optimization of four wave mixing effect in radio-over-fiber for a 32-channel 40-gbps dwdm system
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Optimization of Four Wave Mixing Effect in
Radio-over-Fiber for a 32-Channel 40-GBPS DWDM
SystemBijayananda Patnaik and P.K.Sahu
Indian Institute of Technology Bhubaneswar
E-mail: [email protected], [email protected]
Abstract- In this paper, we have discussed in detail the four
wave mixing (FWM) effect of dense wavelength division
multiplexing (DWDM) in Radio-over-Fiber (RoF) system.
A 32-channel 40-Gbps system is considered. FWM effect
for various channel spacing, input power level, effective
fiber area and modulation formats are analyzed. Different
schemes for minimizing these effects are discussed for the
first time. Considering all these effects, an optimized
DWDM setup is designed using single parameter
optimization (SPO) technique.
Index Terms - Dense wave length division multiplexing,
four wave mixing, Optisystem 8.0, Q-value, radio over
fiber, single parameter optimization.
I. INTRODUCTION
Radio-over-fiber (RoF) technology entails the use of
optical fiber links to distribute radio frequency (RF) signals
from a central location to the remote antenna units (RAUs).
RoF systems with high data rates are used for wireless
broadband communications as they can utilize the low loss and
ultra wide bandwidth provided by optical fiber. The main
benefits of RoF is low attenuation loss, large bandwidth,
immunity to radio frequency interference, reduced power
consumption, multi-operator and multi-service operation,
dynamic resource allocation etc [1], [7]. Hence it is much more
preferable comparing to RF signal processing. The explosion
in demand for network bandwidth is largely due to the growth
in traffic such as video on demand, internet usages, and voice
over IP, streaming video and voice, etc. For utilizing the higher
band width of optical systems, multiplexed systems are
preferred for transmitting huge information on to a single fiber.
A multiplexed system with channel spacing of less than or
equal to 200GHz is called as Dense Wavelength Division
Multiplexing (DWDM). Similarly if the system uses two or
more signals multiplexed onto a single fiber, where one signal
is in the 1550 nm band, and the other in the 1310 nm band, it is
said to be Coarse Wavelength Division Multiplexing
system(CWDM). In CWDM systems, due to wide spacing
between channels, it doesnt supports erbium-doped fiber
amplifier (EDFA), which is the main disadvantage of CWDM
system. FWM is a phenomenon that occurs in DWDM/CWDM
systems, in which the channel spacing are very close to each
other. It is generated by the third order distortion that creates
third order harmonics [9], [2], [3]. These cross products
interfere with the original wavelength and cause the mixing.
These spurious signals may fall right on the original
wavelength which causes difficulty in filtering out them. This
effect is mainly due to narrow channel spacing, high input
power, small cross-sectional area of fiber and fiber dispersion
[5], [6], [8]. Hence, analysis of these effects and system
optimization is highly essential for DWDM/CWDM setup. Its
performance improvement is a challenging task in present
context to meet the demand.
II. THEORY
In DWDM system, for three continuous-wave channels of
input powers Pi, Pj, Pk at frequencies fi, fj, fk, the FWM power
Pijkat the outpXWRIDILEHUZLWKDWWHQXDWLRQDQGOHQJWK]LV>@]
ijkkjieff222
ijkijk ePPPLdP
(1)
Where dijkis the degeneracy factor, which takes value 1 and
2 for degenerate (i = j) and non-degenerate (i j) terms
respectively, Leffis the effective length, ijkis the efficiency is
the nonlinear coefficient, which is given by [4]
22
eff
22
1.
A
)n(2 (2)
Where n2 is the fiber nonlinearity coefficient, Aeff is the core
effective cross-sectional area, is the central wavelength. In
general, the number of cross mixing products M, for N input
channels are given by [9]
1)(N2
NM
2
(3)
Thus as the number of input channels increases FWM effect
is more prominent and it is to be taken care for increasing the
efficiency of DWDM system.
III. SIMULATION
The proposed system consists of a transmitter, fiber and an
optical receiver as shown in Fig. 1. Transmitter consists of 32
number of DWDM channels, optical multiplexer. It supports
different modulation formats e.g., no modulation, non-return to
zero (NRZ) and return to zero (RZ) modulation etc. Standard
single mode fiber (SSMF) is used to achieve long distance
communication in this setup. The simulation parameters used
is given in Table I.
