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

Elsevier eBooks

HIGH-SENSITIVITY JOSEPHSON LOGIC GATE USING LOW βC DEVICES

Masanori Sugahara, H. Kaneda

Published Jan 1, 1982• 0 citations
Publisher
DOI
10.1016/b978-0-408-01252-2.50135-7

Related papers

JOSEPHSON DEVICES FOR QUANTUM COMPUTING

F. Chiarello, Maria Gabriella Castellano, Roberto Leoni +3 more

Computing tools, all based on classical logic at the moment, present intrinsic limitations that can be overcome by using quantum logic. In this direction, superconducting Josephson devices have been proved to be very suitable candidates for the realization of quantum computing tools. We present some basic elements of quantum computing, possible strategies for the implementation of quantum gates by using Josephson devices, and recent experimental results in this field.

International Journal of Modern Physics B•Mar 10, 2003•0 citations

Logic gates using stacked Josephson junctions

P. D. Shaju, V. C. Kuriakose

Physica C Superconductivity•Sep 1, 1999•13 citations

Analog-to-digital conversion with unlatched SQUID's

John P. Hurrell, David C. Pridmore-Brown, Arnold H. Silver

Digital Josephson circuits that do not latch into the voltage state provide an opportunity for high-speed serial processing. These fast logic gates must ultimately generate and record small fast pulses generated by single fluxoid events. This is demonstrated in a concept for a high-speed analog-to-digital (A/D) converter. Low β-value unlatched SQUID's are used throughout for ultimate speed, sensitivity, and simplicity. The analog signal is quantized by a single-junction SQUID and converted into a pulse train resulting from fluxoid transitions. These are counted in a chain of bistable two-junction SQUID's which successively scale the pulse train by a factor 2. These SQUID's perform both logic and memory functions at the single fluxoid level. The bit count stored in the array is gated out each sampling interval to provide the digitized signal. The performance of this device has been simulated and criteria established for the unlatched SQUID design. These include dimensionality, impedance, damping, intra- and inter-SQUID delays and β factor. Large analog dynamic range is available with the high intrinsic linearity of the SQUID quantizer and a long chain of scalers.

IEEE Transactions on Electron Devices•Oct 1, 1980•77 citations

Josephson devices for high-speed digital circuits

Huang-Tian Chan

•Jan 1, 1977•0 citations

Josephson junction quantum logic gates

Yuriy Makhlin, Gerd Schön, Alexander Shnirman

Computer Physics Communications•May 1, 2000•5 citations

ULTIMATE SENSITIVITY OF SQUIDS USING UNSHUNTED JOSEPHSON TUNNEL-JUNCTIONS

Oleg V. Snigirev

•Jan 1, 1984•1 citation
Digital Josephson circuits that do not latch into the voltage state provide an opportunity for high-speed serial processing. These fast logic gates must ultimately generate and record small fast pulses generated by single fluxoid events. This is demonstrated in a concept for a high-speed analog-to-digital (A/D) converter. Low β-value unlatched SQUID's are used throughout for ultimate speed, sensitivity, and simplicity. The analog signal is quantized by a single-junction SQUID and converted into a pulse train resulting from fluxoid transitions. These are counted in a chain of bistable two-junction SQUID's which successively scale the pulse train by a factor 2. These SQUID's perform both logic and memory functions at the single fluxoid level. The bit count stored in the array is gated out each sampling interval to provide the digitized signal. The performance of this device has been simulated and criteria established for the unlatched SQUID design. These include dimensionality, impedance, damping, intra- and inter-SQUID delays and β factor. Large analog dynamic range is available with the high intrinsic linearity of the SQUID quantizer and a long chain of scalers.