Abstract
As quantum computers grow in complexity, the technology will have to evolve from large distributed systems to compact integrated solutions. Spin qubits in silicon quantum dots are thought to offer good scalability because both spin-carrying quantum dots and support complementary metal–oxide–semiconductor (CMOS) electronics can, in principle, be monolithically integrated on a single chip. However, monolithically integrated quantum–classical hybrid circuits based on industry-standard CMOS technology remain limited. Here we report a millikelvin integrated circuit fabricated using 40 nm CMOS technology that integrates silicon quantum-dot arrays with support electronics in an architecture that allows the array to be efficiently addressed and read. The architecture contains integrated microwave lumped-element resonators for dispersive sensing of the charge state of the quantum dots, mediated via digital transistors in a column–row-addressing distribution. With the chip, we demonstrate combined time- and frequency-division multiplexing, which scales sublinearly the resources as well as footprint required for readout.
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Data availability
The data that support the plots within this paper and other findings of this study are available from the corresponding authors upon reasonable request.
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Acknowledgements
We are grateful to S. Schaal for providing useful comments. M.F.G.-Z. was affiliated with Hitachi Cambridge Laboratory at the time of designing and preparing the experiments and is currently affiliated with Quantum Motion Technologies. The research leading to these results has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement nos. 688539 and 951852. M.F.G.-Z. acknowledges support from the Royal Society, Innovate UK’s Industrial Strategy Challenge Fund and UKRI Future Leaders Fellowship under grant no. MR/V023284/1.
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A.R., M.F.G.-Z. and E.C. conceived the architecture and devised the experiments. A.R. and Y.P. designed the chip with inputs from E.C. and M.F.G.-Z. T.-Y.Y., J.M., M.F.G.-Z. and A.R. performed the experiments and analysed the results. A.R., T.-Y.Y. and M.F.G.-Z. wrote the manuscript with inputs from all the co-authors. M.F.G.-Z. and E.C. supervised all the experiments.
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M.F.G.-Z. is employed by Quantum Motion Technologies, a start-up focusing on building a silicon-based quantum computer. All other authors declare no competing interests.
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Extended data
Extended Data Fig. 1 Experimental measurement setup.
Dilution refrigerator measurement setup for the time- and frequency-multiplexed gate-based readout experiment. The DUT is placed at 50 mK on the sample stage of the dilution refrigerator. A cryogenic circulator is placed at the mixing chamber plate and a low-noise amplifier and attenuators are placed at intermediate cryogenic temperatures (~3 K). At room temperature, two microwave signal sources are power-combined to generate two multiplexed single-tone probing signals fmw1 and fmw2, and two I/Q mixers are used to demodulate the reflected signals RF1 and RF2 at the two frequencies, by using the microwave sources as respective local oscillators LO1 and LO2. An oscilloscope acquires the I/Q outputs for each of the two tones.
Extended Data Fig. 2 Signal-to-noise ratio analysis.
a, Trace of reflectometry signal Vmw as a function of VDL1 from an individual measurement of quantum device Q13, corresponding to the black line section in the bottom left inset (left panel in Fig. 2c). The red curve is a Lorentzian fit to the experimental data. Top left inset: zoom-in of the background noise. σ is the standard deviation of noise signals. b, Trace of Vmw as a function of VDL1 for Q13 from an individual device measurement (middle panel in Fig. 3a). A is the Coulomb peak amplitude from the fit. c, Trace of Vmw as a function of VDL1 for Q13 from the time-domain multiplexing measurement (middle panel in Fig. 3c). The measurement in a was performed in a different cool down thermal cycle with respect to those in b and c, while the measurements in b and c are within the same cool down.
Extended Data Fig. 3 Data processing.
a, A single sweep of reflectometry signal Vmw (grey curve) as a function of time t at VS1 = 0 V corresponding to Fig. 3c. The data show the reflectometry signals from Q12 (t = 0 to 8.33 ms), Q13 (t = 8.33 to 16.67 ms), and Q11 (t = 16.67 to 25 ms). The light blue, light green, and gold curves are fits to the data and are used as backgrounds for data processing. b, Processed reflectometry signals of Q12 (blue), Q13 (green), and Q11 (gold) after subtracting the background fits. The arrows indicate Coulomb-blockade peaks.
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Supplementary Sections 1–5, refs. 53–60, Figs. 1–6 and Tables 1 and 2.
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Ruffino, A., Yang, TY., Michniewicz, J. et al. A cryo-CMOS chip that integrates silicon quantum dots and multiplexed dispersive readout electronics. Nat Electron 5, 53–59 (2022). https://doi.org/10.1038/s41928-021-00687-6
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DOI: https://doi.org/10.1038/s41928-021-00687-6
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