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

Bulletin of the American Physical Society

Near-Quantum-Limited SQUID Amplifier

John L. Clarke

Published Mar 18, 2009• 0 citations
OpenAlex

Related papers

A tunable parametric amplifier based on a SQUID array resonator with nearly quantum-limited sensitivity

Manuel A. Castellanos-Beltran, Konrad W. Lehnert

Bulletin of the American Physical Society•Mar 14, 2008•0 citations

Development of SQUID Amplifiers for Axion Search Experiments

Sergey V. Uchaikin, Andrei N. Matlashov, Doyu Lee +11 more

We report results of our development of two types of microwave amplifiers based on Superconducting quantum interference devices (SQUIDs) for CAPP (Center for Axion and Precision Physics Research) axion search experiments. The first amplifier, Microstrip SQUID Amplifier (MSA) has a wide bandwidth. Power dissipation in resistive shunts results in a device overheating and limits the MSA performances. A thermal models of shunt cooling processes is developed and recommendations for a future design is provided. The second amplifier, Josephson Parametric Amplifier (JPA), at limited bandwidth showed a low noise near the standard quantum limit (SQL) of 196 mK. Implementation of a JPA in CULTASK (CAPP's Ultra-Low Temperature Axion Search in Korea) experiment is planned in the end of 2019.

IEEE International Superconductive Electronics Conference (ISEC)•Jul 1, 2019•3 citations

The microstrip SQUID amplifier

Roy Therrien

•Jan 1, 2002•0 citations

Superconducting quantum interference device as a near-quantum-limited amplifier at 0.5 GHz

Michael Mück, Jan B. Kycia, John L. Clarke

A dc superconducting quantum interference device (SQUID) with a resonant microstrip input is operated as an amplifier at temperatures down to 20 mK. A second SQUID is used as a postamplifier. Below about 100 mK, the noise temperature is 52±20 mK at 538 MHz, estimated from measurements of signal-to-noise ratio, and 47±10 mK at 519 MHz, estimated from the noise generated by a resonant circuit coupled to the input. The quantum-limited noise temperatures are 26 and 25 mK, respectively. The measured noise temperature is limited by hot electrons generated by the bias current.

Applied Physics Letters•Feb 12, 2001•119 citations

Microstrip SQUID amplifiers for quantum information science

M. P. DeFeo, B. L. T. Plourde

Bulletin of the American Physical Society•Feb 28, 2012•0 citations

Properties of 4 GHz SQUID amplifier

G.V. Prokopenko, V. P. Koshelets, J. Mygind

•Jan 1, 1999•0 citations
We report results of our development of two types of microwave amplifiers based on Superconducting quantum interference devices (SQUIDs) for CAPP (Center for Axion and Precision Physics Research) axion search experiments. The first amplifier, Microstrip SQUID Amplifier (MSA) has a wide bandwidth. Power dissipation in resistive shunts results in a device overheating and limits the MSA performances. A thermal models of shunt cooling processes is developed and recommendations for a future design is provided. The second amplifier, Josephson Parametric Amplifier (JPA), at limited bandwidth showed a low noise near the standard quantum limit (SQL) of 196 mK. Implementation of a JPA in CULTASK (CAPP's Ultra-Low Temperature Axion Search in Korea) experiment is planned in the end of 2019.
A dc superconducting quantum interference device (SQUID) with a resonant microstrip input is operated as an amplifier at temperatures down to 20 mK. A second SQUID is used as a postamplifier. Below about 100 mK, the noise temperature is 52±20 mK at 538 MHz, estimated from measurements of signal-to-noise ratio, and 47±10 mK at 519 MHz, estimated from the noise generated by a resonant circuit coupled to the input. The quantum-limited noise temperatures are 26 and 25 mK, respectively. The measured noise temperature is limited by hot electrons generated by the bias current.