IEEE PHOTONICS TECHNOLOGY LETTERS, VOL. 18, NO. 20, OCTOBER 15, 2006 2081
Cascadability of Optical 3R Regeneration for
NRZ Format Investigated in Recirculating Loop
Transmission Over Field Fibers
Masaki Funabashi, Zuqing Zhu, Zhong Pan, Bo Xiang, Loukas Paraschis, David L. Harris, and
S. J. B. Yoo, Senior Member, IEEE
Abstract—This letter demonstrates optical 3R regeneration in
10-Gb/s nonreturn-to-zero field transmission. The 3R regenerator
utilizes semiconductor-optical-amplifier-based Mach–Zehnder
interferometer wavelength converters, a synchronous modulator,
and a Fabry–Pérot filter to realize optical 3R regeneration including
all-optical clock recovery. The cascadablity of the 3R regenerator
is investigated in recirculating loop transmission experiments with
various regeneration spacings up to 462 km (corresponding to
an input optical signal-to-noise ratio (OSNR) of 22 dB). Trans-
mission with the 3R regenerator shows significant performance
improvement over that without 3R regeneration. A 66-km-spaced
3R regeneration with a 33-dB input OSNR achieves 1000-hop
cascaded error-free transmission (66 000 km in distance) with no
hop-to-hop power penalties. A 264-km-spaced 3R regeneration
with a 25-dB input OSNR also achieves 100-hop cascaded trans-
mission (26 400 km in distance) with a bit-error-rate error floor at
.
Index Terms—All-optical clock recovery, Fabry–Pérot filter
(FPF), field fiber, nonreturn-to-zero (NRZ), optical regeneration.
I. INTRODUCTION
O
PTICAL signals after fiber transmission undergo various
distortions due to the impairments caused by noise, at-
tenuation, and fiber dispersion and nonlinearity. Optical signal
regeneration is a promising technology for advanced optical
networking in overcoming these impairments by restoring the
signal quality [1]. While numerous publications reported on
optical 3R regeneration in well-controlled laboratory environ-
ments [2]–[5], only a few have demonstrated a field trial of
optical 2R [6] or 3R regeneration [7]. Moreover, the majority
of previous studies on 3R regeneration techniques employ a
return-to-zero (RZ) format [2]–[5], [7], and only a few have
discussed 3R regeneration for the most commonly used non-
return-to-zero (NRZ) format [8], [9]. The main advantage of
optical regeneration is to enhance transmission distance by cas-
cading regenerators, and recirculating loop setups are typically
Manuscript received May 9, 2006; revised July 25, 2006. This work was sup-
ported in part by Furukawa Electric, Cisco System URP Program, and in part
by the National Science Foundation under NSF 0335301 and NSF 9986665.
M. Funabashi is with the Department of Electrical and Computer En-
gineering, University of California, Davis, CA 95616 USA, and also with
Furukawa Electric Co., Ltd., Yokohama 220-0073, Japan.
Z. Zhu, Z. Pan, B. Xiang, and S. J. B. Yoo are with the Department of Elec-
trical and Computer Engineering, University of California, Davis, CA 95616
USA (e-mail: yoo@ece.ucdavis.edu).
L. Paraschis is with Advanced Technology, Core Routing, Cisco Systems,
San Jose, CA 95134 USA.
D. L. Harris is with Advanced Technology Labs, Next Gen Transport, Sprint,
Burlingame, CA 94010 USA.
Color versions of Figs. 1–4 are available online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/LPT.2006.883222
Fig. 1. (a) Experimental setup. (b) Field fiber map. (c) Eye diagrams at the
locations (A)–(E) when km and the lap number is Lap2.
used to investigate the cascadability [2]–[5]. Reference [5]
also investigated the regeneration spacing dependence of the
cascadability for the RZ format in a laboratory environment.
This letter demonstrates 3R regeneration for a 10-Gb/s NRZ
signal in a recirculating loop transmission over field fiber
links. The utilization of semiconductor-optical-amplifier-based
Mach–Zehnder interferometer (SOA-MZI) wavelength con-
verters, a Fabry–Pérot filter (FPF), and a synchronous modulator
realizes 3R regeneration, as well as all-optical clock recovery
from the NRZ signal [10]–[12]. The cascadability of the 3R
regenerator is investigated with various regeneration spacings
and optical signal-to-noise ratios (OSNRs).
II. EXPERIMENTAL SETUP
Fig. 1(a) and (b) shows the experimental setup and the field
fiber map. The recirculating loop transmission setup enables
cascadability evaluation of an inline 3R regenerator. As a trans-
mission line, up to seven sets of field fibers were used. The
field fibers are standard single-mode fibers in a loop-back con-
figuration between Burlingame and Palo Alto. Each field fiber
span has a round-trip length of 66 km, followed by a two-stage
erbium-doped fiber amplifier with a dispersion-compensating
fiber (DCF) in its middle stage. The 3R regenerator was located
after a predetermined number ( ) of the fiber spans (
or ; corresponding to a regeneration spacing ( ) of 66, 264,
or 462 km). After the first, fourth, and seventh span, residual
dispersion values were within 30 ps/nm, and OSNR degraded
to 33, 25, and 22 dB, respectively, from the initial value of 45 dB
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