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Photonics & Electromagnetics Research Symposium - Spring (PIERS-Spring)

Silicon-Based Racetrack Resonators: Harnessing EIT for Enhanced Near Infrared Sensing

Sarah Shafaay, Mohamed A. Swillam

Published May 4, 2025• 0 citations
Publisher

Abstract

Silicon on insulator (SOI) waveguides are the most used waveguides in photonic components and devices, primarily because of their low losses and compatibility with complementary metal oxide semiconductor (CMOS) manufacturing. This compatibility enables the use of electronic fabrication facilities to produce photonic circuits. In SOI waveguides, most of the photonic mode is contained within the silicon core, while an exponentially decaying evanescent tail extends into the surrounding cladding. Racetrack-resonators are pivotal in advancing silicon photonics, enabling the creation of compact resonators that support high-quality factors (Q-factors). A typical racetrack resonator consists of an optical waveguide that loops back on itself, creating resonance when the optical path length corresponds to an integer multiple of the wavelength. In this paper, we introduce an optical gas sensor based on electromagnetically induced transparency (EIT), a quantum interference effect arising from the interaction of two nearby resonant modes. Our design features a double racetrack with varying radii that resonate at$1.55 \mu \mathrm{m}$. By placing the smaller racetrack inside the larger one, we achieve the EIT phenomenon, resulting in the absence of resonant spectral lines at the same wavelength and the emergence of two shifted resonance lines. This sharp and narrow transmission peak enhances gas detection accuracy, making this sensor a promising tool for environmental monitoring and industrial applications, where precise measurements of gas concentrations are essential.

