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Scalable feedback stabilization of quantum light sources on a CMOS chip

Abstract

Silicon photonics could soon be used to create the vast numbers of physical qubits needed to achieve useful quantum information processing by leveraging mature complementary metal–oxide–semiconductor (CMOS) manufacturing to miniaturize optical devices for generating and manipulating quantum states of light. However, the development of practical silicon quantum-photonic integrated circuits faces challenges related to high sensitivity to process and temperature variations, free-carrier and self-heating nonlinearities, and thermal crosstalk. These issues have been partially addressed with bulky off-chip electronics, but this sacrifices many benefits of a chip-scale platform. Here we report an electronic–photonic quantum system-on-chip that consists of quantum-correlated photon-pair sources stabilized via on-chip feedback control circuits and is fabricated in a commercial 45-nm CMOS microelectronics foundry. We use non-invasive photocurrent sensing in a tunable microring cavity photon-pair source to actively lock it to a fixed-wavelength pump laser while operating in the quantum regime, enabling large-scale microring-based quantum systems. We also show that these sources maintain stable quantum properties and operate reliably in a practical setting with many adjacent photon-pair sources creating thermal disturbances on the same chip. Such dense integration of electronics and photonics enables implementation and control of quantum-photonic systems at the scale needed to achieve useful quantum information processing with CMOS-fabricated chips.

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Fig. 1: Electronic–photonic quantum system-on-chip.
Fig. 2: Classical characterization of the electronic–photonic integrated circuit block.
Fig. 3: Quantum characterization of the SFWM photon-pair source with real-time feedback control.
Fig. 4: Experimental demonstration of feedback-controlled SFWM under thermal disturbances.
Fig. 5: Simultaneous operation of many photon-pair sources on a single chip.

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Data availability

Datasets generated during the current study are available from the corresponding authors upon reasonable request.

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Acknowledgements

This work was funded by NSF EQuIP program grant no. 1842692, Packard Fellowship no. 2012-38222, NSF FuSe TG award no. 2,235,466 and the Catalyst Foundation. We thank Ayar Labs and GlobalFoundries for chip fabrication and the Berkeley Wireless Research Center for chip-testing support.

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Authors and Affiliations

Authors

Contributions

I.W. and J.M.F.C. designed the photonic components. D.K. and I.W. designed the electronic–photonic system layout. D.K., S.B., C.A. and P.Z. designed the on-chip electronic circuits. S.B. created and supported the electronic–photonic chip design infrastructure and tool flow. D.K. performed the system integration; package design, control firmware and software development; and initial hardware bring-up. D.K., A.R. and Ð.G. collected and analysed the classical electro-optical characterization data. A.R. developed and performed the quantum characterization experiments, and D.K. contributed the data analysis code. A.R. and D.K. conceptualized and conducted the system-level demonstrations. I.W., Ð.G., D.K. and A.R. developed and validated the photon-pair source device model. The paper was prepared by D.K., A.R., I.W. and Ð.G. D.K., A.R. and I.W. created the figures. All authors contributed to the review of the paper. M.A.P., P.K. and V.M.S. supervised and conceptualized the project. These authors contributed equally: D.K., I.W. and A.R.

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Correspondence to Danielius Kramnik, Imbert Wang or Anirudh Ramesh.

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Nature Electronics thanks Ali Elshaari, Ryota Katsumi and Jianwei Wang for their contribution to the peer review of this work.

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Extended data

Extended Data Fig. 1 High-Extinction Pump Rejection Filter.

(a) Measurement setup for characterizing the extinction ratio of the integrated pump rejection filters. The filters are aligned by using an EDFA in place of the tunable laser to intentionally generate broadband ASE noise, and then maximizing the drop port power meter readings using a Nelder-Mead optimization algorithm. The tunable laser is then swapped back in to take a transmission spectrum. (b) Normalized transmission spectrum of input to drop port response of the aligned filter using a series of stitched continuous sweeps with varying power meter range settings (blue curve) showing ~ 95 dB extinction that is limited by ASE noise of the laser source passing through the aligned passband. When an external ASE filter is enabled and the integration time is increased, the noise floor falls below the minimum detectable level of the power meter, indicating > 100 dB extinction at an offset wavelength of one FSR of the photon-pair source, which is required for fully on-chip pump filtering (red points). The filter uses a Vernier scheme to extend the FSR, resulting in less extinction (~ 60 dB) at the FSRs of the cascaded sub-filters, which are selected not to align with either the pump laser or other single-photon channel when the pump rejection filter is aligned to a particular signal or idler output wavelength. Limited heater tuning range prevented the on-chip filters from being aligned to a photon-pair source resonance wavelength on all tested chips, which is correctable by improving the source and filter heater designs and slightly adjusting the microring radii to target specific resonance wavelengths, reducing the initial error between the source and filter resonances. We have characterized the insertion loss of this filter to be < 1 dB using measurements at a separate test site with through port and drop port grating couplers oriented in the same direction, allowing the same fiber to measure both ports one at a time74.

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Supplementary Sections 1–5.

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Kramnik, D., Wang, I., Ramesh, A. et al. Scalable feedback stabilization of quantum light sources on a CMOS chip. Nat Electron 8, 620–630 (2025). https://doi.org/10.1038/s41928-025-01410-5

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