Multiwavelength generation using an add-drop microring
resonator integrated with an InGaAsP/InP sampled
grating distributed feedback
S. E. Alavi
1
, I. S. Amiri
2,
*, M. R. K. Soltanian
2
, R. Penny
2
, A. S. M. Supa’at
1
,
and H. Ahmad
2
1
Faculty of Electrical Engineering, Universiti Teknologi Malaysia, 81310 UTM Johor Bahru, Malaysia
2
Photonics Research Centre, University of Malaya, 50603 Kuala Lumpur, Malaysia
*Corresponding author: isafiz@yahoo.com
Received September 30, 2015; accepted December 11, 2015; posted online February 5, 2016
A system of an add-drop microring resonator integrated with a sampled grating distributed feedback
(SG-DFB) is investigated via modeling and simulation with the time-domain traveling wave (TDTW)
method. The proposed microring resonator comprises a SiO
2
waveguide integrated with an InGaAsP/InP
SG-DFB, and the SiO
2
waveguide consists of a silicon core having a refractive index of 3.48 and Kerr co-
efficient of 4.5 × 10
−18
m
2
∕W. The SG-DFB consists of a series of grating bursts that are constructed using a
periodic apodization function with a burst spacing in the grating of 45 μm, a burst length of 5 μm, and 10
bursts across the total length of the SG-DBR. Transmission results of the through and drop port of the
microring resonator show the significant capacity enhancement of the generated center wavelengths. The
Q-factor of the microring resonator system, defined as the center wavelength (λ
0
) divided by 3 dB FWHM,
without and with integration with the SG-DFB is calculated as 1.93 × 10
5
and 2.87 × 10
5
, respectively.
Analysis of the dispersion of the system reveals that increasing the wavelength results in a decrease of
the dispersion. The higher capacity and efficiency are the advantages of integrating the microring resonator
and the InGaAsP/InP SG-DFB.
OCIS codes: 130.3130, 130.3990, 130.7408, 050.2770.
doi: 10.3788/COL201614.021301.
Researchers have been actively investigating wavelength-
selective reflective elements based on microring resonators
(MRs)
[1]
in recent years, with experimental demonstrations
of resonance splitting and enhanced notch depth in MRs
due to mutual mode coupling. The free spectral range is
usually large for small-radius rings, and this limits the
number of channels that can be adopted for operation
[2]
.
Split resonances provide more wavelengths for signal
processing and thus increase the system capacity. Integra-
tion of inline reflectors into planar optical circuits is
important for several reasons
[3]
; integrated reflectors can
be much smaller than corresponding fiber devices, can
be fabricated in a variety of materials with special nonlin-
ear functionality or with specific dispersion properties, and
can be combined on a single chip with additional photonic
devices such as modulators, couplers, or sources
[4]
. How-
ever, integration of sample gratings within a planar wave-
guide optical circuit is difficult due to the high-resolution
lithography required over large areas to achieve high
reflection efficiency and low scattering loss
[5]
. This is espe-
cially the case with integrated geometries that necessitate
aperiodic gratings
[6,7]
. As an alternative to integrated sam-
ple gratings, the microring-based reflector presents several
advantages including increase d flexibility
[8]
, compactness
allowing for simpler and more controlled fabrication,
and the possibility of incorporation with additional pho-
tonic devices
[9,10]
.
Silicon photonics has become one of the most promising
photonic integration platforms over the last few years
[11–13]
,
and passive silicon waveguide structures have shown an
unprecedented reduction in footprint of the waveguides,
and especially for wavelength-selective devices
[14,15]
. Exper-
imentally, the integration technology is the planar fabrica-
tion process, which has been well studied and finds a host of
applications in both telecommunications and sensing
[13]
.
Ring resonators play an important role in the success of
silicon photonics since ring resonators of silicon can be con-
structed at an unprecedented small size
[16,17]
. Integrated
optic MRs have exhibited attractive filter and switching
behavior in connection with extremely small chip-areas
for single functional elements
[18]
. These ring resonators
behave as spectral filters that can be used for applications
in optical communication, particularly wavelength divi-
sion multiplexing (WDM)
[19,20]
. An integrated add-drop
MR has been proposed in this paper. This proposed reso-
nator comprised a SiO
2
waveguide integrated with a
sampled grating distributed feedback (SG-DFB) made of
an InGaAsP/InP semiconductor. The time-domain travel-
ing wave (TDTW) method was employed for modeling and
simulating the proposed MR integrated system. Silicon
photonic wires represent an ideal platform for nonlinear
behavior because silicon exhibits a variety of strong nonlin-
ear effects, such as Kerr nonlinearity
[21–24]
. Maximizing the
nonlinearity required optimization of the nonlinear param-
eter whereby the effective area of nonlinear interaction
depends on the waveguide geometry
[25]
.
The add-drop MR system illustrated in Fig.
1(a)
provided the foundation for the proposed integrated
COL 14(2), 021301(2016) CHINESE OPTICS LETTERS February 10, 2016
1671-7694/2016/021301(6) 021301-1 © 2016 Chinese Optics Letters