The transmission link is designed suitably, so that the first-
order dispersion is compensated exactly (D =0), that is [10],
DCFDCFSMFSMF LDLD (4)
2010 International Symposium on Electronic System Design
978-0-7695-4294-2/10 $26.00 2010 IEEE
DOI 10.1109/ISED.2010.31
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D stands for first-order dispersion and L stands for length of
the respective fiber. Fiber parameters used in the system model
is as given in Table II, which is practically available and
suitable. The EDFA is used for compensating the linear loss
and the noise figure of which is set to 6dB. The model is
simulated using symmetrical dispersion compensation
technique. Thereafter, the SPO approach is used to design the
optimal system.
In the receiver the signal is passed through an optical
demultiplexer, detected by PIN detector, filtered, applied to
power meter and BER analyzer. The responsivity and dark
current of PIN diode taken is 1A/W & 10nA respectively and a
4th
order filter is used. 3R regenerator is used to generate an
electrical signal connected directly to the BER analyzer which
is used to visualize the graphs and results such as eye diagram,
eye opening, BER, Q value of the setup. For analyzing the
FWM effect, we have used the WDM analyzer, spectrum
analyzer at the input and output of the standard single mode
fiber(SSMF).
Fig. 1 Schematic of the DWDM setup using symmetric compensation
technique
Table I: Simulation parameters
Bit rate 40Gbps
Sequence length 64
Samples/bit 256
DWDM channel spacing 200GHz
Capacity 32-channel 40-Gbps
Distance 120 Km
Input Power 5dBm
Table II: Fiber Parameters
Fiber Atten.
(dB/Km)
Disp.
(ps/km-
nm)
Disp. Slope
(ps/km-nm2)
Effective
core
area(m2)
SMF 0.2 17 0.075 70
DCF 0.5 -85 -0.3 22
IV. RESULTS AND DISCUSSION
A. FWM effect for varying channel spacing
For analyzing this effect in the proposed setup (Fig. 1), the
following parameters are considered: input power level of
0dBm; no modulation format; laser line-width of 0Hz and
P2 as the effective cross-sectional area of fiber. The input
and output spectrum of SSMF is observed by varying the
channel spacing. Fig. 2 and 3 shows the input and output
spectrum of the setup respectively, for channel spacing of
25GHz. From these Figures, we observed the effect of FWM
that is the spectrum is broadened and many side bands arenoticed. Fig. 4 shows the output spectrum of SSMF for
200GHz channel spacing. In a similar fashion the output
spectrum can be observed for 100GHz spacing. Table III
summarizes the effect of FWM for various channel spacing.
Comparing the Fig. 3, 4 (maximum side lobe power) and from
table 3, it can be concluded that the FWM effect increases, as
the channel spacing decreases. However it is not possible to
increase the channel spacing too much, because in the fiber
link faithful amplification can't be achieved for wideband
signal. Again for DWDM system maximum channel spacing
should be 200GHz.
Fig. 2 Input spectrum of SSMF of 50Km length (25GHz spacing)
31
32
31
1
WDM &
SPECTRUM
ANALYZER
2
WDM &
SPECTRUM
ANALYZER
SMF
50K
DCF
20K
SMF
50Km
EDFA
10dB
EDFA
10dB
EDFA
10dB
.
.
.
.
.
.
.
.
.
.
.
.
1
2
32
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Fig. 3 Output spectrum of SSMF of 50Km length (25GHz spacing)
Fig. 4 Output spectrum of SSMF of 50Km length (200GHz spacing)
Table III: Maximum FWM power with respect to Channel spacing
Channel Spacing
(GHz)
25 100 200
Approximate Max.
FWM side band
power (dBm)
-36 -38 -39
B. FWM effect for varying Input power
For this analysis of the setup of Fig. 1 the input and output
spectrum of SSMF is observed by varying the input power
levels, keeping other parameters as constant: the channel
spacing is 200GHz; no modulation format is used; the laser
line-width taken is 0Hz and effective cross- sectional area of
ILEHU LV FRQVLGHUHG DV P2. Fig. 5 and Fig. 6 show the
output spectrum for input power level of 20 dBm and -10
dBm respectively. Fig. 4 shows the output spectrum for input
power level of 0 dBm and spacing of 200GHz. Table IV
summarizes the maximum sideband power of FWM, forvarying input power. Comparing Fig.4, 5, and 6 and from
Table IV, it can be concluded that the FWM effect decreases
as the input signal power decreases. However, the input
power level can't be reduced below a certain limit, as it may
not be sufficient to drive the components.
