Author
Listed:
- Paul Steinacker
(University of New South Wales)
- Nard Dumoulin Stuyck
(University of New South Wales
Diraq)
- Wee Han Lim
(University of New South Wales
Diraq)
- Tuomo Tanttu
(University of New South Wales
Diraq)
- MengKe Feng
(University of New South Wales
Diraq)
- Santiago Serrano
(University of New South Wales
Diraq)
- Andreas Nickl
(University of New South Wales)
- Marco Candido
(University of New South Wales)
- Jesus D. Cifuentes
(University of New South Wales
Diraq)
- Ensar Vahapoglu
(University of New South Wales
Diraq)
- Samuel K. Bartee
(University of New South Wales
Diraq)
- Fay E. Hudson
(University of New South Wales
Diraq)
- Kok Wai Chan
(University of New South Wales
Diraq)
- Stefan Kubicek
(Imec)
- Julien Jussot
(Imec)
- Yann Canvel
(Imec)
- Sofie Beyne
(Imec)
- Yosuke Shimura
(Imec)
- Roger Loo
(Imec
Ghent University)
- Clement Godfrin
(Imec)
- Bart Raes
(Imec)
- Sylvain Baudot
(Imec)
- Danny Wan
(Imec)
- Arne Laucht
(University of New South Wales
Diraq)
- Chih Hwan Yang
(University of New South Wales
Diraq)
- Andre Saraiva
(Diraq)
- Christopher C. Escott
(Diraq)
- Kristiaan Greve
(Imec
KU Leuven)
- Andrew S. Dzurak
(University of New South Wales
Diraq)
Abstract
Among the many types of qubit presently being investigated for a future quantum computer, silicon spin qubits with millions of qubits on a single chip are uniquely positioned to enable quantum computing. However, it has not been clear whether the outstanding high-fidelity operations and long coherence times shown by silicon spin qubits fabricated in academic settings1–8 can be reliably reproduced when the qubits are manufactured in a semiconductor foundry9–11. Here we show precise qubit operation of silicon two-qubit devices made with standard semiconductor tooling in a 300-mm foundry environment. Of the key metrics, single- and two-qubit control fidelities exceed 99% for all four devices, and the state preparation and measurement fidelities reach up to 99.9%, as evidenced by gate set tomography. We report spin lifetime and coherence up to T1 = 9.5 s, $${T}_{2}^{* }=40.6\,{\rm{\mu }}{\rm{s}}$$ T 2 * = 40.6 μ s and $${T}_{2}^{{\rm{Hahn}}}=1.9\,{\rm{ms}}$$ T 2 Hahn = 1.9 ms . We determine that residual nuclear spin-carrying isotopes contribute substantially to operational errors, identifying further isotopic purification as a clear pathway to even higher performance.
Suggested Citation
Paul Steinacker & Nard Dumoulin Stuyck & Wee Han Lim & Tuomo Tanttu & MengKe Feng & Santiago Serrano & Andreas Nickl & Marco Candido & Jesus D. Cifuentes & Ensar Vahapoglu & Samuel K. Bartee & Fay E. , 2025.
"Industry-compatible silicon spin-qubit unit cells exceeding 99% fidelity,"
Nature, Nature, vol. 646(8083), pages 81-87, October.
Handle:
RePEc:nat:nature:v:646:y:2025:i:8083:d:10.1038_s41586-025-09531-9
DOI: 10.1038/s41586-025-09531-9
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