Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Foundations of Quantum Mechanics in the Light of New Technology

SUPERCONDUCTING QUANTUM BIT WITH FERROMAGNETIC π-JUNCTION

T. YAMASHITA, Satoshi Takahashi, Sadamichi Maekawa

Published Jun 1, 2006• 0 citations
Publisher
DOI
10.1142/9789812773210_0020

Related papers

Flux-bias-free flux quantum bit with ferromagnetic π junction

Taro Yamashita, Kun Zuo, Yoshiro Urade +4 more

The Japan Society of Applied Physics•Jan 28, 2020•0 citations

Superconducting π Qubit with a Ferromagnetic Josephson Junction

禎通 前川

Physical Review Letters•Jan 1, 2005•0 citations

X-BAND PARAMETRIC AMPLIFIER AND MICROWAVE SQUID USING SINGLETUNNEL- JUNCTION SUPERCONDUCTING INTERFEROMETER

L. S. Kuzmin, K. K. Likharev, V. V. Migulin +2 more

X-BAND PARAMETRIC AMPLIFIER AND MICROWAVE SQUID USING SINGLETUNNEL- JUNCTION SUPERCONDUCTING INTERFEROMETER was published in SQUID '85 Superconducting Quantum Interference Devices and their Applications on page 1029.

De Gruyter eBooks•Dec 31, 1986•7 citations

Demonstration of Low-Power Shift-Register Based on Half-Flux-Quantum Logic

Masamitsu Tanaka, Toranosuke Nakayama, Shoma Tanemura +3 more

We report on low-power operation of the half-flux-quantum (HFQ) shift-register circuit. We used a superconducting quantum interference device composed of two conventional switching junctions (0-junctions) and one π-shifted non-switching magnetic Josephson junction (π-junction) as a switching element, called 0-0-π SQUID. Because the π-shift assists switching by inducing a spontaneous current, the 0-0-π SQUID shows a nominal small critical current value and is easily switched by a weak driving force. This feature allows us to significantly reduce static and dynamic power consumption at junctions and bias-feeding resistors. We carefully designed the HFQ circuit elements using a circuit parameter optimization tool and introducing additional non-switching 0-0-π SQUIDs to compensate for superconductor phase shifts. We fabricated the test circuit of the 4-bit shift-register by forming Nb/PdNi/Nb π-junctions on the Nb four-layer, 10-kA/cm2 device. We successfully obtained correct operation with measured power consumption of 0.12-0.18 μW/bit, which was about 1/10 of the conventional single-flux-quantum shift-register designed with the 0-junctions of the same critical currents and the standard bias voltage.

IEICE Transactions on Electronics•Feb 17, 2025•3 citations

Theory of superconducting π-qubit with a ferromagnetic insulator

Shiro Kawabata, Satoshi Kashiwaya, Yasuhiro Asano +1 more

Physica C Superconductivity•May 1, 2006•15 citations

Phase-shift flux qubit with a ferromagnetic π junction

Taro Yamashita, Kun Zuo, Yoshiro Urade +4 more

Bulletin of the American Physical Society•Mar 2, 2020•0 citations
We report on low-power operation of the half-flux-quantum (HFQ) shift-register circuit. We used a superconducting quantum interference device composed of two conventional switching junctions (0-junctions) and one π-shifted non-switching magnetic Josephson junction (π-junction) as a switching element, called 0-0-π SQUID. Because the π-shift assists switching by inducing a spontaneous current, the 0-0-π SQUID shows a nominal small critical current value and is easily switched by a weak driving force. This feature allows us to significantly reduce static and dynamic power consumption at junctions and bias-feeding resistors. We carefully designed the HFQ circuit elements using a circuit parameter optimization tool and introducing additional non-switching 0-0-π SQUIDs to compensate for superconductor phase shifts. We fabricated the test circuit of the 4-bit shift-register by forming Nb/PdNi/Nb π-junctions on the Nb four-layer, 10-kA/cm2 device. We successfully obtained correct operation with measured power consumption of 0.12-0.18 μW/bit, which was about 1/10 of the conventional single-flux-quantum shift-register designed with the 0-junctions of the same critical currents and the standard bias voltage.