2021 IEEE International Solid- State Circuits Conference (ISSCC) 2021
DOI: 10.1109/isscc42613.2021.9365762
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13.1 A Fully Integrated Cryo-CMOS SoC for Qubit Control in Quantum Computers Capable of State Manipulation, Readout and High-Speed Gate Pulsing of Spin Qubits in Intel 22nm FFL FinFET Technology

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Cited by 63 publications
(19 citation statements)
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“…This variability is clearly observed in recent cryo-CMOS integrated circuits for qubit interfacing, as SH ranged from 1 to 3 K in a 40-nm bulk-CMOS high-speed ADC with low power density [26] to more than 10 K in a 22-nm FinFET microwave driver [12]. As device geometry and power density differ considerably between advanced bulk CMOS nodes and the previously studied mature technologies, it is necessary from a modeling perspective to characterize SH on devices better resembling those employed in practical cryo-CMOS designs [26]- [29], both in geometry and power density. Understanding the impact of SH is especially crucial for the cryo-CMOS low-noise amplifiers (LNA) necessary for the detection of the weak signals from quantum processors, as an increase of the device temperature of only a few Kelvin can strongly affect the noise performance, e.g., in a thermal-noiselimited amplifier in which the noise is directly proportional to the device temperature.…”
Section: Imentioning
confidence: 99%
“…This variability is clearly observed in recent cryo-CMOS integrated circuits for qubit interfacing, as SH ranged from 1 to 3 K in a 40-nm bulk-CMOS high-speed ADC with low power density [26] to more than 10 K in a 22-nm FinFET microwave driver [12]. As device geometry and power density differ considerably between advanced bulk CMOS nodes and the previously studied mature technologies, it is necessary from a modeling perspective to characterize SH on devices better resembling those employed in practical cryo-CMOS designs [26]- [29], both in geometry and power density. Understanding the impact of SH is especially crucial for the cryo-CMOS low-noise amplifiers (LNA) necessary for the detection of the weak signals from quantum processors, as an increase of the device temperature of only a few Kelvin can strongly affect the noise performance, e.g., in a thermal-noiselimited amplifier in which the noise is directly proportional to the device temperature.…”
Section: Imentioning
confidence: 99%
“…The junction geometry opens space between modules to route the gate lines and/or to place cryogenic classical electronics in the quantum processor plane [10,34]. Fabricating the qubits and the classical control layer using the same technology is appealing because it will facilitate the integration process, improving feedback speeds in error-correction protocols, and offer potential solutions to wiring and layout challenges [7,[77][78][79][80][81]. Integrating classical and quantum devices monolithically, using CMOS processes, enables the quantum processor to profit from the most mature industrial technology for the fabrication of large-scale circuits [35].…”
Section: Discussionmentioning
confidence: 99%
“…This variability is clearly observed in recent cryo-CMOS integrated circuits for qubit interfacing, as SH ranged from 1 to 3 K in a 40-nm bulk-CMOS high-speed ADC [26] to more than 10 K in a 22-nm FinFET microwave driver [12]. As device geometry and power density differ considerably between advanced bulk CMOS nodes and the previously studied mature technologies, it is necessary from a modeling perspective to characterize SH on devices better resembling those employed in practical cryo-CMOS designs [26]- [29], both in geometry and power density. Understanding the impact of SH is especially crucial for the cryo-CMOS low-noise amplifiers (LNA) necessary for the detection of the weak signals from quantum processors, as an increase of the device temperature of only a few Kelvin can strongly affect the noise performance, e.g., in a thermal-noiselimited amplifier in which the noise is directly proportional to the device temperature.…”
Section: Imentioning
confidence: 99%