2568 IEEE PHOTONICS TECHNOLOGY LETTERS, VOL. 16, NO. 11, NOVEMBER 2004
Automatic Tunable Chromatic Dispersion
Compensation at 40 Gb/s in ASK and DPSK, NRZ,
and CSRZ 263-km Transmission Experiments
D. Sandel, S. Bhandare, A. F. Abas, B. Milivojevic, R. Noé, Martin Guy, and Martin Lapointe
Abstract—Chromatic dispersion (CD) in single-mode optical
fiber distorts pulses and is a big obstacle for the installation of
long-haul dynamically routed transmission systems, especially
at 40 Gb/s. Here the automatic residual CD compensation of a
263-km fiber link in the range 300 to 700 ps/nm is demon-
strated for nonreturn-to-zero amplitude-shift keying (NRZ-ASK),
carrier-suppressed return-to-zero (CSRZ)-ASK, NRZ differential
phase-shift keying (DPSK), and CSRZ-DPSK modulation formats
at 40 Gb/s. A thermally tunable dispersion compensator minimizes
residual CD, which is measured by a synchronous arrival time
detection scheme. The measured transmission penalty with online
CD compensation is between 1.2 dB for various link lengths and
compensated CD values.
Index Terms—Arrival time detection, chromatic dispersion
(CD), optical fiber transmission, tunable dispersion compensator.
I. INTRODUCTION
T
UNABLE chromatic dispersion (CD) compensation is
needed in long-haul and dynamically routed transmission
links, especially at 40 Gb/s. Various integrated optical disper-
sion compensators [1]–[5] have been demonstrated but fiber
Bragg gratings (FBGs) exhibit the largest dispersion and lowest
insertion loss with an associated tunability. Recent advances
in FBG technology now allow the realization of single and
multichannel tunable devices [6]. Among many CD detection
schemes, synchronous arrival time detection with a sensitivity
limit of 100 attoseconds [7] is the most promising option
because the scheme has an extremely low incremental cost,
provides the sign of CD, responds in 1 ms and is usable for
various modulation formats [8]. Prior to this, a similar method
was reported by Takushima and Kikuchi [9], but arrival time
detection was asynchronous. As a consequence, the required
frequency deviation was larger, the measurement interval was
longer, and the sign of dispersion remained ambiguous.
The tolerance to residual CD with respect to in-line CD
compensation ratio for various modulation formats including
nonreturn-to-zero amplitude-shift keying (NRZ-ASK), carrier-
suppressed return-to-zero (CSRZ)-ASK, NRZ differential
phase-shift keying (DPSK), and CSRZ-DPSK was evaluated
Manuscript received May 25, 2004; revised June 23, 2004.
D. Sandel, S. Bhandare, A. F. Abas, B. Milivojevic, and R. Noé are with
Department of Optical Communication and High Frequency Engineering, Uni-
versity of Paderborn, 33098 Paderborn, Germany (e-mail: suhas@ont.upb.de;
noe@upb.de).
M. Guy and M. Lapointe are with TeraXion, Sainte-Foy, QC G1P 4N3,
Canada (e-mail: mguy@teraxion.com).
Digital Object Identifier 10.1109/LPT.2004.834889
Fig. 1. Chromatic dispersion compensation (CDC) setup for 40-Gb/s ASK and
DPSK transmission experiments.
numerically in [10] at 43 Gb/s. To our knowledge, we report
for the first time an automatic CD compensation for all these
modulation formats. We conduct 40-Gb/s transmission exper-
iments, with a commercially available FBG-based thermally
tunable dispersion compensator and synchronous arrival time
detection.
II. TRANSMISSION SETUP
A small pump current modulation of a distributed-feedback
(DFB) laser will not only modulate the optical power but also
the optical frequency. At low frequencies, there can be a consid-
erable phase lag between pump current and frequency modula-
tion because the latter depends not only on the carrier density
but likewise on the chip temperature which is modulated by the
pump current with an intrinsic delay. In the presence of CD with
a dispersion coefficient and a fiber length , a frequency ex-
cursion causes an arrival time delay .
It can be neglected in comparison with the eye closure as long
as . In the following, this will be the case. It allows
the small-signal modulation frequency to be chosen so high that
it is outside the phase-locked loop bandwidth of the clock re-
covery in the receiver.
Fig. 1 shows the transmission setup. A DFB laser at 192.5 THz
(1557.366 nm) is modulated with a 5-MHz sinusoidal source
to provide 1.8% [root mean square (rms)] power modulation
and 336-MHz (rms) frequency modulation. The 40-Gb/s
pseudorandom binary sequence data obtained from a 16 : 1
1041-1135/04$20.00 © 2004 IEEE
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