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Using Cryogenic CMOS Control Electronics to Enable a Two-Qubit Cross-Resonance Gate

delete2024-02-14
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OA
AI
D
Devin Underwood *
J
Joseph Glick
K
Ken Inoue
D
D.J. Frank
J
John Timmerwilke
E
Emily Pritchett
S
Sudipto Chakraborty
K
Kevin Tien
M
Mark Yeck
J
John F. Bulzacchelli
C
Chris Baks
R
R. P. Robertazzi
M
Matthew J. Beck
R
Rajiv Joshi
D
Dorothy Wisnieff
S
Scott Lekuch
B
B. Gaucher
D
Daniel J. Friedman
P
Pat Rosno
R
Ramirez, Daniel
J
Jeff Ruedinger
DOI:10.1103/PRXQuantum.5.010326delete
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Abstract

Abstract

En 中文
Qubit control electronics composed of CMOS circuits are of critical interest for next-generation quantum computing systems. A CMOS-based application-specific integrated circuit (ASIC) fabricated in 14-nm fin field-effect transistor (FinFET) technology was used to generate and sequence qubit control wave forms and demonstrate a two-qubit cross-resonance gate between fixed-frequency transmons. The controller was thermally anchored to the T = 4 K stage of a dilution refrigerator and the measured power was 23 mW per qubit under active control. The chip generated single-side banded output frequencies between 4.5 and 5.5 GHz, with a maximum power output of -18 dBm. Randomized-benchmarking (RB) experiments revealed an average number of 1.71 instructions per Clifford (IPC) for single-qubit gates and 17.51 IPC for two-qubit gates. A single-qubit error per gate of E1Q = 8 x 10-4 and a two-qubit error per gate of E2Q = 1.4 x 10-2 were shown. A drive-induced Z rotation was observed by way of a rotary-echo experiment; this observation is consistent with the expected qubit behavior given the measured excess local-oscillator (LO) leakage from the CMOS chip. The effect of spurious drive-induced Z errors was numerically evaluated with a two-qubit model Hamiltonian and shown to be in good agreement with the measured RB data. The modeling results suggest that the Z error varies linearly with the pulse amplitude.

Journal

P
PRX Quantum
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international business machines (ibm)
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