different propagation times due to the fact that the transport medium has
different effective refractive indices for different wavelengths. In recent years, with the rapid growth internet
business needs, people urgently need more capacity and network systems. So the demand for transmission
capacity and bandwidth are becoming more and more challenging to the carriers and service suppliers. Under
the situation, with its huge bandwidth and excellent transmission performance, optical fiber is becoming the
most favourable delivering media and laying more and more important role in information industry [2,3].
Therefore, it is very necessary to investigate the transmission characteristics of optical fiber. And the
main goal of communication system is to increase the transmission distance. Loss and dispersion are the major
factor that affect fiber-optical communication being the high-capacity develops. The EDFA is the gigantic
change happened in the fiber-optical communication system; the loss is no longer the major factor to restrict the
fiber optical transmission. Since EDFA works in 1550 nm wave band, the average Single Mode Fiber (SMF)
dispersion value in that wave band is very big, about 15-20ps / (nm.km-1) . It is easy to see that the dispersion
become the major factor that restricts long distance fiber optical transfers.[4]. In this study, we propose three
DCF compensation scheme, post-compensation, pre-compensation and symmetrical/mix compensation scheme.
Simulation studies show that post compensation scheme is the best. It can greatly reduce the influences of the
fiber nonlinearity and increase the transmission distance greatly.
The rest of paper is organized as followed. In Section II, the cause of fiber dispersion and its effects on
optical transmission is introduced. In Section III, present fiber dispersion compensation technology. In Section
IV, present the research of DCF dispersion compensation scheme. Section V present transmission system
simulation with OPTISYSTEM 11.0, analyses and compare each kind of compensation scheme, Section VI
concludes the paper.
II. Fiber Optic Dispersion On Optical Transmission
Loss and dispersion are the major factor that affect fiber-optical communication being the high-
capacity develops. The EDFA is the gigantic change happened in the fiber-optical communication system; the
loss is no longer the major factor to restrict the fiber-optical transmission. Since EDFA works in 1550 nm wave
band, the average Single Mode Fiber (SMF) dispersion value in that wave band is very big, about 15-20ps / (nm.
km-1
). It is easy to see that the dispersion become the major factors that restrict long distance fiber-optical
transfers. Dispersion is defined as because of the different frequency or mode of light pulse in fiber transmits at
different rates, so that these frequency components or models receive the fiber terminals at different time. It can
cause intolerable amounts of distortions that ultimately lead to errors. In single-mode fiber performance is
primarily limited by chromatic dispersion which occurs because the index of the glass varies slightly depending
on the wavelength of the light, and light from real optical transmitters necessarily has nonzero spectral width.
Polarization mode dispersion another source of limitation occurs because although the single-mode fiber can
sustain only one transverse mode, it can carry this mode with two different polarizations, and slight
Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF
www.iosrjournals.org 20 | Page
imperfections or distortions in a fiber can alter the propagation velocities for the two polarizations. This
phenomenon is called birefringence. Mode birefringence Bm is defined as the follow
Bm =
𝛽𝑥 −𝛽𝑦
𝑘0
= nx - ny (1)
Where nx, ny are the effective refractive of the two orthogonal polarizations. For a given Bm, its fast
axis and slow axis components will be formed the phase difference after the light waves transmission L Km.
φ = k0BmL
2𝜋
𝜆
(NX-NY) = (𝛽𝑥 − 𝛽𝑦)L (2)
If the Bm is a constant, through the light waves in transmission process the phase difference between
its fast axis and slow axis will periodicity repetition. The length that it leads to a phase difference of 2π or power
periodic exchange is called polarization beat length.
LB =
2𝜋
𝛽𝑥 −𝛽𝑦
=
𝜆
𝛽𝑚
(3)
If the incident light has two polarization components, due to refractive difference between the fast axis
and slow axis, the transmit rate of two polarization components will be different. Degree of pulse broadening
can be expressed by different group delay Δτ. The influence of dispersion on system performance is also
reflected in the optical fiber nonlinear effects. Dispersion increased the pulse shape distortion caused by the self-
phase modulation dispersion (SPM); the other hand, dispersion in WDM systems can also increase the cross-
phase modulation (XPM), four-wave mixing (FWM) and other nonlinear effects [6,7].
