Combining n-MOS Charge Sensing with p-MOS Silicon Hole Double Quantum Dots in a CMOS platform.

CMOS Quantum dots singlet−triplet relaxation spin-qubit

Journal

Nano letters
ISSN: 1530-6992
Titre abrégé: Nano Lett
Pays: United States
ID NLM: 101088070

Informations de publication

Date de publication:
22 Feb 2023
Historique:
medline: 8 2 2023
pubmed: 8 2 2023
entrez: 7 2 2023
Statut: ppublish

Résumé

Holes in silicon quantum dots are receiving attention due to their potential as fast, tunable, and scalable qubits in semiconductor quantum circuits. Despite this, challenges remain in this material system including difficulties using charge sensing to determine the number of holes in a quantum dot, and in controlling the coupling between adjacent quantum dots. We address these problems by fabricating an ambipolar complementary metal-oxide-semiconductor (CMOS) device using multilayer palladium gates. The device consists of an electron charge sensor adjacent to a hole double quantum dot. We demonstrate control of the spin state via electric dipole spin resonance. We achieve smooth control of the interdot coupling rate over 1 order of magnitude and use the charge sensor to perform spin-to-charge conversion to measure the hole singlet-triplet relaxation time of 11 μs for a known hole occupation. These results provide a path toward improving the quality and controllability of hole spin-qubits.

Identifiants

pubmed: 36748989
doi: 10.1021/acs.nanolett.2c04417
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

1261-1266

Auteurs

Ik Kyeong Jin (IK)

School of Physics, The University of New South Wales, Sydney, New South Wales 2052, Australia.

Krittika Kumar (K)

School of Physics, The University of New South Wales, Sydney, New South Wales 2052, Australia.

Matthew J Rendell (MJ)

School of Physics, The University of New South Wales, Sydney, New South Wales 2052, Australia.

Jonathan Yue Huang (JY)

School of Electrical Engineering and Telecommunications, The University of New South Wales, Sydney, New South Wales 2052, Australia.
Diraq, Sydney, New South Wales 2052, Australia.

Chris C Escott (CC)

School of Electrical Engineering and Telecommunications, The University of New South Wales, Sydney, New South Wales 2052, Australia.
Diraq, Sydney, New South Wales 2052, Australia.

Fay E Hudson (FE)

School of Electrical Engineering and Telecommunications, The University of New South Wales, Sydney, New South Wales 2052, Australia.
Diraq, Sydney, New South Wales 2052, Australia.

Wee Han Lim (WH)

School of Electrical Engineering and Telecommunications, The University of New South Wales, Sydney, New South Wales 2052, Australia.
Diraq, Sydney, New South Wales 2052, Australia.

Andrew S Dzurak (AS)

School of Electrical Engineering and Telecommunications, The University of New South Wales, Sydney, New South Wales 2052, Australia.
Diraq, Sydney, New South Wales 2052, Australia.

Alexander R Hamilton (AR)

School of Physics, The University of New South Wales, Sydney, New South Wales 2052, Australia.

Scott D Liles (SD)

School of Physics, The University of New South Wales, Sydney, New South Wales 2052, Australia.

Classifications MeSH