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

Cryogenics

Rf-biased SQUID with half-wavelength transmission line

Thomas W. Bradshaw, William P. Pratt

Published Sep 1, 1979• 2 citations
Publisher
DOI
10.1016/0011-2275(79)90014-6

Related papers

Measurement of the input resistance of a rf biased SQUID

S.S. Tinchev, P. Gutmann

Cryogenics•Sep 1, 1983•0 citations

Measurement of the input impedance of a rf biased SQUID

Franco Bordoni, I. Modena, Romani G. L. +1 more

•Jan 1, 1979•0 citations

Planar Microwave Biased rf-SQUIDs with a Cryogenic HEMT amplifier

R. Mezzena, Stefano Vitale

•Jan 1, 1992•0 citations

An on-chip superconducting clock with two modes

G.S. Lee, Arnold H. Silver, Robert D. Sandell

A superconducting clock based on a 2-junction SQUID (superconducting quantum interference device) flip-flop with feedback is presented. The feedback consists of transmission lines that emanate from and return to the SQUID; the entire clock is built as a compact integrated circuit. The period of the clock is mainly determined by the length of transmission line, and there are two modes of operation that can be separately excited whose periods are in a ratio of 2:1. I-V data for a pair of clocks with different designed periods confirm the presence of the two modes, show how period depends on length, and give information on the switching time of the SQUID flip-flops. Specifically, the I-V data show that there exist both a fundamental model for flux bias at odd multiples of Phi /sub 0//2 (half-flux quantum) and a doubled mode with precisely half the period flux bias at even multiples. Clocks with longer transmission lines have longer periods, but simple scaling does not occur due to other sources of time delay.>

IEEE Transactions on Magnetics•Mar 1, 1989•1 citation

RF-SQUID CHARACTERISTICS IN A HIGH-FREQUENCY LIMIT

Oleg V. Snigirev

•Jan 1, 1981•0 citations

Radio frequency bias current scheme for dc superconducting quantum interference device

Y. Zhang, Dongfeng He, N. Wolters +7 more

We have developed a radio frequency bias current scheme with reversal frequency up to 50 MHz for dc superconducting quantum interference devices (SQUIDs). The SQUID and the readout electronics, were connected via a quarter wavelength (/spl lambda//4) transmission line. This transmission line not only transported the SQUID signal, but also served as the resonant matching circuit. For a dc SQUID of inductance 115 pH (loop size 75/spl times/75 /spl mu/m/sup 2/), we measured a flux noise of 33 /spl mu//spl phi//sub 0///spl radic/Hz at 77 K in the flux locked loop configuration. The corner frequency of 1/f noise was less than 0.5 Hz.

IEEE Transactions on Applied Superconductivity•Jun 1, 1999•0 citations
A superconducting clock based on a 2-junction SQUID (superconducting quantum interference device) flip-flop with feedback is presented. The feedback consists of transmission lines that emanate from and return to the SQUID; the entire clock is built as a compact integrated circuit. The period of the clock is mainly determined by the length of transmission line, and there are two modes of operation that can be separately excited whose periods are in a ratio of 2:1. I-V data for a pair of clocks with different designed periods confirm the presence of the two modes, show how period depends on length, and give information on the switching time of the SQUID flip-flops. Specifically, the I-V data show that there exist both a fundamental model for flux bias at odd multiples of Phi /sub 0//2 (half-flux quantum) and a doubled mode with precisely half the period flux bias at even multiples. Clocks with longer transmission lines have longer periods, but simple scaling does not occur due to other sources of time delay.>
We have developed a radio frequency bias current scheme with reversal frequency up to 50 MHz for dc superconducting quantum interference devices (SQUIDs). The SQUID and the readout electronics, were connected via a quarter wavelength (/spl lambda//4) transmission line. This transmission line not only transported the SQUID signal, but also served as the resonant matching circuit. For a dc SQUID of inductance 115 pH (loop size 75/spl times/75 /spl mu/m/sup 2/), we measured a flux noise of 33 /spl mu//spl phi//sub 0///spl radic/Hz at 77 K in the flux locked loop configuration. The corner frequency of 1/f noise was less than 0.5 Hz.