Controlling the dynamic range of a Josephson parametric amplifier
By Christopher Eichler, Andreas Wallraff. 2013
152 citations recorded by the source corpus.
One of the central challenges in the development of parametric amplifiers is the control of the dynamic range relative to its gain and bandwidth, which typically limits quantum limited amplification to signals which contain only a few photons per inverse bandwidth. Here, we discuss the control of the dynamic range of Josephson parametric amplifiers by using Josephson junction arrays. We discuss gain, bandwidth, noise, and dynamic range properties of both a transmission line and a lumped element based parametric amplifier. Based on these investigations we derive useful design criteria, which may find broad application in the development of practical parametric amplifiers.
Subfields: Artificial Intelligence, Atomic and Molecular Physics, and Optics, Electrical and Electronic Engineering
View Paper: https://www.semanticscholar.org/paper/a6273e14ee027ff181c16e27470e15d88531a9a0
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In Artificial Intelligence
- Steven M. Girvin
- Alexandre Blais
- Andreas Wallraff
- Michel H. Devoret
- A. Grimsmo
- Robert J. Schoelkopf
- V. Sivak
- S. Gasparinetti
In Atomic and Molecular Physics, and Optics
- Steven M. Girvin
- Alexandre Blais
- Andreas Wallraff
- Michel H. Devoret
- A. Grimsmo
- Robert J. Schoelkopf
- S. Gasparinetti
- Franco Nori
In Electrical and Electronic Engineering
Citations in the corpus
- Strong Coupling Cavity QED with Gate-Defined Double Quantum Dots Enabled by a High Impedance Resonator (2017, background): “At higher drive strength, the nonlinearity of the device is observed and may be characterized in spectroscopic measurements [29].”
- Circuit quantum electrodynamics (2020, background): “Importantly, this can be done without degrading the amplifier’s bandwidth (Eichler and Wallraff, 2014).”
- Optimizing the Nonlinearity and Dissipation of a SNAIL Parametric Amplifier for Dynamic Range (2018, methodology): “The SPA is based on an array of SNAILs [12,13], which provides the flexibility needed to optimize the three-wave-mixing amplification process, while simultaneously minimizing the four-wavemixing Kerr nonlinearity suspected to cause amplifier saturation [14,15].”