A Cryo-CMOS Low-Power Semi-Autonomous Transmon Qubit State Controller in 14-nm FinFET Technology

A scalable, non-multiplexed cryogenic 14-nm FinFET quantum bit (qubit) state controller (QSC) for use in the semi-autonomous control of superconducting transmon qubits is reported. The QSC includes an augmented general-purpose digital processor that supports waveform generation and phase rotation op...

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Veröffentlicht in:IEEE journal of solid-state circuits 2022-11, Vol.57 (11), p.3258-3273
Hauptverfasser: Chakraborty, Sudipto, Frank, David J., Tien, Kevin, Rosno, Pat, Yeck, Mark, Glick, Joseph A., Robertazzi, Raphael, Richetta, Ray, Bulzacchelli, John F., Underwood, Devin, Ramirez, Daniel, Yilma, Dereje, Davies, Andrew, Joshi, Rajiv V., Chambers, Shawn D., Lekuch, Scott, Inoue, Ken, Wisnieff, Dorothy, Baks, Christian W., Bethune, Donald S., Timmerwilke, John, Fox, Thomas, Song, Peilin, Johnson, Blake R., Gaucher, Brian P., Friedman, Daniel J.
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Sprache:eng
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Zusammenfassung:A scalable, non-multiplexed cryogenic 14-nm FinFET quantum bit (qubit) state controller (QSC) for use in the semi-autonomous control of superconducting transmon qubits is reported. The QSC includes an augmented general-purpose digital processor that supports waveform generation and phase rotation operations combined with a low-power current-mode single sideband upconversion {I}/{Q} mixer-based RF arbitrary waveform generator (AWG). Implemented in the 14-nm CMOS FinFET technology, the QSC generates control signals in its target 4.5-5.5-GHz-frequency range, achieving an spurious free dynamic range (SFDR) > 50 dB for a signal bandwidth of 500 MHz. With the controller operating in the 4 K stage of a cryostat and connected to a transmon qubit in the cryostat's millikelvin stage, measured transmon T_{1} and T_{2} coherence times were 75.7 and 73 \mu \text{s} , respectively, in each case comparable to results achieved using conventional room temperature (RT) controls. In further tests with transmons, a qubit-limited error rate of 7.76 × 10−4 per Clifford gate is achieved, again comparable to the results achieved using RT controls. The QSC's maximum RF output power is −18 dBm, and power dissipation per qubit under active control is 23 mW.
ISSN:0018-9200
1558-173X
DOI:10.1109/JSSC.2022.3201775