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Integrating suspended tapered photonic waveguides with thermal alkali vapour

Benyamin Shnirman

Published Jan 1, 2026• 0 citations
Publisher

Abstract

In this work, we demonstrate - for the first time, to the best of our knowledge - electromagnetically induced transparency (EIT) on a fully integrated, chip-scale platform based on nanoscale tapered suspended waveguides surrounded by hot rubidium vapour. We further show that these waveguides enable the excitation of rubidium atoms to Rydberg states, and implement an electric readout scheme to detect these atoms by their ionisation currents. The fabrication workflow for standard ridge waveguides made of silicon nitride (Si3N4) is optimised, leading to significantly improved optical quality. Building on this, different techniques for locally suspending photonic structures out of Si3N4 are developed, allowing us to retain the waveguide interconnects between the structures on a conventional SiO2 layer for full chip integration. The use of a sacrificial silicon layer proves to be advantageous for suspending resonator structures, as this method does not change the optical properties of the device, as opposed to other established suspension methods. With these fabrication techniques, high quality suspended tapered waveguides are realised. Spectroscopy measurements on the D2 transition of rubidium confirm that the Doppler and transit time broadening are significantly reduced compared to standard ridge waveguides, owing to the extended evanescent field of the tapered geometry. After this, EIT is demonstrated on the tapered waveguides using a three level ladder scheme, benefiting from the longer atomic interaction times enabled by the extended evanescent field. The experimental results are compared to numerical simulations, showing good agreement. Finally, the excitation to Rydberg levels in the evanescent field of the tapered waveguide is investigated. An electrically contacted vapour cell is designed to detect the current from excited Rydberg atoms, ionised through collisions with ground-state atoms or perturber gases in the cell. Clear Rydberg signals are observed and compared with simulations modelling excitation and ionisation in the confined geometry of the evanescent field. The results indicate that the excitation can indeed occur within the guided mode and that the corresponding ionisation currents are of the same order of magnitude as those measured experimentally. However, strong scattering of the guided light is also observed at the transitions to the underetched regions, suggesting that a fraction of the Rydberg excitation may originate from this scattered light rather than from the evanescent field alone. Further investigations are ongoing at the time of writing to quantify this contribution.

