Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency Fluxoniums
We demonstrate a controlled-Z gate between capacitively coupled fluxonium qubits with transition frequencies 72.3 and 136.3 MHz. The gate is activated by a 61.6-ns-long pulse at a frequency between noncomputational transitions |10⟩-|20⟩ and |11⟩-|21⟩, during which the qubits complete only four and e...
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American Physical Society
2021-05-01
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Series: | Physical Review X |
Online Access: | http://doi.org/10.1103/PhysRevX.11.021026 |
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doaj-25e56d548f74432b9b79eb9e361e537e2021-05-03T15:10:53ZengAmerican Physical SocietyPhysical Review X2160-33082021-05-0111202102610.1103/PhysRevX.11.021026Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency FluxoniumsQuentin FicheuxLong B. NguyenAaron SomoroffHaonan XiongKonstantin N. NesterovMaxim G. VavilovVladimir E. ManucharyanWe demonstrate a controlled-Z gate between capacitively coupled fluxonium qubits with transition frequencies 72.3 and 136.3 MHz. The gate is activated by a 61.6-ns-long pulse at a frequency between noncomputational transitions |10⟩-|20⟩ and |11⟩-|21⟩, during which the qubits complete only four and eight Larmor periods, respectively. The measured gate error of (8±1)×10^{-3} is limited by decoherence in the noncomputational subspace, which will likely improve in the next-generation devices. Although our qubits are about 50 times slower than transmons, the two-qubit gate is faster than microwave-activated gates on transmons, and the gate error is on par with the lowest reported. Architectural advantages of low-frequency fluxoniums include long qubit coherence time, weak hybridization in the computational subspace, suppressed residual ZZ-coupling rate (here 46 kHz), and the absence of either excessive parameter-matching or complex pulse-shaping requirements.http://doi.org/10.1103/PhysRevX.11.021026 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Quentin Ficheux Long B. Nguyen Aaron Somoroff Haonan Xiong Konstantin N. Nesterov Maxim G. Vavilov Vladimir E. Manucharyan |
spellingShingle |
Quentin Ficheux Long B. Nguyen Aaron Somoroff Haonan Xiong Konstantin N. Nesterov Maxim G. Vavilov Vladimir E. Manucharyan Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency Fluxoniums Physical Review X |
author_facet |
Quentin Ficheux Long B. Nguyen Aaron Somoroff Haonan Xiong Konstantin N. Nesterov Maxim G. Vavilov Vladimir E. Manucharyan |
author_sort |
Quentin Ficheux |
title |
Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency Fluxoniums |
title_short |
Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency Fluxoniums |
title_full |
Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency Fluxoniums |
title_fullStr |
Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency Fluxoniums |
title_full_unstemmed |
Fast Logic with Slow Qubits: Microwave-Activated Controlled-Z Gate on Low-Frequency Fluxoniums |
title_sort |
fast logic with slow qubits: microwave-activated controlled-z gate on low-frequency fluxoniums |
publisher |
American Physical Society |
series |
Physical Review X |
issn |
2160-3308 |
publishDate |
2021-05-01 |
description |
We demonstrate a controlled-Z gate between capacitively coupled fluxonium qubits with transition frequencies 72.3 and 136.3 MHz. The gate is activated by a 61.6-ns-long pulse at a frequency between noncomputational transitions |10⟩-|20⟩ and |11⟩-|21⟩, during which the qubits complete only four and eight Larmor periods, respectively. The measured gate error of (8±1)×10^{-3} is limited by decoherence in the noncomputational subspace, which will likely improve in the next-generation devices. Although our qubits are about 50 times slower than transmons, the two-qubit gate is faster than microwave-activated gates on transmons, and the gate error is on par with the lowest reported. Architectural advantages of low-frequency fluxoniums include long qubit coherence time, weak hybridization in the computational subspace, suppressed residual ZZ-coupling rate (here 46 kHz), and the absence of either excessive parameter-matching or complex pulse-shaping requirements. |
url |
http://doi.org/10.1103/PhysRevX.11.021026 |
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