DOI
10.1109/piers-spring66516.2025.11276643

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Silicon on insulator (SOI) waveguides are the most used waveguides in photonic components and devices, primarily because of their low losses and compatibility with complementary metal oxide semiconductor (CMOS) manufacturing. This compatibility enables the use of electronic fabrication facilities to produce photonic circuits. In SOI waveguides, most of the photonic mode is contained within the silicon core, while an exponentially decaying evanescent tail extends into the surrounding cladding. Racetrack-resonators are pivotal in advancing silicon photonics, enabling the creation of compact resonators that support high-quality factors (Q-factors). A typical racetrack resonator consists of an optical waveguide that loops back on itself, creating resonance when the optical path length corresponds to an integer multiple of the wavelength. In this paper, we introduce an optical gas sensor based on electromagnetically induced transparency (EIT), a quantum interference effect arising from the interaction of two nearby resonant modes. Our design features a double racetrack with varying radii that resonate at1.55μm1.55 \mu \mathrm{m}1.55μm. By placing the smaller racetrack inside the larger one, we achieve the EIT phenomenon, resulting in the absence of resonant spectral lines at the same wavelength and the emergence of two shifted resonance lines. This sharp and narrow transmission peak enhances gas detection accuracy, making this sensor a promising tool for environmental monitoring and industrial applications, where precise measurements of gas concentrations are essential.
We investigate the resonance property of a self-coupled optical waveguide (SCOW) with four coupling points. Under a special condition that the two outer couplers are in weak coupling and the two inner couplers are in strong coupling, an implicit standing-wave resonance mode is formed inside the SCOW structure. As the resonance is feedback coupled via an S-shape bus waveguide, electromagnetically induced transparency (EIT)-like resonance features are observed in the output transmission spectrum. The SCOW resonator is analyzed using the coupled mode theory and finite-difference time-domain simulation. The device is experimentally demonstrated on the silicon-on-insulator platform. The measurement results overall agree well with the theoretical calculation. The EIT-like peak can be tuned by a thermo-optic phase shifter made of a NIN-type silicon resistor integrated in the feedback waveguide. The results point to new ways of creating on-chip optical analog of the EIT phenomenon that can be utilized for various optical signal processing applications.
An all-optical realization scheme of electromagnetically induced transparency (EIT) in a single silicon optomechanical microring resonator is proposed and demonstrated. Due to the strong mechanical Kerr effect and well-designed microring resonator, two modes with a resonant frequency separation of 292 GHz (2.35 nm) can be tuned into resonance when the control power is about 4.3 µW, and the EIT spectrum is achieved. Our work provides a constructive solution for realizing EIT in a single microcavity with a low mode density. Furthermore, this device is fully integrated on-chip and compatible with current complementary metal-oxide semiconductor (CMOS) processing and has great potential in applications such as light storage, optical sensing, and quantum optics.
Microring resonators (MRRs) are key building blocks in integrated photonics, but their performances usually suffer from limitations in extinction ratio and slope rate (SR), primarily due to their symmetrical Lorentzian resonance line shape. To overcome these limitations, special transmission spectra (STS), such as Fano resonance and electromagnetically induced transparency (EIT)-like resonance, offer asymmetric line shapes that exhibit a higher extinction ratio (ER) and a steeper SR, thereby enhancing the sensitivity and selectivity of optical switches, filters, and high-sensitivity sensors. However, the current reported works typically achieved only one type of STS and had limited tunability. In this Letter, we experimentally demonstrate a novel, to the best of our knowledge, device using two cascaded MRRs with different quality factors to generate Fano and EIT-like resonances at distinct ports. The ER can reach up to 31.2 dB with a sharp SR of 130.1 dB/ nm, for Fano resonance, and the EIT-like resonance is 12.4 dB. By adjusting the resonator wavelength of the MRRs and the phase shifter, the STS can be working at any desired wavelength. The device is demonstrated on a silicon-on-insulator platform, offering versatile application potential in optical sensors, slow and fast light generation, and microwave photonics.
A microring resonator consists of a ring side-coupled to a bus waveguide, where the light exchange is achieved by means of evanescent coupling mechanism.It is a strong candidate for integrated optics due to its advantage of compact size, cascadable input/output ports, and the compatibility of CMOS fabrication.The microring resonator can be used to create many interesting phenomena that are difficult to obtain in other classical configurations.This thesis focuses on the theoretical analysis and experimental realization of induced transparency in optical devices derived from ring resonators.In this thesis, I propose a ring-bus-ring Mach-Zehnder interferometer (RBRMZI) system based on a 3×3 coupler, and show that such a system can generate an electromagnetically induced transparency (EIT)-like spectrum via phase engineering facilitated by interpathways interference between RBR and MZI, instead of separate light interaction in two resonators alone.Both the transfer matrix formalism and the temporal coupled mode theory are investigated to model this induced transparency.The relationship between the two theories is obtained via the energy-conservation and Q-factors.In addition, the EIT-like spectrum in the RBRMZI is experimentally realized using silicon-oninsulator technology.The best RBRMZI device has a transparency with a bandwidth of 0.25nm, a free spectral range of 12nm and a Q-factor of ~6300.With further measurements of the devices having strong ring-bus coupling, we obtain a Q~18000 when the circumference of one ring is 43.4μm and the circumference of the other ring is slightly detuned by ~0.035%.Moreover, we achieve a roundtrip loss as small as ~0.5% of the input energy.The measurement results agree well with theoretical prediction and 2D-FDTD numerical calculations.
Photon pair sources with the capability to tune the wavelength and correlation properties of the generated photons can be useful for quantum applications such as communication, sensing, and computing. Silicon devices based on the SOI (silicon-on-insulator) platform benefits from both tight modal confinement, due to high index contrast between core and cladding, and CMOS compatible manufacturing process, making it a suitable platform for such sources. In the present work, we discuss the possibility of using planar resonant silicon devices with bend radii of a few tens of microns as photon pair sources. We discuss that a silicon nanophotonic chip consisting of either a single microring or coupled microrings can be used to generate photon pairs around 1.55 um. We discuss that the photons are generated in multiple pairs of wavelengths and can be tuned over several nanometers, demonstrating the capability to generate wavelength division multiplexed photon pairs at freely chosen telecommunication-band wavelengths. Further on, we discuss the ease of control over the bi-photon spectrum of the generated photon pairs and its implication in controlling their correlation properties. Uncorrelated photon pairs can be used to herald a single photon, and correlated photon pairs can be used in various quantum applications such as communication and sensing. In the end, we discuss the design parameters of a single microring resonator based sources.
Controlling the optical response of a medium through suitably tuned coherent electromagnetic fields is highly relevant in a number of potential applications, from all-optical modulators to optical storage devices. In particular, electromagnetically induced transparency (EIT) is an established phenomenon in which destructive quantum interference creates a transparency window over a narrow spectral range around an absorption line, which, in turn, allows to slow and ultimately stop light due to the anomalous refractive index dispersion. Here we report on the observation of a new form of both induced transparency and amplification of a weak probe beam in a strongly driven silicon photonic crystal resonator at room temperature. The effect is based on the oscillating temperature field induced in a nonlinear optical cavity, and it reproduces many of the key features of EIT while being independent of either atomic or mechanical resonances. Such thermo-optically induced transparency will allow a versatile implementation of EIT-analogs in an integrated photonic platform, at almost arbitrary wavelength of interest, room temperature and in a practical, low cost, and scalable system.