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Along with the resurgent use of parametric amplifiers as applied to quantum systems, a quantum optics formalism is also typically adopted to explain the amplifier.
The use of parametric amplifiers with Josephson junctions was pioneered by several researchers in the 1970s [2 6], as well as Bernard Yurke in the 1980s [7, 8].
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In this context some authors have proposed the use of parametric and non-parametric flexible models.
Superconducting circuits can also be used to build parametric amplifiers in the microwave domain.
Here, we discuss the control of the dynamic range of Josephson parametric amplifiers by using Josephson junction arrays.
The dynamic clocked comparator using a parametric amplifier is proposed and designed using a concept of the charge transfer amplification (CTA).
The pump pulse of 570 nm was created using an optical parametric amplifier and a series of filters (TOPAS-NIRUVIS).
One beam was used to generate the pump beam at 590 nm using an optical parametric amplifier (OPA).
From this point of view, parametric amplifiers may be divided into two groups; phase sensitive amplifiers which amplify only one of the incoming quadratures, and phase insensitive amplifiers which amplify both quadratures, thereby preserving the phase of the signal.
Based on these investigations we derive useful design criteria, which may find broad application in the development of practical parametric amplifiers.
There are two major advantages of superconducting parametric amplifiers: (i) they have very low dissipation, and (ii) they have well characterized and engineer-able properties.
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