2015
DOI: 10.1063/1.4933265
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Characterization of a multimode coplanar waveguide parametric amplifier

Abstract: We characterize a novel Josephson parametric amplifier based on a flux-tunable quarter-wavelength resonator. The fundamental resonance frequency is ∼1 GHz, but we use higher modes of the resonator for our measurements. An on-chip tuning line allows for magnetic flux pumping of the amplifier. We investigate and compare degenerate parametric amplification, involving a single mode, and nondegenerate parametric amplification, using a pair of modes. We show that we reach quantum-limited noise performance in both ca… Show more

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Cited by 43 publications
(41 citation statements)
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“…The layout of the device is similar to that in Ref. [22]. The distance between the interdigitated coupling capacitor and the SQUID is 31 mm, yielding a fundamental resonant frequency ω 1 /2π = 912 MHz.…”
Section: Experimental Methodsmentioning
confidence: 85%
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“…The layout of the device is similar to that in Ref. [22]. The distance between the interdigitated coupling capacitor and the SQUID is 31 mm, yielding a fundamental resonant frequency ω 1 /2π = 912 MHz.…”
Section: Experimental Methodsmentioning
confidence: 85%
“…For instance, the presence of an idler in parametric amplification below the parametric instability threshold defines the structure of a squeezed vacuum and twomode entanglement of the output photons [4][5][6]. This is true for both degenerate and nondegenerate parametric resonances, with the only difference being that for the nondegenerate case, the idler has a frequency far detuned from the signal frequency and appears within the bandwidth of the conjugated mode [22], while for the degenerate case, the idler appears within the bandwidth of the signal mode.…”
Section: B Response To An External Signalmentioning
confidence: 99%
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“…For this purpose, one can either use broadband traveling wave parametric amplifiers [1,2] or band tunable narrow-band JPAs [3][4][5][6]. The latter are nowadays routinely used to provide amplification with a noise performance close to the standard quantum limit [7][8][9][10][11][12]. Moreover, if operated in the phase sensitive regime, JPAs can even achieve noise temperatures below the standard quantum limit [11,13,14].…”
Section: Introductionmentioning
confidence: 99%
“…Tuning the resonance frequency is a pre-requisite for the dynamic coupling of quantum bits (qubits), 12 controllable storage and release of microwave photons, 13 photon generation via the dynamical Casimir effect, 14 and parametric amplification. 15,16 In all the above examples, the frequency tuning was achieved in CPW resonators by inserting a superconducting quantum interference device (SQUID) into the resonator as a control element. Such a scheme allows for fast ($1 ns) and wide range ($700 MHz) tuning but at the expense of introducing an extra dissipation channel associated with the SQUID.…”
mentioning
confidence: 99%