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Toward Scalable All-Silicon Superconducting-Photonic Integration on SOI

Waveren A. Van, Damiano Ricciarelli, Calogero G., D. Débarre, Géraldine Hallais, Alonso-Ramos C., Magna A. La, F. Chiodi

Published Jun 1, 2026• 0 citations
OpenAlex

Abstract

The reproducibility and scalability associated to the CMOS industry have led to a large increase in the use of siliconfor other applications as well, most notably the surge of silicon integrated photonics during the past decade.However, it is less well-known that this material cannot only host electronic and photonic circuits, but alsobecomes superconducting when hyper doped with Boron above 1 at.%.[1] We are currently working on buildingall-Si devices that combine superconductivity with integrated photonics to directly link quantum circuits to fast,low noise optical waveguides.Achieving the concentration required for superconductivity in silicon-on-insulator (SOI) used for photonic circuitsposes multiple challenges, as they can only be obtained via an out-of-equilibrium processes. Nanosecond laserdoping, that induces an ultra-fast liquid-phase epitaxy enables boron incorporation far above the solubility limit(up to 8 at.% in bulk silicon.[2]) The reduced heat dissipation through the 1-3 μm thick buried oxide (BOX)compared to bulk silicon leads to a large reduction of the recrystallization velocity from 4 m/s to 2 m/s and thus toa lower charge carrier concentration. Additionally, the higher thermal budget enhances dopant diffusion, leadingto unwanted deactivation of the boron.By combining experiments and simulations, we investigated the influence of the silicon and BOX thicknesses(notably Si/SiO2 = 220/2000, 700/3000 and 88/145 nm) on recrystallization dynamics and electrical properties. Itwas shown that the silicon thickness is the dominant factor for the melting threshold, whereas the BOX thicknessstrongly impacts the thermal budget, leading to dopant deactivation. As a result, both the total stack and thechosen laser energy determine the final recrystallization velocity. For the 700/3000 nm SOI reducing the layerthickness from 250 to 80 nm lowers the thermal budget and hence improves the layer quality, leading to a doublingof the charge carrier concentration. This enables superconductivity with a critical temperature of 0.5 K and, to ourbest knowledge, constitutes the first demonstration of superconductivity on photonics-compatible SOI.For SOI with thinner BOX layers, typical substrates for microelectronics applications such as FD-SOI MOSFET, thethermal confinement is smaller, and high dopant activation is systematically achieved. Furthermore, it has beenshown that implantation followed by nanosecond laser annealing can reach similar active concentrations as in-situdoping [3], allowing the implementation of superconducting devices on 'microelectronics' SOI with CMOScompatible techniques. These results indicate a promising potential for the industrial fabrication of hybrid circuitscombining integrated photonics and superconductive silicon.