III. Dispersion Compensation Technology
To improve overall system performance and reduced as much as possible the transmission performance
influenced by the dispersion, several dispersion compensation technologies were proposed. Amongst the various
techniques proposed in the literature, the ones that appear to hold immediate promise for dispersion
compensation and management could be broadly classified as: dispersion compensating fiber (DCF), chirped
fiber Bragg gratings (FBG), and high-order mode (HOM) fiber [8]. The idea of using dispersion compensation
fiber for dispersion compensation was proposed as early as in 1980 but, until after the invention of optical
amplifiers, DCF began to be widespread attention and study. DCF has become a most useful method of
dispersion compensation and has been extensively studied.
There is positive second-order and third-order dispersion value in SMF while the DCF dispersion value
is negative. So by inserting a DCF, the average dispersion is close to zero. As the local dispersion of higher
transmission link, FWM and XPM were ignored; only to consider the role of SPM and dispersion.
IV. Dispersion Compensation Scheme
To support a high-capacity wavelength-division-multiplexing (WDM) transmission, the embedded
standard single-mode fiber (SMF) should be up graded to overcome the dispersion limit. In this paper dispersion
compensating fiber is analyzed with dispersion compensation with the help of fiber bragg compensator.
According to relative position of DCF and single mode fiber, post-compensation, pre-compensation and
symmetrical/mix compensation is proposed. DCF Pre-compensation scheme achieve dispersion compensation
by place the DCF before a certain conventional single-mode fiber, or after the optical transmitter. Post
compensation scheme achieve dispersion compensation by place the DCF after a certain conventional single-
mode fiber, or before the optical transmitter. Symmetrical/mix compensation scheme is consist of post
compensation and pre compensation. Different location on the system will generate different nonlinear effects.
The Simulation of three dispersion compensation system is shown in Figure 1.
(a) Simulation for post compensation
Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF
www.iosrjournals.org 21 | Page
(b) Simulation for pre compensation
(c) Simulation for symmetrical compensation
Figure 1 : Three dispersion compensation scheme
Figure 1 (a) shows the post compensation schemes. The simulation module includes the transmission
module, transmission link and the receiver module. Simulation model use Mach-Zehnder external modulator to
modulate the CW Laser at central frequency 193.1 THz. Optical fiber transmission link composed of a 100Km.
The kind of optical fiber is G.655. Dispersion compensation is achieved with fiber bragg gratings (FBG) are
implemented instead of using dispersion compensated fiber (DCF). EDFA is used to compensate the power loss
generating by SMF and the DCF signal. Receiver module includes de multiplexer and receiver filters.
Figure 1 (b) and Figure l (c) respectively show the pre compensation scheme and the symmetrical/mix
compensation scheme. The simulation configuration is as similar as Figure 1 (a). The difference is that at the
transmitter DCF compensate 100 Km of single-mode fiber dispersion in Figure 1 (b). In Figure l (c), there is a
symmetrical/mix compensation scheme.
V. Result And Analysis
In optical communication only optical signal to noise ratio (OSNR) could not accurately measure the
system performance, especially in WDM systems. Quality factor is a one of the important indicators to measure
the optical performance by which to characterize the BER. Figure 2 and Figure 3 display the influence of input
optical power on the performance of transmission system.
Figure 2: Comparison among three dispersion
compensation (DCF) on the basis of Q-factor
Figure 3: Comparison among three dispersion
compensation (DCF) on the basis of BER
Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF
www.iosrjournals.org 22 | Page
Figure 2 shows the effect on Q-factor with the variation in optical power and compensator dispersion in
fiber bragg grating (FBG) of all dispersion compensation fiber (DCF) model. We can observe that with the input
power increasing steadily up to about 5 dBm brings the nominal increases in Q-factor and when input optical
power approaches to 5 dBm, the Q-factor becomes maximum. When equal power is launched into the various
models of the link, the Q-factor of post compensation scheme is greater than the two other kinds of dispersion
compensation scheme. When the input optical power is greater than 5 dBm the quality factor decreased
gradually and the error performance is gradually degraded. This is because as the optical power increases,
nonlinear effects increase, but the optical signal noise ratio increased. Through the whole system study found
that the performance of post compensation system is best in the long-distance high-speed WDM systems.
