Abstract:We demonstrate the high-speed electrical delay tuning of slow light pulses using Si photonic crystal waveguides. The device has an i-region-chirped pin diode, within which thermo-optic and carrier plasma effects are generated by forward bias. The former changes the delay up to 62 ps for the DC bias. The latter changes the delay for 1 Gbps pseudo random bit sequence tuning signals, which will be applicable to advanced time-domain optical signal processing.
“…The working principle of a tunable delay line is simple: a PhC waveguide supports both fast (n g of approximately 5) and slow light regions. An external tuning mechanism, such as thermal tuning [32,34], electrical tuning [34] or ultrafast, adiabatic frequency tuning [33] can then be used to select which of these regions a signal pulse will experience and therefore the time taken to travel through the device.…”
Photonic crystal(PhC) waveguides are used for a wide range of applications with diverse performance metrics. A waveguide optimised for one application may not be suitable for others and no one-size-fits-all solution exists. Therefore each application requires a specialised waveguide design, a computationally and time intensive process. Here, we present a hybrid, multi-objective optimisation routine for PhC waveguides, to efficiently guide the device design. The algorithm can be configured to optimise for a wide range of performance metrics and applications. We demonstrate optimisations for three different applications: slow light performance, propagation loss due to fabrication disorder and delay line applications. For each optimisation target, our routine quickly finds practical waveguide designs (<48 h, on a laptop computer) that match or exceed the performance of state-of-the-art devices designed by the community over the last 10 years. This is also the first time that scattering loss from fabrication disorder has been incorporated into an optimisation algorithm, ensuring realistic predictions of a PhC waveguide design's practical performance.
“…The working principle of a tunable delay line is simple: a PhC waveguide supports both fast (n g of approximately 5) and slow light regions. An external tuning mechanism, such as thermal tuning [32,34], electrical tuning [34] or ultrafast, adiabatic frequency tuning [33] can then be used to select which of these regions a signal pulse will experience and therefore the time taken to travel through the device.…”
Photonic crystal(PhC) waveguides are used for a wide range of applications with diverse performance metrics. A waveguide optimised for one application may not be suitable for others and no one-size-fits-all solution exists. Therefore each application requires a specialised waveguide design, a computationally and time intensive process. Here, we present a hybrid, multi-objective optimisation routine for PhC waveguides, to efficiently guide the device design. The algorithm can be configured to optimise for a wide range of performance metrics and applications. We demonstrate optimisations for three different applications: slow light performance, propagation loss due to fabrication disorder and delay line applications. For each optimisation target, our routine quickly finds practical waveguide designs (<48 h, on a laptop computer) that match or exceed the performance of state-of-the-art devices designed by the community over the last 10 years. This is also the first time that scattering loss from fabrication disorder has been incorporated into an optimisation algorithm, ensuring realistic predictions of a PhC waveguide design's practical performance.
“…Control and tuning delays of slow light photonic crystal Si waveguides are discussed in Refs. [20,21]. Active spectral filtering by Si Bragg grating, nano-beam resonator and p-i-n junctions are demonstrated in Refs.…”
Changes in refractive index and the corresponding changes in the characteristics of an optical waveguide in enabling propagation of light are the basis for many modern silicon photonic devices. Optical properties of these active nanoscale waveguides are sensitive to the little changes in geometry, external injection/biasing, and doping profiles, and can be crucial in design and manufacturing processes. This paper brings the active silicon waveguide for complete characterization of various distinctive guiding parameters, including perturbation in real and imaginary refractive index, mode loss, group velocity dispersion, and bending loss, which can be instrumental in developing optimal design specifications for various application-centric active silicon waveguides.
“…Si photonics is a fascinating platform that enables not only large-scale photonic integration on a silicon-on-insulator (SOI) wafer with high uniformity and reproducibility but also low-cost mass production via a CMOS-compatible process. We have studied an Si PCW fabricated by such a process and its slow-light generation, demonstrating tunable delays [13,14] and a TPA-PD [15] at telecom wavelengths. In this study, we propose and demonstrate an on-chip optical correlator in which the two basic components are integrated monolithically.…”
Section: Introductionmentioning
confidence: 99%
“…A heater was integrated into the reference branch for phase tuning, where the change of the delay by the heating was negligible. In a delay scanner based on a lattice-shifted photonic crystal waveguide (LSPCW) [13][14][15][16], the delay is scanned by integrated heaters integrated beside the LSPCW. This delay scanner is followed by a LSPCW dispersion controller operated by other heaters.…”
We propose and demonstrate an on-chip optical correlator, in which two types of photonic crystal slow-light waveguides are integrated and operated as an optical delay scanner and a two-photon-absorption photodetector. The footprint of the device, which was fabricated using a CMOS-compatible process, was 1.0 × 0.3 mm(2), which is substantially smaller than that of conventional optical correlators with free-space optics. We observed optical pulses using this device and confirmed the correspondence of pulse waveforms with those observed using a commercial correlator when the pulse width was 5-7 ps. This device will achieve one-chipping of an optical correlator and related measurement instruments.
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