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The reproducibility and scalability associated to the CMOS industry have led to a large increase in the use of siliconfor other applications as well, most notably the surge of silicon integrated photonics during the past decade.However, it is less well-known that this material cannot only host electronic and photonic circuits, but alsobecomes superconducting when hyper doped with Boron above 1 at.%.[1] We are currently working on buildingall-Si devices that combine superconductivity with integrated photonics to directly link quantum circuits to fast,low noise optical waveguides.Achieving the concentration required for superconductivity in silicon-on-insulator (SOI) used for photonic circuitsposes multiple challenges, as they can only be obtained via an out-of-equilibrium processes. Nanosecond laserdoping, that induces an ultra-fast liquid-phase epitaxy enables boron incorporation far above the solubility limit(up to 8 at.% in bulk silicon.[2]) The reduced heat dissipation through the 1-3 μm thick buried oxide (BOX)compared to bulk silicon leads to a large reduction of the recrystallization velocity from 4 m/s to 2 m/s and thus toa lower charge carrier concentration. Additionally, the higher thermal budget enhances dopant diffusion, leadingto unwanted deactivation of the boron.By combining experiments and simulations, we investigated the influence of the silicon and BOX thicknesses(notably Si/SiO2 = 220/2000, 700/3000 and 88/145 nm) on recrystallization dynamics and electrical properties. Itwas shown that the silicon thickness is the dominant factor for the melting threshold, whereas the BOX thicknessstrongly impacts the thermal budget, leading to dopant deactivation. As a result, both the total stack and thechosen laser energy determine the final recrystallization velocity. For the 700/3000 nm SOI reducing the layerthickness from 250 to 80 nm lowers the thermal budget and hence improves the layer quality, leading to a doublingof the charge carrier concentration. This enables superconductivity with a critical temperature of 0.5 K and, to ourbest knowledge, constitutes the first demonstration of superconductivity on photonics-compatible SOI.For SOI with thinner BOX layers, typical substrates for microelectronics applications such as FD-SOI MOSFET, thethermal confinement is smaller, and high dopant activation is systematically achieved. Furthermore, it has beenshown that implantation followed by nanosecond laser annealing can reach similar active concentrations as in-situdoping [3], allowing the implementation of superconducting devices on 'microelectronics' SOI with CMOScompatible techniques. These results indicate a promising potential for the industrial fabrication of hybrid circuitscombining integrated photonics and superconductive silicon.
The capability of realizing quantum photonics implementations on-chip will have a strong impact on several aspects of quantum computation and information processing. The implementation of large scale integrated quantum photonic technologies requires on-chip reconfigurable waveguide circuits as well as single-photon sources and detectors. Many successes have been made in recent years to demonstrate complex quantum circuits in many material platforms. Among all these platforms, the Silicon-on-Insulator (SOI) platform is outstanding as it is well developed for classical applications and therefore deploys a high component density, mature fabrication techniques and compatibility with the telecom regime and the complementary metal-oxide-semiconductor (CMOS) technology. However, the lack of on-demand non-classical light sources, directly incorporated in silicon chips, forces the use of nonlinear processes to generate non-classical light states: the probabilistic nature of the emission process sets a limit in the maximally achievable experimental complexity. The use of on-demand sources will have a strong impact on the device’s scalability.
Photon pairs and heralded single photons are a useful resource in quantum communication, computation, and measurement. Room-temperature microchip-scale integrated devices could enable scalability, robustness and low-cost deployment in practical applications. Silicon is an attractive integration platform, since pair generation by spontaneous four-wave mixing at 1.2 - 1.6 micron wavelengths requires optical power levels that can be delivered by compact electrically-driven laser diodes. However, silicon photonics lacks a native laser device, and the propagation losses are not especially low, although they are somewhat lower than III-V integrated optics, which does have an integrated laser. Nevertheless, silicon photonics can be expected to become a widely-adopted platform for photonics – both classical and quantum – because of the ability to leverage the mature fabrication processes using large-area silicon wafers inherited from the development of microelectronics. Moreover, scalable quantum optics requires electronics for control, drivers and readout circuits, which silicon microelectronic technology can supply. Our research is improving the performance of silicon photonics components for quantum optical communications, and is increasing the level of integration in the quantum silicon photonics toolkit, using microelectronic components and electrically-driven hybrid silicon lasers.
Quantum-based communication systems can potentially achieve the ultimate security from eavesdropping and greatly reduce the operating powers on chip. Light-speed transmission, noise immunity, and low noise properties make photons indispensable for quantum communication to transfer a quantum state through a transmission line. Furthermore, the field of silicon nanophotonics is fast growing field which is driven by the attractive and promising improvements it has to offer in high speed communication systems and on chip optical interconnects. Consequently, there is a high demand to develop the building blocks for photon manipulation in silicon nanophotonic circuits. The goal of the work is to enable high performance optoelectronic computing and communication systems that overcome the barriers of electronics and dramatically enhance the performance of circuits and systems. We will focus our attention on solving some of the issues with the current systems regarding photon storage, routing, isolation, switching, and energy conversion. We realize a continuously tunable optical memory which breaks the time-bandwidth limit by more than thirty times. This enabled the storage of ultra-short pulses of light for hundreds of picoseconds. Also, we investigate on-chip photon scattering when transmitted through micro-scale optical cavities. In addition, we develop novel dynamic quantum mechanical models that predict quantum-like behavior of single and multi-photon wavepackets. Furthermore, we report for the first time that efficient red shifts in silicon are achievable with free carrier injection which generally produces blue wavelength shifts. We realize adiabatic wavelength conversion and discrete photonic transitions of single photons in silicon cavities. Moreover, we demonstrate a basic quantum network on chip with an on-chip photon source. We present a novel design for CMOS compatible optical isolator on silicon chip using a system of active cavities. And finally, we analyze a novel ultra-fast broadband modulator in silicon based on free-carrier absorption effect in SOI waveguides integrated with Schottky diodes.
Integrated photonics offers great potential for quantum communication devices in terms of complexity, robustness and scalability. Silicon photonics in particular is a leading platform for quantum photonic technologies, with further benefits of miniaturisation, cost-effective device manufacture and compatibility with CMOS microelectronics. However, effective techniques for high-speed modulation of quantum states in standard silicon photonic platforms have been limited. Here we overcome this limitation and demonstrate high-speed low-error quantum key distribution modulation with silicon photonic devices combining slow thermo-optic DC biases and fast (10~GHz bandwidth) carrier-depletion modulation. The ability to scale up these integrated circuits and incorporate microelectronics opens the way to new and advanced integrated quantum communication technologies and larger adoption of quantum-secured communications.
Integrated photonics offers great potential for quantum communication devices in terms of complexity, robustness, and scalability. Silicon photonics in particular is a leading platform for quantum photonic technologies, with further benefits of miniaturization, cost-effective device manufacture, and compatibility with CMOS microelectronics. However, effective techniques for high-speed modulation of quantum states in standard silicon photonic platforms have been limited. Here we overcome this limitation and demonstrate high-speed low-error quantum key distribution modulation with silicon photonic devices combining slow thermo-optic DC biases and fast (10 GHz bandwidth) carrier-depletion modulation. The ability to scale up these integrated circuits and incorporate microelectronics opens the way to new and advanced integrated quantum communication technologies and larger adoption of quantumsecured communications.
Silicon-on-insulator (SOI) wafers have been developed for electronic integrated circuits, but are also one of the most promising platforms in photonic integrated circuits due to its low loss, high refractive index, ability to fast phase modulation, and well-developed fabrication technologies. With advantages to handle light with a small volume and high modulation speed, silicon photonics has been intensively investigated as the next generation platform of signal processing, interconnection, and communication devices. Recently, silicon photonics has been attracted great interests in quantum optics communities as optical quantum systems for linear optical quantum computing are achievable using silicon photonic components including beam splitters, phase modulators, and filters and the small footprint of a silicon photonic quantum system has unprecedented performances of high stability and scalability. Here we show our recent results on the fabrication of silicon photonic elements for quantum applications. We fabricated low-loss optical waveguides, efficient fiber-to-waveguide grating couplers, resonator-based optical filters, and tunable beam splitters and tested their performances. A micro-sized heater is attached on a Mach-Zehnder interferometer, showing stable operation as a slow phase modulator. In addition, phase modulators using plasma dispersion effects are under investigation. Finally, the quantum characteristics of photon pairs generated by spontaneous four-wave mixing in silicon waveguides are investigated. These results will be an essential cornerstone for the realization of quantum optical computing and quantum communication devices.