(a) At 0 dB power with compensator
dispersion -2000 ps/nm for post compensation
(b) At 0 dB power with compensator
dispersion -2000 ps/nm for pre compensation
(c) At 0 dB power with compensator
dispersion -2000 ps/nm for symmetrical
compensation
(d) At 0 dB power with compensator
dispersion 0 ps/nm for post compensation
(e) At 0 dB power with compensator
dispersion 0 ps/nm for pre compensation
(f) At 0 dB power with compensator
dispersion 0 ps/nm for symmetrical compensation
Figure 4: Eye diagram of different compensation technique at different compensator dispersion of fiber bragg
Figure 4 gives the simulation results at different dispersion compensator of fiber bragg at same
optical power. As we can see from the figure 4 (a), the effect of dispersion compensation is very good with -
2000 ps/nm dispersion compensator of fiber bragg at 0 dB power. The signal quality is high, eye’s shape is very
good and the effect of dispersion compensation is quite good. The curve of Q-factor changes with the open
degree of eye diagram as follows. More approaches the point of largest eye diagram opened, the Q-factor is
bigger, and the corresponding BER is smaller.
VI. Conclusion
On the basis of compared and analyzed the three system simulation results conclusions are as the
followings. Using fiber bragg gratings (FBG) are implemented instead of using dispersion compensated fiber
(DCF) for dispersion compensation in 40Gb/s WDM system is an effective solution. It is observed that the
compensation schemes reduced the dispersion appropriately but among them post compensation scheme
reduced the accumulated fiber chromatic dispersion to the maximum possible extent. A moderate lesser value of
fiber bragg grating dispersion and bigger value of laser average power is favorable to the performance of the
transmission system. Variation of the input power launched and compensator dispersion of fiber bragg grating
resulted in variation in Q-factor and the corresponding graph showed that at 5 dBm and -2000ps/nm the link
performance with the regard the Q-factor provides the better result.
Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF
www.iosrjournals.org 23 | Page
References
[1] Bo-ning HU, Wang Jing, Wang Wei, Rui-mei Zhao, “Analysis on Dispersion Compensation with DCF based on Optisystem”. 2nd
International Conference on Industrial and Information Systems pp. 40-43 2010.
[2] Mochida Y, Yamaguchi N, Ishikawa G, "Technology-oriented review and vision of 40Gb/s based optical transport Networks",
Journal of light-wave technology.PP. 2272-228,12002,20(12)
[3] Omae T, "Universal conditions for estimating the nonlinear refractive index n2 of dispersion com- pensating fibers by the CWSPM
method", IEEE Photon. Technol. Lett., Vol 13. No.6, pp. 571-573, Nov, 2001.
[4] Zou X Y, Hayee M I, H wang S M, et al. Limitations in 10Gb/s WDM optical-fiber transmission when using a variety of fiber types
to manage dispersion and nonlinearities[J]. Lightwave Technol., PP: 1144-1152,June,1996.
[5] BU CHAL IF, LANNES. Fast eye monitor for 10G/bs and its applicationg for optical PMD compensation [Z]. Optical Society of
America,2000.
[6] Killy R I, Thiele H J, Mikhailov v, ea al. Reduction of intrachannel nonlinear distortion in 40-Gb/s based WDM transmission over
standard fiber [J]. IEEE Photonics Technology Letters, 2000, 12(12): 1642-1626.
[7] Eggleton B 1. Dynamic dispersion, compensation devices for high speed transmission systems. Optical Fiber communication
conference and exhibit, 2001(3): WHlII-WH1I3
[8] jianjun Yu, Bojun Yang,"Dispersion-allacated soliton technology with long amplifier spacing and long distance," IEEEphoton
technol lett, vol 9, pp. 952-954,No.7, 1997.