Fig. 5 Output spectrum of SSMF of 50Km length (20 dBm input Power)
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Fig. 6 Output spectrum of SSMF of 50Km length (-10 dBm Input Power)
Table IV: Maximum FWM side band power value w.r.t Input power
Input power
(dBm)
-10 0 10 20
Approximate Max.
FWM side band
power (dBm)
-59 -41 -20 -12
C. FWM effect for various Modulation formats.
For this analysis modulation formats considered are RZ
and NRZ. All other parameters are considered as constant: the
input power level is 0dBm; channel spacing is 200GHz; fiber
effective cross-sectional area is P2 and laser line-width is
0Hz. From WDM analyzer shown in Fig 7 and 9, we found that
OSNR is 29.83 for NRZ but 33.77 for RZ of channel no 1.
Again from Fig. 8 and 10 we have observed that, RZ
modulation has less FWM effect comparing to NRZ
modulation. Hence RZ is preferable in case of high data rate
and long-haul communication system for minimizing the
FWM effect.
Fig. 7 WDM analyzer output for NRZ modulation (After transmission through
SSMF of 50Km length)
Fig. 8 Output spectrum for NRZ modulation (After transmission through
SSMF of 50Km length)
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Fig. 9 WDM analyzer output for RZ modulation (After transmission through
SSMF of 50Km length)
Fig. 10 Output spectrum for RZ modulation (After transmission through SSMF
of 50Km length)
D. FWM effect for varying fiber effective cross-sectional
area
For this analysis, the fiber effective cross-sectional area is
varied, by considering all other parameters as constant: input
power is 0dBm; channel spacing is 200GHz; laser line-width is
0Hz; no modulation format is used. Effective cross-sectional
area of fiber is considered as 64P2
and then 80 P2. Table V
summarizes the approximate maximum FWM side band
power. It can be concluded that FWM effect decreases as the
effective area of the fiber increases.
Table V: Maximum FWM side band value with respect to effective cross-sectional area of fiber
Effective cross-sectional
area (mt2)
64 80
Approximate maximum
FWM side band power
(dBm)
-39 -41
At the end a complete DWDM system is designed and
simulated as shown in Fig. 1 by considering, a) without
minimizing and b) with minimizing the FWM effect. The
worse case performance is always observed at channel no 1
(end Channel) for the DWDM system. Hence channel no 1
output is considered for analysis. Fig. 11 shows the eye
diagram of channel no 1, when the FWM minimization
technique is not considered. The eye is completely a distorted
one. Then considering all these minimizing effects of FWM
such as modulation technique of RZ; channel spacing of
200GHz; input power of 5dBm; fiber effective cross-sectionalarea of 70 mt2 the set up is again designed. Symmetrical
dispersion compensation scheme and single parameter
optimization technique is utilized for simulating the link length
of 120Km. Fig. 12 and 13 shows the eye diagram and Q-value
of the system for Channel no1 before and after optimization. It
is observed that the maximum Q-value is improved from 19.33
to 36.24 after optimization. Fig. 13 also shows the 3-
dimentional BER plot of the optimized link. Hence the system
performance is found to be improved by taking care of FWM
effect.
Fig. 11 Eye diagram and Q-value of the link without optimization
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Fig. 12 Eye diagram and Q-value of the link after optimization
Fig. 13 Three-dimensional BER plot of the link after optimization
V. CONCLUSION
In our work, an optimized 32-channel 40-GBPS DWDM
system is designed, by considering all the effects of four wave
mixing. The Q-value obtained for channel no. 1 of the
proposed system at a distance of 120Km is 36.24. From our
observations we found that the detrimental FWM effect can be
minimized for higher data rate and long-haul communicationsystem by maintaining the following conditions: a) the channel
spacing should be as high as possible; b) input power should be
as low as possible; c) the fiber cross-sectional area should be as
high as possible; d) preferably RZ modulation is to be used
comparing to NRZ modulation. The above system may be
further analyzed and optimized for long distance
communication, for more number of input channels and also
for advanced modulation formats.
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Johannisson, Reduction of intrachannel four-wave mixing using thealternate-phase RZ modulation format, IEEE Photonics Technol. Lett.14 (9, 14) ,pp. 1285, 2002.
[3] K.S. Cheng and J. Conradi, Reduction of pulse-to-pulse interactionusing alternative RZ Formats in 40-Gb/s systems, IEEE PhotonicsTechnol. Lett. 14 (1), pp. 98, 2002.
[4] Antonella Bogoni and Luca Poti, Effective channel allocation to reduce
inband FWM crosstalk in DWDM transmission systems, IEEE Journalof selected topics in Quantum Electronics, Vol. 10, No. 2,April 2004.
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