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Journal of Networks - Academy Publisher

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160 JOURNAL OF NETWORKS, VOL. 5, NO. 2, FEBRUARY 2010<br />

ps/nm pre-compensation, or if the improvement <strong>of</strong> one<br />

method is very high.<br />

a) b)<br />

c)<br />

Figure 3. Q gain [dB] with respect to the conventional receiver vs.<br />

residual dispersion [ps/nm] for the combined method MEAN + MSPE<br />

with different pre-compensations and a) 4 dBm, b) 6 dBm and c)<br />

8 dBm average fibre input power.<br />

C. Summary<br />

The performance <strong>of</strong> three strategies for compensation<br />

<strong>of</strong> phase noise effects: the compensation <strong>of</strong> the mean<br />

nonlinear phase shift, the multi-symbol phase estimation<br />

and the combination <strong>of</strong> both methods for 43 Gbit/s RZ-<br />

DQPSK multi-span transmission was obtained by Monte-<br />

Carlo simulations for various dispersion maps and<br />

different fibre input powers. In general, all three methods<br />

exhibit the same optimum dispersion map with respect to<br />

the residual dispersion as is given for the conventional<br />

receiver. Thus, it is not required to change the dispersion<br />

map if receivers are upgraded with one <strong>of</strong> these phase<br />

noise compensation methods. Furthermore, it was shown<br />

that the MEAN is most efficient for systems with high<br />

performance loss due to the influence <strong>of</strong> nonlinearities<br />

and therefore also for non-optimised dispersion maps<br />

(0.9 dB Q gain for 6 dBm input power and 2.3 dB for<br />

8 dBm with 38 ps/nm residual dispersion). The<br />

improvement <strong>of</strong> this method for systems with low<br />

influence <strong>of</strong> nonlinearities however is very poor (0.35 dB<br />

Q gain for 4 dBm with 38 ps/nm residual dispersion).<br />

The Q gain <strong>of</strong> MSPE is almost independent <strong>of</strong> the<br />

dispersion map that is used. The maximum Q gain<br />

decreases with increasing fibre input power (1.4 dB Q<br />

gain for 4 dBm input power, 0.9 dB for 6 dBm and<br />

0.7 dB for 8 dBm with 38 ps/nm residual dispersion).<br />

The improvement <strong>of</strong> the combination <strong>of</strong> MEAN and<br />

MSPE is approximately equal to the sum <strong>of</strong> the<br />

improvement from each individual method (1.8 dB Q<br />

gain for 4 dBm input power, 1.9 dB for 6 dBm and<br />

2.7 dB for 8 dBm with 38 ps/nm residual dispersion).<br />

Therefore, depending on the system setup, it has to be<br />

decided if the additional gain <strong>of</strong> implementing both<br />

methods, MEAN and MSPE, is reasonable.<br />

© 2010 ACADEMY PUBLISHER<br />

III. ELECTRONIC EQUALIZERS IN COHERENT<br />

PSK-RECEIVERS<br />

In a second part we investigate electronic equalization<br />

in coherent receivers in combination with multi-level<br />

modulation and nonlinear fiber effects. The next bitrate in<br />

the Ethernet hierarchy is expected to be 100Gb/s. For this<br />

bitrate, multi-level modulation formats should be used to<br />

reduce the bandwidth requirements. In conjunction with a<br />

coherent receiver the multi-level formats can be detected<br />

in the electrical domain with digital signal processing<br />

(DSP), due to the availability <strong>of</strong> high-speed digital signal<br />

processors. Similarly carrier and phase recovery as well<br />

as the equalization can be achieved with DSP [5].<br />

A. Simulation Setup<br />

At the transmitter side either 53.5GBaud RZ-QPSK<br />

[6], 35.7GBaud RZ-8PSK [7] or 26.75GBaud Star-RZ-<br />

16QAM are generated to achieve 107Gb/s for all<br />

modulation formats according to Fig. 4 (top). Star-RZ-<br />

16QAM is generated from RZ-8PSK with an additional<br />

Mach-Zehnder modulator (MZM). The advantage <strong>of</strong> this<br />

setup is the necessity <strong>of</strong> only binary driving signals,<br />

contrary to multi-level driving signals in the case <strong>of</strong> pure<br />

I/Q-modulation. All data signals are differentially<br />

encoded due to the phase ambiguity <strong>of</strong> the carrier<br />

recovery.<br />

The transmission channel is modelled as a single span<br />

with variable length to adjust the chromatic dispersion<br />

(CD). A linear channel (only CD, D=17ps/nm/km) as<br />

well as a nonlinear channel (self-phase-modulation<br />

(SPM) and CD, γ=1.6215 1/W/km, α=0.21dB/km,<br />

Pfiber in, average=5dBm) is assumed.<br />

At the receiver side an EDFA with a Gaussian optical<br />

bandpass filter (BP, f3dB= 4.1x Baudrate) is used for noise<br />

loading. The received signal is combined with the signal<br />

<strong>of</strong> a local oscillator (LO) in a 2x4 90º hybrid (for this<br />

contribution ideal homodyne detection is assumed) and<br />

detected with two balanced photo-detectors. Afterwards<br />

the resulting electrical inphase and quadrature signals are<br />

lowpass (LP) filtered (Butterworth 3 rd order, f3dB= 1x<br />

Baudrate), sampled twice per symbol and then processed<br />

in a digital signal processing unit (fig. 5).<br />

CW<br />

laser<br />

SSMF<br />

RZ pulse train<br />

MZM<br />

clock<br />

Var.<br />

att.<br />

3 dB<br />

coupler<br />

EDFA<br />

BP<br />

LO<br />

data 1<br />

MZM<br />

MZM 90º<br />

data 2<br />

90º<br />

Hybrid<br />

3 dB<br />

coupler<br />

RZ-QPSK<br />

Inphase component<br />

LP<br />

LP<br />

data 3<br />

PM<br />

Quadrature component<br />

data 4<br />

MZM<br />

RZ-8PSK Star-<br />

RZ-16QAM<br />

ADC<br />

X r<br />

X i<br />

EDC<br />

&<br />

phase<br />

estimation<br />

DSP<br />

data' 1<br />

data' 2<br />

data' 3<br />

data' 4<br />

Figure 4. Transceiver (top), channel and receiver (bottom) setup; PM:<br />

Phase Modulator.<br />

For EDC, linear transversal filters for all investigated<br />

equalizers are used. The performance <strong>of</strong> equalizers with<br />

only a feed forward filter (FFE[x], where x denotes the

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