Nelson et al. VOL. 4, NO. 11/NOVEMBER 2012/J. OPT. COMMUN. NETW. B133
Fig. 2. (Color online) Block diagram of the 100 Gb/s WDM test
setup over the uncompensated 1000 km link. The tunable laser,
N7788B polarization controller (PC) and polarimeter were added for
the experiments of Section V. Inset: the 40-channel spectrum at the
booster output.
Fig. 3. (Color online) Measurements of pre-FEC BER versus OSNR
for the 100 Gb/s MSA transceiver as channel 20 of the 40 × 100 Gb/s
1000 km system, with +3 to +6 dBm/ch launch powers into the spans.
used in the link; hence, the MSA transceiver compensated
for approximately 17,000 ps/nm of chromatic dispersion. After
each span, a two-stage erbium-doped fiber amplifier (EDFA)
was used to amplify the optical signal power. To optimize the
gain tilt, variable optical attenuators were introduced at the
mid-stages of EDFAs 1, 2, 4, 5, 7, 8, and 9, while 50 GHz
grid wavelength blockers at the mid-stages of EDFAs 3 and 6
allowed per-channel equalization. The total launch power into
each span could be varied from +19 to +21 dBm, while still
maintaining a flat channel spectrum to within ±1.5 dB at the
input to each span. Following the tenth fiber span, the test
channel was noise loaded, and its OSNR was measured with an
optical spectrum analyzer (OSA). Finally, a second commercial
50 GHz WSS was used to de-multiplex the test channel before
it was sent to the receiver input of the 100G transceiver.
Figure 3 presents BER curves after 1000 km WDM trans-
mission for launch powers of +3, +4, +5 and +6 dBm/channel
into the fiber spans. (To reach +6 dBm/ch, 20 channels in the
center of the band were transmitted.) At +3 dBm/ch, the OSNR
Fig. 4. (Color online) Comparison of the measured pre-FEC BER
versus OSNR curves from Fig. 3 with the curves measured when the
three channels on both sides of channel 20 were turned off.
penalty relative to back-to-back is 1.0 dB for a BER of 1.9×10
−2
(the SD-FEC threshold). Moreover, the received OSNR after
1000 km is 22.8 dB, indicating that sufficient margin remains
for transmission distances of 2000 km. As shown in Fig. 3, the
OSNR penalty increases to 3 dB for +6 dBm/ch; however, at
that launch power, the BER floor is still well below the FEC
threshold. To test the impact of the neighboring 100G channels,
BER curves were also measured at the different launch powers
when the six nearest neighbors (i.e., ch 17–19 and 21–23)
were turned off. To maintain the same per-channel power and
EDFA loading, three additional channels were turned on at
the short and long wavelength ends of the spectrum. Figure 4
shows a comparison of the BER curves for the channel under
test with neighboring 50-GHz-spaced, 100G channels and with
nearest neighbors spaced 200 GHz from the channel under test
(i.e., with ch 17–19 and 21–23 turned off). At +3 dBm/ch, the
required OSNR difference is only 0.3 dB, while the difference
is 1.5 dB for +6 dBm/ch. Note that, given the SSMF dispersion
and the uncompensated link, we believe the 2 Gbaud lower
symbol rate of the loading channels compared with that of
the channel under test will have only a minor impact on
the measured WDM penalties. In fact, the 28 Gbaud loading
channels walk through the channel under test at a slightly
slower rate than 30 Gbaud loading channels would, and thus
the measured WDM penalties may be slightly higher than the
actual WDM penalties would be with loading channels at the
same 30 Gbaud symbol rate as the channel under test.
As mentioned previously, the SD-FEC has been designed to
convert a pre-FEC BER of 1.9 × 10
−2
to less than 1 × 10
−15
after SD-FEC decoding, corresponding to more than 11 dB net
coding gain. In the experiments, the measured FEC threshold
is in good agreement with prediction. Figure 5 presents the
recorded post-FEC errors after SD-FEC decoding as a function
of measured pre-FEC BER for the different launch powers,
including the points from the curves of Fig. 3. Comparing the
curve for back-to-back with those after transmission verifies
that the FEC threshold—and thereby the coding gain—is
essentially maintained in the presence of fiber nonlinearities.
The FEC threshold was measured to change by <0.15 dBQ
at power levels up to +6 dBm per channel, the maximum
launch power attainable in this setup. To test repeatability,
BER curves for 3 dBm/ch and 5 dBm/ch were measured twice,
with slightly different received OSNRs.