2026 IEEE PHOTONICS TECHNOLOGY LETTERS, VOL. 17, NO. 10, OCTOBER 2005
Uncooled DBR Laser Directly Modulated
at 3.125 Gb/s as Athermal Transmitter
for Low-Cost WDM Systems
Yiran Liu, Student Member, IEEE, Andrew R. Davies, Jonathan D. Ingham, Member, IEEE,
Richard V. Penty, Member, IEEE, and Ian H. White, Fellow, IEEE
Abstract—An uncooled three-section tunable distributed Bragg
reflector laser is demonstrated as an athermal transmitter for
low-cost uncooled wavelength-division-multiplexing (WDM) sys-
tems with tight channel spacing. A 0.02-nm thermal wavelength
drift is achieved under continuous-wave operation up to 70 C.
Dynamic sidemode suppression ratio of greater than 35 dB is
consistently obtained under 3.125-Gb/s direct modulation over
a 20 C–70 C temperature range, with wavelength variation of
as low as 0.2 nm. This indicates that more than an order of
magnitude reduction in coarse WDM channel spacing is possible
using this source.
Index Terms—Direct intensity modulation, optical fiber com-
munications, semiconductor lasers, tunable lasers, wavelength-
division-multiplexing (WDM) applications.
I. INTRODUCTION
D
UE TO the current economic drive for low-cost compo-
nents and solutions, coarse wavelength-division-multi-
plexing (CWDM) technology is attracting increasing interest.
The technology has major benefits as it employs uncooled
laser transmitters, which have smaller footprints and lower
power consumption. However, due to the thermal drift of such
lasers being typically 0.1 nm/ C, CWDM usually specifies a
20-nm channel spacing to tolerate wavelength variation over
an operating temperature range of least 70 C. Such channel
spacing limits the number of channels available for a fiber link,
and also prevents it from taking advantage of erbium-doped
fiber amplification (EDFA). Therefore, athermal operation
of wavelength-division-multiplexing (WDM) lasers, where
the thermal drift of wavelength is suppressed, is of much
interest, as it allows reduced channel spacing. Clearly any such
source should operate under modulation. Although CWDM
technology typically employs a 2.5-Gb/s channel data rate, the
recent 10-Gb/s Ethernet 10 GBASE-LX4 [1] demands use of
uncooled lasers on multiple wavelengths, with a higher data
rate of 3.125 Gb/s for each wavelength channel. This presents
a further challenge for athermal laser operation.
We have previously reported athermal operation of a four-
section sampled-grating distributed Bragg reflector (DBR) laser
[2], with continuous-wave (CW) performance limited by tem-
perature range and coarse wavelength control. We later reported
Manuscript received April 26, 2005; revised June 22, 2005.
The authors are with the Photonic Systems Group, Engineering Department,
Cambridge University, Cambridge CB2 1PZ, U.K. (e-mail: yl250@cam.ac.uk).
Digital Object Identifier 10.1109/LPT.2005.856367
Fig. 1. Demonstration of athermal operation principle.
athermal performance based on a three-section DBR laser [3] by
controlling the grating section bias only. In this letter, we report
enhanced CW performance and, for the first time, dynamic
operation of an uncooled DBR laser. Direct modulation at a
data rate of 3.125 Gb/s is demonstrated with dynamic sidemode
suppression ratio (DSMSR) consistently higher than 35 dB, over
an extended temperature range of 10 C–70 C. Enhanced CW
wavelength accuracy is achieved, with thermal drift of as low
as 0.02 nm over 10 C–70 C temperature span. Furthermore,
wavelength variation of 0.2 nm is demonstrated over the
20 C–70 C temperature range under direct modulation.
II. PRINCIPLE OF OPERATION
Fig. 1 illustrates experimentally the principle and basis of
athermal operation. The emission wavelength of the DBR laser
is recorded as the grating section bias current is swept from 0 to
75 mA. This is repeated over the temperature span from 10 C
to 70 C, in 10 C steps, to demonstrate the thermal drift of the
wavelength. As the dotted horizontal line in Fig. 1 indicates, it is
then possible to restrict the wavelength to a fixed value by con-
trolling the current into the grating section as the temperature
increases.
The device used in this letter is a three-section DBR laser,
with the grating, phase, and gain sections being 600, 100, and
600 m long, respectively. The front facet has a 4% reflective
coating and the rear facet is antireflection coated. An open-loop
current tuning scheme is adopted while the laser emission is col-
lected using a fiber lens and monitored by an optical spectrum
analyzer (OSA). The peak wavelength and DSMSR are col-
lected simultaneously. The operating temperature is monitored
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