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Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF

  • 1. IOSR Journal of Electronics and Communication Engineering (IOSR-JECE) e-ISSN: 2278-2834,p- ISSN: 2278-8735.Volume 6, Issue 6 (Jul. - Aug. 2013), PP 19-23 www.iosrjournals.org www.iosrjournals.org 19 | Page Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF Saurabh Kumar1 , Prof. A. K. Jaiswal2 , Er. Mukesh Kumar3 , Er. Rohini Saxena4 1 (M.Tech Student of ECE, SSET/ SHIATS, Allahabad, India) 2 (Prof. & Head of ECE, SSET/ SHIATS, Allahabad, India) 3,4 (Assistant Prof. of ECE, SSET/ SHIATS, Allahabad, India) Abstract : In this paper, We investigate post, pre and symmetrical/mix dispersion compensation methods for 40 Gb/s non-return to zero link using standard and dispersion compensated fiber through FBG compensator to optimize high data rate optical transmission. The influence of dispersion of FBG compensator and increases in the power of CW laser has been studied to evaluate the performance of optical communication systems. The simulation model of the WDM based on the Optisystem 11.0 is presented according to the above principle. The simulation results are validated by analysing the Q-factor and Bit error rate (BER) in the numerical simulator. It is found that post compensation performance is best and the input fiber power is taken as 5-10dB, the corresponding BER performance is better. Keywords - BER, Dispersion compensation, Q-factor, WDM. I. Introduction When optical signals are transmitted over optical links, different wavelength components of the optical signals will generally experience different propagation times due to the fact that the transport medium has different effective refractive indices for different wavelengths. In recent years, with the rapid growth internet business needs, people urgently need more capacity and network systems. So the demand for transmission capacity and bandwidth are becoming more and more challenging to the carriers and service suppliers. Under the situation, with its huge bandwidth and excellent transmission performance, optical fiber is becoming the most favourable delivering media and laying more and more important role in information industry [2,3]. Therefore, it is very necessary to investigate the transmission characteristics of optical fiber. And the main goal of communication system is to increase the transmission distance. Loss and dispersion are the major factor that affect fiber-optical communication being the high-capacity develops. The EDFA is the gigantic change happened in the fiber-optical communication system; the loss is no longer the major factor to restrict the fiber optical transmission. Since EDFA works in 1550 nm wave band, the average Single Mode Fiber (SMF) dispersion value in that wave band is very big, about 15-20ps / (nm.km-1) . It is easy to see that the dispersion become the major factor that restricts long distance fiber optical transfers.[4]. In this study, we propose three DCF compensation scheme, post-compensation, pre-compensation and symmetrical/mix compensation scheme. Simulation studies show that post compensation scheme is the best. It can greatly reduce the influences of the fiber nonlinearity and increase the transmission distance greatly. The rest of paper is organized as followed. In Section II, the cause of fiber dispersion and its effects on optical transmission is introduced. In Section III, present fiber dispersion compensation technology. In Section IV, present the research of DCF dispersion compensation scheme. Section V present transmission system simulation with OPTISYSTEM 11.0, analyses and compare each kind of compensation scheme, Section VI concludes the paper. II. Fiber Optic Dispersion On Optical Transmission Loss and dispersion are the major factor that affect fiber-optical communication being the high- capacity develops. The EDFA is the gigantic change happened in the fiber-optical communication system; the loss is no longer the major factor to restrict the fiber-optical transmission. Since EDFA works in 1550 nm wave band, the average Single Mode Fiber (SMF) dispersion value in that wave band is very big, about 15-20ps / (nm. km-1 ). It is easy to see that the dispersion become the major factors that restrict long distance fiber-optical transfers. Dispersion is defined as because of the different frequency or mode of light pulse in fiber transmits at different rates, so that these frequency components or models receive the fiber terminals at different time. It can cause intolerable amounts of distortions that ultimately lead to errors. In single-mode fiber performance is primarily limited by chromatic dispersion which occurs because the index of the glass varies slightly depending on the wavelength of the light, and light from real optical transmitters necessarily has nonzero spectral width. Polarization mode dispersion another source of limitation occurs because although the single-mode fiber can sustain only one transverse mode, it can carry this mode with two different polarizations, and slight
