3392 JOURNAL OF LIGHTWAVE TECHNOLOGY, VOL. 21, NO. 12, DECEMBER 2003
Rigorous Beam Propagation Analysis of Tapered
Spot-Size Converters in Deep-Etched
Semiconductor Waveguides
B. M. A. Rahman, Senior Member, IEEE, W. Boonthittanont, S. S. A. Obayya, T. Wongcharoen, E.O. Ladele,
and K. T. V. Grattan
Abstract—A rigorous study of a tapered spot-size converter in a
deep-etched GaAs/AlGaAs optical modulator is reported through
the use of full vectorial approaches. Mode beating in the tapered
section, the expansion of the spot-size, and the consequent enhance-
ment of the coupling to an optical fiber are also reported.
Index Terms—Beam propagation method, finite-element
method, optical coupling, spot-size converters.
I. INTRODUCTION
I
N the design of semiconductor optical waveguides, power
splitters, bends, lasers, modulators, and amplifiers, two dif-
ferent manufacturing technologies creating different design ap-
proaches are often used. The first type, the shallow rib type de-
signs [1], [2], are more widely used; however, the performance
of the devices often critically depends on the etch depth, and
in this approach, the resulting optical mode shape is also diffi-
cult to control. On the other hand, by deep-etching through and
beyond the core to part of the lower cladding [3], the modal be-
havior of the structure would be less sensitive to the etch depth.
Besides, due to the strong horizontal confinement, the bending
losses would be greatly reduced [4], [5] and consequently a
more compact optoelectronic system design would be possible,
which will lead to an increased functionality of the subsystems
than would be allowed by using the shallow-etching approach.
This type of deep-etched waveguide structure has been used for
the design of multimode interference (MMI)-based power split-
ters [6], [7], delay lines, and high-speed modulators [8].
For many semiconductor devices, such as lasers, modulators,
and amplifiers, their optical spot-sizes are small in size and often
highly nonsymmetrical. If such a device is directly butt-coupled
to a single-mode fiber (SMF), which has a much larger and cir-
cular field profile, often 90% or more of the optical power would
be lost due to the mismatch between their field profiles. In the
design of a deep-etched semiconductor waveguide, effectively
single-mode operation is possible [3] for a much wider wave-
guide by controlling the lower cladding index to radiate out all
the higher order modes. In this case, the resulting spot-size is
Manuscript received May 29, 2003; revised September 3, 2003. This work
was supported by EPSRC.
B. M. A. Rahman, W. Boonthittanont, S. S. A. Obayya, E. O. Ladele, and
K. T. V. Grattan are with the School of Engineering and Mathematical Sciences,
City University London, EC1V 0HB London, U.K. (e-mail: B.M.A.Rahman@
city.ac.uk).
T. Wongcharoen is with Bangkok University, Bangkok, Thailand.
Digital Object Identifier 10.1109/JLT.2003.821753
slightly bigger and more symmetrical, but not yet comparable
with that of a SMF. As an example, in the design optimization
of high-speed GaAs modulators [8], often values of the wave-
guide core width of between 3.0 to 5.0 m with heights between
1.5 to 3.0 m are used, which may yield 30-40% coupling ef-
ficiency. However, these spot-sizes need to be improved further
to reduce significantly the coupling loss with the SMFs and to
minimize the packaging costs.
Recently, in the design of a semiconductor photonic compo-
nent or a subsystem, monolithically integrated spot-size con-
verters (SSCs) have often been incorporated to improve the cou-
pling efficiency along with the much relaxed alignment toler-
ances. In the design of such an SSC, often the primary guide is
tapered down [9]–[13] to push the mode to the secondary guide,
which is designed to have a similar spot-size to that of a SMF. In
this work, a SSC converter compatible with deep-etched semi-
conductor photonic components is investigated, by using rig-
orous vectorial approaches to study the spot-size transformation
and the resultant enhancement of the coupling efficiency.
II. NUMERICAL METHOD
The expansion of the spot-size is often achieved by reducing
the core dimension to a sufficiently small value [9]–[13] so
that the primary guide cannot support any guided mode and
consequently the optical power is pushed out of this core to a
secondary core. Often a closely spaced twin-core superstructure
may be used, with one core being axially nonuniform and the
resultant waveguide cross-section can be quite complex in
shape. To study the mode-shape and the evolution of the optical
beam, both a modal solution and a beam propagation-type
evolutionary approach would be necessary. Over the last two
decades, many numerical methods have been reported for
the eigenmode solutions of the optical waveguides. However,
many of these approaches would not be accurate for optical
waveguides operating near their modal cutoff conditions. In this
respect, the -field based full-vectorial finite-element method
(FEM) [14] has established itself as one of the most rigorous
full vectorial approaches for the characterization of a wide
range of optical waveguides [14], [15]. In the FEM approach,
the waveguide cross section is represented by a large number of
triangles, and since these triangles could be of different shapes
and sizes, any waveguide cross-section can be accurately
represented. The full vectorial -field formulation (VFEM) is
used here, which allows each of these elements to have different
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