1985
DOI: 10.1109/tmag.1985.1063777
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A travelling-wave parametric amplifier utilizing Josephson junctions

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Cited by 33 publications
(23 citation statements)
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“…A major challenge in the design of TWPAs, however, is that optimum parametric gain is achieved only when the amplification process is phase matched. TWPAs based on Josephson junctions have been investigated theoretically [22][23][24][25] and experimentally [26-28] but have not demonstrated sufficient gain, in part due to phase-matching limitations, to replace existing semiconductor amplifier technology. TWPAs based on the weaker nonlinear kinetic inductance of thin titanium nitride wires and phase matched through periodic loading have also been demonstrated [29,30], but they require significantly longer propagation lengths and higher pump powers to achieve comparable gain.…”
mentioning
confidence: 99%
“…A major challenge in the design of TWPAs, however, is that optimum parametric gain is achieved only when the amplification process is phase matched. TWPAs based on Josephson junctions have been investigated theoretically [22][23][24][25] and experimentally [26-28] but have not demonstrated sufficient gain, in part due to phase-matching limitations, to replace existing semiconductor amplifier technology. TWPAs based on the weaker nonlinear kinetic inductance of thin titanium nitride wires and phase matched through periodic loading have also been demonstrated [29,30], but they require significantly longer propagation lengths and higher pump powers to achieve comparable gain.…”
mentioning
confidence: 99%
“…In this pioneering experiment a gain of 10 dB and a bandwidth of 3 MHz were shown. After the theorizing and the subsequent discovery of the Josephson effect [2], it was understood that an easy way to embed a non-linear component into a transmission line and simultaneously reduce losses, was to build a non-linear inductance made of superconducting material, exploiting a Josephson junction as a source of non-linearity following the vanguard idea by M. Sweeny and R. Mahler [13]. There the parametric amplifier was modeled by a first-order small-signal theory with the same approach adopted to predict the behaviour of GaAsFET transmission line amplifiers.…”
Section: Historical Evolution Of the Travelling Wave Parametric Amplimentioning
confidence: 99%
“…As an example, a weak signal travelling in a metamaterial can interact with a strong pump tone at a different frequency, activating the so called parametric amplification [12]. The class of devices where these phenomena are promoted is commonly known as Travelling Wave Josephson Parametric Amplifiers (TWJPA) and represents the solid state analogous to optical χ n nonlinear crystals [13].…”
Section: Introductionmentioning
confidence: 99%
“…This configuration constitutes a distributed parametric amplifier since the length of the array of junctions, 9 mm, greatly exceeds the calculated wavelength of 0.65 mm for the 19 GHz signals propagating along the coplanar waveguide. Distributed parametric amplifiers of this type have been discussed in the literature 11 . The amplifier was pumped at the signal carrier frequency, the so-called doubly degenerate mode of operation.…”
Section: ͓S0003-6951͑96͒03546-2͔mentioning
confidence: 99%