  • 2. Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF www.iosrjournals.org 20 | Page imperfections or distortions in a fiber can alter the propagation velocities for the two polarizations. This phenomenon is called birefringence. Mode birefringence Bm is defined as the follow Bm = 𝛽𝑥 −𝛽𝑦 𝑘0 = nx - ny (1) Where nx, ny are the effective refractive of the two orthogonal polarizations. For a given Bm, its fast axis and slow axis components will be formed the phase difference after the light waves transmission L Km. φ = k0BmL 2𝜋 𝜆 (NX-NY) = (𝛽𝑥 − 𝛽𝑦)L (2) If the Bm is a constant, through the light waves in transmission process the phase difference between its fast axis and slow axis will periodicity repetition. The length that it leads to a phase difference of 2π or power periodic exchange is called polarization beat length. LB = 2𝜋 𝛽𝑥 −𝛽𝑦 = 𝜆 𝛽𝑚 (3) If the incident light has two polarization components, due to refractive difference between the fast axis and slow axis, the transmit rate of two polarization components will be different. Degree of pulse broadening can be expressed by different group delay Δτ. The influence of dispersion on system performance is also reflected in the optical fiber nonlinear effects. Dispersion increased the pulse shape distortion caused by the self- phase modulation dispersion (SPM); the other hand, dispersion in WDM systems can also increase the cross- phase modulation (XPM), four-wave mixing (FWM) and other nonlinear effects [6,7]. III. Dispersion Compensation Technology To improve overall system performance and reduced as much as possible the transmission performance influenced by the dispersion, several dispersion compensation technologies were proposed. Amongst the various techniques proposed in the literature, the ones that appear to hold immediate promise for dispersion compensation and management could be broadly classified as: dispersion compensating fiber (DCF), chirped fiber Bragg gratings (FBG), and high-order mode (HOM) fiber [8]. The idea of using dispersion compensation fiber for dispersion compensation was proposed as early as in 1980 but, until after the invention of optical amplifiers, DCF began to be widespread attention and study. DCF has become a most useful method of dispersion compensation and has been extensively studied. There is positive second-order and third-order dispersion value in SMF while the DCF dispersion value is negative. So by inserting a DCF, the average dispersion is close to zero. As the local dispersion of higher transmission link, FWM and XPM were ignored; only to consider the role of SPM and dispersion. IV. Dispersion Compensation Scheme To support a high-capacity wavelength-division-multiplexing (WDM) transmission, the embedded standard single-mode fiber (SMF) should be up graded to overcome the dispersion limit. In this paper dispersion compensating fiber is analyzed with dispersion compensation with the help of fiber bragg compensator. According to relative position of DCF and single mode fiber, post-compensation, pre-compensation and symmetrical/mix compensation is proposed. DCF Pre-compensation scheme achieve dispersion compensation by place the DCF before a certain conventional single-mode fiber, or after the optical transmitter. Post compensation scheme achieve dispersion compensation by place the DCF after a certain conventional single- mode fiber, or before the optical transmitter. Symmetrical/mix compensation scheme is consist of post compensation and pre compensation. Different location on the system will generate different nonlinear effects. The Simulation of three dispersion compensation system is shown in Figure 1. (a) Simulation for post compensation
  • 3. Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF www.iosrjournals.org 21 | Page (b) Simulation for pre compensation (c) Simulation for symmetrical compensation Figure 1 : Three dispersion compensation scheme Figure 1 (a) shows the post compensation schemes. The simulation module includes the transmission module, transmission link and the receiver module. Simulation model use Mach-Zehnder external modulator to modulate the CW Laser at central frequency 193.1 THz. Optical fiber transmission link composed of a 100Km. The kind of optical fiber is G.655. Dispersion compensation is achieved with fiber bragg gratings (FBG) are implemented instead of using dispersion compensated fiber (DCF). EDFA is used to compensate the power loss generating by SMF and the DCF signal. Receiver module includes de multiplexer and receiver filters. Figure 1 (b) and Figure l (c) respectively show the pre compensation scheme and the symmetrical/mix compensation scheme. The simulation configuration is as similar as Figure 1 (a). The difference is that at the transmitter DCF compensate 100 Km of single-mode fiber dispersion in Figure 1 (b). In Figure l (c), there is a symmetrical/mix compensation scheme. V. Result And Analysis In optical communication only optical signal to noise ratio (OSNR) could not accurately measure the system performance, especially in WDM systems. Quality factor is a one of the important indicators to measure the optical performance by which to characterize the BER. Figure 2 and Figure 3 display the influence of input optical power on the performance of transmission system. Figure 2: Comparison among three dispersion compensation (DCF) on the basis of Q-factor Figure 3: Comparison among three dispersion compensation (DCF) on the basis of BER
