DPSK Modulation Using a Microring Modulator
Kishore Padmaraju
1
, Noam Ophir
1
, Sasikanth Manipatruni
2
, Carl B. Poitras
2
,
Michal Lipson
2
, Keren Bergman
1
1: Department of Electrical Engineering, Columbia University, 500 West 120
th
Street, New York, New York 10027, USA
2: School of Electrical and Computer Engineering, Cornell University, 428 Phillips Hall, Ithaca, New York 14853, USA
kpadmara@ee.columbia.edu
Abstract: We present the first experimental demonstration of DPSK modulation using a
microring modulator. A 250-Mb/s electro-optic silicon microring modulator is shown with a
measured 2-dB power penalty in comparison to a commercial LiNbO
3
phase modulator.
©2011 Optical Society of America
OCIS codes: (060.5060) Phase modulation; (200.4650) Optical Interconnects; (130.4110) Modulators
As multi-core processors (MCPs) continue to scale in size and complexity, the emerging interconnect-bandwidth
bottleneck will have to be resolved by technology that transcends traditional electronic interconnects. The lower
power dissipation and improved scalability of photonic links over electronic links at high data rates is motivating the
development of photonic networks-on-chip (NoCs) for MCPs. Through a combination of individual nanophotonic
components, such as waveguides, switches, detectors, and modulators, a photonic NoC enables inter-core
communication at data rates currently unfeasible with electronic NoCs. In the realm of nanophotonic modulators,
microring modulators are an ideal candidate for photonic NoCs because of their small size and low power
consumption.
Electro-optic microring modulators have demonstrated on-off-keyed (OOK) modulation in a variety of material
platforms [1-3]. Phase modulation is an attractive alternative to OOK modulation as it offers superior receiver
sensitivity (with balanced detection), lower susceptibility to nonlinear effects, and potentially improved spectral
efficiency [4]. In this work, we report the first experimental implementation of differential-phase-shift-keyed
(DPSK) modulation using a microring modulator.
Figure 1: (a,b) DPSK modulation is produced by positioning the laser wavelength at (), at which it experiences a
constant amplitude between resonance transitions and a π phase shift. (c) Microscope image of microring with metal
contacts and indicated doping. (d)Transmission spectrum and (e) phase response of the device.
Current iterations of microring modulators induce optical modulation through a change in the optical length of
the microring. The subsequent change in the resonance condition is used to produce the amplitude modulation found
in OOK (Fig. 1a). In an electro-optic silicon microring the modulation mechanism is a p-i-n junction formed by
appropriately doping the inner and outer regions of the microring (Fig. 1c). Application of an electrical signal allows
the injection of carriers into the ring, affecting the refractive index through free-plasma dispersion, and reducing the
optical length of the microring. In addition to the blue shift of the resonance, there is also a significant blue shift in
the phase response of the microring (Fig. 1b). For over-coupled microrings, the shift in the phase response can be
used to produce the π phase shift needed for differential-phase-shift-keyed (DPSK) modulation [5].
The device used in this work, fabricated at the Cornell Nanofabrication Facility, was designed for quasi-TE
operation using a waveguide height of 250 nm and width of 450 nm. A surrounding Si slab of 50 nm was used for
the doping. A coupling gap of 200 nm over-coupled the 18-µm-radius microring with the waveguide. The Q-factor
of the microring is ~13000. Application of a DC current to the device confirmed the blue shift of both the
transmission spectrum (Fig. 1d) and phase response (Fig. 1e) of the microring modulator. The phase response was
measured using a modulation phase-shift method [6].
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OSA/ CLEO 2011
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