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Digital Control of a Superconducting Qubit Using a Josephson Pulse Generator at 3 K

Scaling of quantum computers to fault-tolerant levels relies critically on the integration of energy-efficient, stable, and reproducible qubit control and readout electronics. In comparison to traditional semiconductor-control electronics (TSCE) located at room temperature, the signals generated by...

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Detalles Bibliográficos
Autores principales: Howe, L., Castellanos-Beltran, M. A., Sirois, A. J., Olaya, D., Biesecker, J., Dresselhaus, P. D., Benz, S. P., Hopkins, P. F.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9888300/
https://www.ncbi.nlm.nih.gov/pubmed/36726390
http://dx.doi.org/10.1103/prxquantum.3.010350
Descripción
Sumario:Scaling of quantum computers to fault-tolerant levels relies critically on the integration of energy-efficient, stable, and reproducible qubit control and readout electronics. In comparison to traditional semiconductor-control electronics (TSCE) located at room temperature, the signals generated by rf sources based on Josephson-junctions (JJs) benefit from small device sizes, low power dissipation, intrinsic calibration, superior reproducibility, and insensitivity to ambient fluctuations. Previous experiments to colocate qubits and JJ-based control electronics have resulted in quasiparticle poisoning of the qubit, degrading the coherence and lifetime of the qubit. In this paper, we digitally control a 0.01-K transmon qubit with pulses from a Josephson pulse generator (JPG) located at the 3-K stage of a dilution refrigerator. We directly compare the qubit lifetime T(1), the coherence time [Formula: see text] , and the thermal occupation P(th) when the qubit is controlled by the JPG circuit versus the TSCE setup. We find agreement to within the daily fluctuations of ±0.5 μs and ±2 μs for T(1) and [Formula: see text] , respectively, and agreement to within the 1% error for P(th). Additionally, we perform randomized benchmarking to measure an average JPG gate error of 2.1 × 10(−2). In combination with a small device size (< 25 mm(2)) and low on-chip power dissipation (≪100 μW), these results are an important step toward demonstrating the viability of using JJ-based control electronics located at temperature stages higher than the mixing-chamber stage in highly scaled superconducting quantum information systems.