  • 4. Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF www.iosrjournals.org 22 | Page Figure 2 shows the effect on Q-factor with the variation in optical power and compensator dispersion in fiber bragg grating (FBG) of all dispersion compensation fiber (DCF) model. We can observe that with the input power increasing steadily up to about 5 dBm brings the nominal increases in Q-factor and when input optical power approaches to 5 dBm, the Q-factor becomes maximum. When equal power is launched into the various models of the link, the Q-factor of post compensation scheme is greater than the two other kinds of dispersion compensation scheme. When the input optical power is greater than 5 dBm the quality factor decreased gradually and the error performance is gradually degraded. This is because as the optical power increases, nonlinear effects increase, but the optical signal noise ratio increased. Through the whole system study found that the performance of post compensation system is best in the long-distance high-speed WDM systems. (a) At 0 dB power with compensator dispersion -2000 ps/nm for post compensation (b) At 0 dB power with compensator dispersion -2000 ps/nm for pre compensation (c) At 0 dB power with compensator dispersion -2000 ps/nm for symmetrical compensation (d) At 0 dB power with compensator dispersion 0 ps/nm for post compensation (e) At 0 dB power with compensator dispersion 0 ps/nm for pre compensation (f) At 0 dB power with compensator dispersion 0 ps/nm for symmetrical compensation Figure 4: Eye diagram of different compensation technique at different compensator dispersion of fiber bragg Figure 4 gives the simulation results at different dispersion compensator of fiber bragg at same optical power. As we can see from the figure 4 (a), the effect of dispersion compensation is very good with - 2000 ps/nm dispersion compensator of fiber bragg at 0 dB power. The signal quality is high, eye’s shape is very good and the effect of dispersion compensation is quite good. The curve of Q-factor changes with the open degree of eye diagram as follows. More approaches the point of largest eye diagram opened, the Q-factor is bigger, and the corresponding BER is smaller. VI. Conclusion On the basis of compared and analyzed the three system simulation results conclusions are as the followings. Using fiber bragg gratings (FBG) are implemented instead of using dispersion compensated fiber (DCF) for dispersion compensation in 40Gb/s WDM system is an effective solution. It is observed that the compensation schemes reduced the dispersion appropriately but among them post compensation scheme reduced the accumulated fiber chromatic dispersion to the maximum possible extent. A moderate lesser value of fiber bragg grating dispersion and bigger value of laser average power is favorable to the performance of the transmission system. Variation of the input power launched and compensator dispersion of fiber bragg grating resulted in variation in Q-factor and the corresponding graph showed that at 5 dBm and -2000ps/nm the link performance with the regard the Q-factor provides the better result.
  • 5. Performance Analysis of Dispersion Compensation in Long Haul Optical Fiber with DCF www.iosrjournals.org 23 | Page References [1] Bo-ning HU, Wang Jing, Wang Wei, Rui-mei Zhao, “Analysis on Dispersion Compensation with DCF based on Optisystem”. 2nd International Conference on Industrial and Information Systems pp. 40-43 2010. [2] Mochida Y, Yamaguchi N, Ishikawa G, "Technology-oriented review and vision of 40Gb/s based optical transport Networks", Journal of light-wave technology.PP. 2272-228,12002,20(12) [3] Omae T, "Universal conditions for estimating the nonlinear refractive index n2 of dispersion com- pensating fibers by the CWSPM method", IEEE Photon. Technol. Lett., Vol 13. No.6, pp. 571-573, Nov, 2001. [4] Zou X Y, Hayee M I, H wang S M, et al. Limitations in 10Gb/s WDM optical-fiber transmission when using a variety of fiber types to manage dispersion and nonlinearities[J]. Lightwave Technol., PP: 1144-1152,June,1996. [5] BU CHAL IF, LANNES. Fast eye monitor for 10G/bs and its applicationg for optical PMD compensation [Z]. Optical Society of America,2000. [6] Killy R I, Thiele H J, Mikhailov v, ea al. Reduction of intrachannel nonlinear distortion in 40-Gb/s based WDM transmission over standard fiber [J]. IEEE Photonics Technology Letters, 2000, 12(12): 1642-1626. [7] Eggleton B 1. Dynamic dispersion, compensation devices for high speed transmission systems. Optical Fiber communication conference and exhibit, 2001(3): WHlII-WH1I3 [8] jianjun Yu, Bojun Yang,"Dispersion-allacated soliton technology with long amplifier spacing and long distance," IEEEphoton technol lett, vol 9, pp. 952-954,No.7, 1997.