DOI
10.18419/opus-18253

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In this work, we demonstrate - for the first time, to the best of our knowledge - electromagnetically induced transparency (EIT) on a fully integrated, chip-scale platform based on nanoscale tapered suspended waveguides surrounded by hot rubidium vapour. We further show that these waveguides enable the excitation of rubidium atoms to Rydberg states, and implement an electric readout scheme to detect these atoms by their ionisation currents. The fabrication workflow for standard ridge waveguides made of silicon nitride (Si3N4) is optimised, leading to significantly improved optical quality. Building on this, different techniques for locally suspending photonic structures out of Si3N4 are developed, allowing us to retain the waveguide interconnects between the structures on a conventional SiO2 layer for full chip integration. The use of a sacrificial silicon layer proves to be advantageous for suspending resonator structures, as this method does not change the optical properties of the device, as opposed to other established suspension methods. With these fabrication techniques, high quality suspended tapered waveguides are realised. Spectroscopy measurements on the D2 transition of rubidium confirm that the Doppler and transit time broadening are significantly reduced compared to standard ridge waveguides, owing to the extended evanescent field of the tapered geometry. After this, EIT is demonstrated on the tapered waveguides using a three level ladder scheme, benefiting from the longer atomic interaction times enabled by the extended evanescent field. The experimental results are compared to numerical simulations, showing good agreement. Finally, the excitation to Rydberg levels in the evanescent field of the tapered waveguide is investigated. An electrically contacted vapour cell is designed to detect the current from excited Rydberg atoms, ionised through collisions with ground-state atoms or perturber gases in the cell. Clear Rydberg signals are observed and compared with simulations modelling excitation and ionisation in the confined geometry of the evanescent field. The results indicate that the excitation can indeed occur within the guided mode and that the corresponding ionisation currents are of the same order of magnitude as those measured experimentally. However, strong scattering of the guided light is also observed at the transitions to the underetched regions, suggesting that a fraction of the Rydberg excitation may originate from this scattered light rather than from the evanescent field alone. Further investigations are ongoing at the time of writing to quantify this contribution.
Electromagnetically induced transparency (EIT) enables an otherwise opaque medium to become transparent and can dramatically slow or even temporarily store light pulses within the medium. It provides a robust platform for manipulating and preserving quantum optical signals, making it a powerful tool for quantum information processing and precision sensing. In this work, we demonstrate EIT on a fully integrated, chip-scale platform based on nanoscale atomic suspended waveguides (NASWAGs) surrounded by hot rubidium vapor. These structures provide submillimeter-scale interaction lengths and feature a tapered geometry that extends the optical mode into the surrounding vapor, increasing the atom-light interaction volume and reducing transit-time broadening. Combined with the strong spatial confinement of both probe and control beams, this enables efficient EIT with only a few microwatts of control power. This represents a significant advance over standard nanophotonic platforms, where weak evanescent fields and short interaction times have previously prevented the observation of EIT.
Alkali vapours, such as rubidium, are being used extensively in several important fields of research such as slow and stored light nonlinear optics quantum computation, atomic clocks and magnetometers. Recently, there is a growing effort towards miniaturizing traditional centimetre-size vapour cells. Owing to the significant reduction in device dimensions, light–matter interactions are greatly enhanced, enabling new functionalities due to the low power threshold needed for nonlinear interactions. Here, taking advantage of the mature platform of silicon photonics, we construct an efficient and flexible platform for tailored light–vapour interactions on a chip. Specifically, we demonstrate light–matter interactions in an atomic cladding waveguide, consisting of a silicon nitride nano-waveguide core with a rubidium vapour cladding. We observe the efficient interaction of the electromagnetic guided mode with the rubidium cladding and show that due to the high confinement of the optical mode, the rubidium absorption saturates at powers in the nanowatt regime. Alkali vapours are increasingly useful in photonic research and metrology applications, and they provide a useful test bed for investigating light–matter interaction. Stern et al. integrate silicon nitride waveguides with alkali vapours to study light–matter interactions on a chip-scale platform.
We investigate an integrated optical chip immersed in atomic vapor providing several waveguide geometries for spectroscopy applications. The narrow-band transmission through a silicon nitride waveguide and interferometer is altered when the guided light is coupled to a vapor of rubidium atoms via the evanescent tail of the waveguide mode. We use grating couplers to couple between the waveguide mode and the radiating wave, which allow for addressing arbitrary coupling positions on the chip surface. The evanescent atom-light interaction can be numerically simulated and shows excellent agreement with our experimental data. This work demonstrates a next step towards miniaturization and integration of alkali atom spectroscopy and provides a platform for further fundamental studies of complex waveguide structures.
We investigate an integrated optical chip immersed in atomic vapor providing several waveguide geometries for spectroscopy applications. The narrow-band transmission through a silicon nitride waveguide and interferometer is altered when the guided light is coupled to a vapor of rubidium atoms via the evanescent tail of the waveguide mode. We use grating couplers to couple between the waveguide mode and the radiating wave, which allow for addressing arbitrary coupling positions on the chip surface. The evanescent atom-light interaction can be numerically simulated and shows excellent agreement with our experimental data. This work demonstrates a next step towards miniaturization and integration of alkali atom spectroscopy and provides a platform for further fundamental studies of complex waveguide structures.
Deterministic quantum state control at ambient temperature remains a central challenge for scalable photonic quantum technologies. Thermal rubidium vapor cells offer a cryogenic-free platform for light-matter interaction, but Doppler broadening, collision-induced dephasing, and transit-time effects limit coherent state transfer. We present a CMOS-compatible photonic architecture for studying room-temperature Rydberg electromagnetically induced transparency (EIT) in rubidium vapor, combining integrated on-chip pulse generation, counter-propagating beam geometry, and Stark-Chirped Rapid Adiabatic Passage (SCRAP). The platform integrates an on-chip silicon nitride pulse-generation stage, dual-wavelength optical addressing at 780 nm and 480 nm, a heated rubidium vapor microcell near 140°C, and a quasiperiodic Fibonacci control layer. We model the atomic response with a three-level ladder Hamiltonian and confirm numerically that the EIT transparency window scales as Ωc²/Γe, consistent with analytic theory. Thermal averaging over the Maxwell-Boltzmann velocity distribution confirms that counter-propagating excitation reduces residual Doppler-induced absorption relative to a co-propagating geometry. Fibonacci-modulated control fields are shown to possess substantially broader spectral content than periodic modulation, supporting their use as a candidate noise-avoidance strategy; this is presented as a spectral-shaping hypothesis, not as established topological protection. Numerical scans of SCRAP-assisted Rydberg transfer under realistic Rabi frequencies do not yet show a clear efficiency advantage over resonant excitation, and this is reported as an open problem for parameter optimization. We do not claim a demonstrated two-qubit logic gate; multi-atom blockade dynamics and gate fidelity benchmarking are identified explicitly as future work.
Accurate and stable frequency sources can be realized by locking lasers to well-known transitions between energy levels in isolated quantum systems such as alkali atoms. Unfortunately, current implementations of such frequency standards typically involve bulky optical setups and discrete optical components. Furthermore, the common transitions of alkali atoms are in the near-infrared, hindering their use as frequency references in the telecom regime. Our current work is focused on mitigating these deficiencies. In particular, we demonstrate the design, fabrication, and experimental characterization of an on-chip telecom frequency reference that is based on a ladder transition of rubidium atoms integrated with nanoscale optical waveguides. These atomic cladded waveguides are implemented in a serpentine geometry in order to optimize the chip area and maximize the interaction of light with the alkali atoms. Following its fabrication, the device is used to stabilize a telecom laser around a 1.5 μm wavelength to a precision better than 200 kHz at ∼250 s. Moreover, in spite of the fact that the natural lifetime of the excited state of the atom corresponding to only a few megahertz line widths, the nanoscale confinement of the optical mode dictates ultrashort interaction times and extreme photonic energy densities allowing us to demonstrate low power and faster (∼200 MHz) all-optical modulation of a near-infrared light with a telecom light. The results presented in this paper push forward the efforts toward fully integrated chip-scale stabilization system and provide an extremely efficient link between atomic based devices and silicon photonics platform in the telecom.