482 IEEE JOURNAL OF SELECTED TOPICS IN QUANTUM ELECTRONICS, VOL. 15, NO. 3, MAY/JUNE 2009
Discretely Tunable Semiconductor Lasers Suitable
for Photonic Integration
Diarmuid C. Byrne, Jan Peter Engelstaedter, Wei-Hua Guo, Qiao Yin Lu, Brian Corbett, Brendan Roycroft,
James O’Callaghan, F. H. Peters, and John F. Donegan, Senior Member, IEEE
Abstract—A sequence of partially reflective slots etched into an
active ridge waveguide of a 1.5 μm laser structure is found to
provide sufficient reflection for lasing. Mirrors based on these re-
flectors have strong spectral dependence. Two such active mirrors
together with an active central section are combined in a Vernier
configuration to demonstrate a tunable laser exhibiting 11 dis-
crete modes over a 30 nm tuning range with mode spacing around
400 GHz and side-mode suppression ratio larger than 30 dB. The
individual modes can be continuously tuned by up to 1.1 nm by
carrier injection and by over 2 nm using thermal effects. These
mirrors are suitable as a platform for integration of other optical
functions with the laser. This is demonstrated by monolithically
integrating a semiconductor optical amplifier with the laser result-
ing in a maximum channel power of 14.2 dBm from the discrete
modes.
Index Terms—Photonic integration, semiconductor lasers, semi-
conductor optical amplifiers, tunable lasers.
I. INTRODUCTION
W
IDELY tunable semiconductor lasers will play an impor-
tant part in next generation optical networks. Tunable
lasers are essential in wavelength-agile networks and as a means
to reduce costs as sparing lasers in wavelength-division multi-
plexing (WDM) systems. New approaches to data transmission
such as coherent WDM (CoWDM [1]) require discrete tuning
between particular wavelength channels on a grid. There is ad-
ditionally an urgent need to integrate semiconductor lasers with
other optical components such as amplifiers, modulators and
detectors [2]–[5] in order to reduce chip cost, system size, and
complexity. Tunable lasers are also needed in other important
markets such as trace gas detection for environmental emission
motoring [6].
Laser operation requires optical feedback, which is conven-
tionally obtained in a semiconductor Fabry–P´ erot laser by cleav-
ing the ends of the laser waveguide along either (0 1 1) or (0 1
−1) crystallographic planes to form two semireflecting facets.
However, due to the need for cleavage, it is difficult to integrate
these lasers with other optical components on a single chip.
Manuscript received October 30, 2008; revised February 3, 2009. First pub-
lished May 15, 2009; current version published June 5, 2009.
D. C. Byrne, W.-H. Guo, Q. Y. Lu, and J. F. Donegan are with the Semicon-
ductor Photonics Group, School of Physics and Centre for Telecommunication
Value Driven Research (CTVR), Trinity College, Dublin 2, Ireland (e-mail:
byrnedc@tcd.ie).
J. P. Engelstaedter, B. Corbett, B. Roycroft, and J. O’Callaghan are with the
Tyndall National Institute and Centre for Telecommunication Value Driven Re-
search (CTVR), Cork, Ireland.
F. H. Peters is with the Physics Department, University College Cork, Cork,
Ireland.
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/JSTQE.2009.2016981
Distributed-Bragg-reflector (DBR) lasers and distributed
feedback (DFB) lasers, which employ a series of small refrac-
tive index perturbations to provide feedback, do not rely on
cleaved facets, and therefore, can be integrated with optical am-
plifiers and modulators [4], [5]. However, complex processing
with multiple epitaxial growth stages is required for fabricating
these lasers. Another method to obtain feedback is to etch a
facet. However, this approach is limited by difficulties in the
smoothness and verticality of the etched facet, particularly, for
structures based on InP materials.
Previously, it was shown that by introducing a shallow slot
into the active ridge waveguide of a laser, the longitudinal modes
of the Fabry–Perot (FP) cavity were perturbed according to the
position of the slot with respect to the cleaved facets [7]–[9].
By judicious placement of a sequence of low-loss slots with
respect to the facets, preselected FP modes could be signifi-
cantly enhanced leading to robust single-frequency lasing with
wide temperature stability [10], [11] as well as tuning with fast
switching characteristics [12]. More recently, we have character-
ized the properties of slots that are etched more deeply, namely,
to the depth of, but not through, the core waveguide containing
the quantum wells [13]. In that case, the reflection of each slot
is of the order of ∼1% with transmission of ∼80% and the slot
will strongly perturb the mode spectrum of the FP cavity by
creating subcavities. The loss introduced by the presence of the
slot is compensated by gain in the laser. An array of such slots
can provide the necessary reflectivity for the laser operation in-
dependent of a cleaved facet where the gain between the slots
compensates for the slot loss producing an active slotted mir-
ror region. Such a mirror has been used in conjunction with a
cleaved facet permitting the integration of a photodetector with
the laser [14].
In this paper, we use reflective slots and the associated mir-
rors as the platform technology for the realization of a facetless
laser that can be tuned using differential current injection into
different longitudinal sections. Furthermore, the integration of
the tunable laser with an optical amplifier is also demonstrated.
The electrical isolation between the different sections is made
possible by the etched slots. The slots are realized by conven-
tional photolithography and dry etching during the definition of
the waveguide. As the technology is based on a generic single
epitaxial growth stage and upon standard laser processing steps,
it is compatible with implementation in a foundry.
II. TUNABLE LASER DESIGN
The semiconductor laser employing etched slots as the front
and back mirrors is shown schematically in Fig. 1(a). The laser
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