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

Springer series in solid-state sciences

Josephson Transmission Line Oscillators

Alwyn C. Scott

Published Jan 1, 1978• 1 citation
Publisher
DOI
10.1007/978-3-642-81291-0_32

Related papers

Josephson junction transmission lines

A. Barone, R.D. Permentier

•Feb 1, 1971•0 citations

The phase of the microwave on a Josephson transmission line

E.V. Ponizovska

Applied Superconductivity•May 1, 1995•0 citations

Subpicosecond measurements of the response of Josephson transmission lines to large current pulses

M. Currie, Roman Sobolewski, T.Y. Hsiang

Josephson transmission lines (JTLs) are commonly used as signal interconnects in single-flux quantum (SFQ) circuits. They are also used, however, to transform arbitrary waveforms into SFQ pulses. Here we use a low-temperature electro-optic sampling system with subpicosecond resolution to observe the response of a JTL to a picosecond input pulse. Previously, this system has been used to directly observe SFQ pulses on niobium transmission lines. In our experiment, niobium metal semiconductor-metal (MSM) photodiodes were connected to 3, 4, 19, and 20-stage JTLs. The MSM photodiodes provided picosecond pulses to excite the JTL. The JTL bias and input pulse amplitude were varied to observe fluxon interaction and time delay of the JTL stages. Observed JTL behavior is dominated by dipolar oscillations radiated from the first stages of the JTL. By varying the values of line inductance and junction capacitance, thus changing the oscillation periods, these oscillations were traced to the coupling of the junction capacitance and line inductance. This is a new feature of the JTL that has thus far not been observed or incorporated into simulations. Our results could have significant implications on the limit of SFQ circuits.

IEEE Transactions on Applied Superconductivity•Jun 1, 1999•2 citations

Josephson millimeter wave oscillators

R. Monaco

International Journal of Infrared and Millimeter Waves•Apr 1, 1990•8 citations

Oscillation of SFQ pulse in oxide JTL

Y. Tarutani, H. Sugiyama, K. Tanabe

Characteristics of SFQ signal propagation in oxide circuits were investigated by numerical simulation. The numerical simulation for the SFQ signal propagating in the Josephson transmission line (JTL) was performed by assuming the inductor to be a passive transmission line and by taking into account the high I/sub c/R/sub n/ value of oxide junctions. The SFQ signal was found to oscillate when the inductor length was more than 20 /spl mu/m. The origin of the oscillation and the oscillation conditions were investigated with respect to the Josephson plasma frequency. A shunt resistor connected between an inductor and the groundplane was found to be effective for suppressing the oscillation. The JTL in which shunt resistors are connected may also be used as a delay line.

IEEE Transactions on Applied Superconductivity•Jun 1, 2003•1 citation

Fluxon Feedback Oscillator

Shigeki Sakai, Hiroshi Akoh, Hisao Hayakawa

A fluxon feedback oscillator which is formed by a ring-like Josephson transmission line with a feedback resistor is proposed. A device with a Josephson transmission line made by the NbN/NbN junction is fabricated, and the successful operation of the device is obtained using the Josephson sampler. The oscillation period can be controlled between 35 and 70 ps. The results agree well with simulation results. Possible applications of the fluxon feedback oscillator are also discussed.

Japanese Journal of Applied Physics•Aug 1, 1984•21 citations
Josephson transmission lines (JTLs) are commonly used as signal interconnects in single-flux quantum (SFQ) circuits. They are also used, however, to transform arbitrary waveforms into SFQ pulses. Here we use a low-temperature electro-optic sampling system with subpicosecond resolution to observe the response of a JTL to a picosecond input pulse. Previously, this system has been used to directly observe SFQ pulses on niobium transmission lines. In our experiment, niobium metal semiconductor-metal (MSM) photodiodes were connected to 3, 4, 19, and 20-stage JTLs. The MSM photodiodes provided picosecond pulses to excite the JTL. The JTL bias and input pulse amplitude were varied to observe fluxon interaction and time delay of the JTL stages. Observed JTL behavior is dominated by dipolar oscillations radiated from the first stages of the JTL. By varying the values of line inductance and junction capacitance, thus changing the oscillation periods, these oscillations were traced to the coupling of the junction capacitance and line inductance. This is a new feature of the JTL that has thus far not been observed or incorporated into simulations. Our results could have significant implications on the limit of SFQ circuits.
Characteristics of SFQ signal propagation in oxide circuits were investigated by numerical simulation. The numerical simulation for the SFQ signal propagating in the Josephson transmission line (JTL) was performed by assuming the inductor to be a passive transmission line and by taking into account the high I/sub c/R/sub n/ value of oxide junctions. The SFQ signal was found to oscillate when the inductor length was more than 20 /spl mu/m. The origin of the oscillation and the oscillation conditions were investigated with respect to the Josephson plasma frequency. A shunt resistor connected between an inductor and the groundplane was found to be effective for suppressing the oscillation. The JTL in which shunt resistors are connected may also be used as a delay line.