1988
DOI: 10.1103/physrevlett.60.764
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Observation of 4.2-K equilibrium-noise squeezing via a Josephson-parametric amplifier

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Cited by 227 publications
(170 citation statements)
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“…To reconstruct the output field, we first deconvolve D [|0 0|] (S) with Q vacuum to obtain 1 Gc P HEMT and then deconvolve D [ρ] (S) with 1 Gc P HEMT to obtain Q JPA . Both deconvolutions are performed in Matlab using the LucyRichardson method [78].…”
Section: Discussionmentioning
confidence: 99%
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“…To reconstruct the output field, we first deconvolve D [|0 0|] (S) with Q vacuum to obtain 1 Gc P HEMT and then deconvolve D [ρ] (S) with 1 Gc P HEMT to obtain Q JPA . Both deconvolutions are performed in Matlab using the LucyRichardson method [78].…”
Section: Discussionmentioning
confidence: 99%
“…1(b), the lumped-element JPA is simply a capacitively shunted Josephson junction coupled to a transmission line [1,7]. The Hamiltonian of this standard circuit iŝ…”
Section: A Jpa Circuitmentioning
confidence: 99%
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“…Nevertheless, the considered qubit constitutes an open system. Our choice of a finite bosonic environment is motivated by recent progress in quantum engineering of non-classical electromagnetic fields which can be prepared in various states, both in the optical [22] and in the microwave [23] energetic regimes. As an example, we consider a single boson mode.…”
Section: Model B: Qubit Coupled To a Finite Environmentmentioning
confidence: 99%
“…The next step in this line of research is to consider nonclassical electromagnetic fields [15,16] which are carefully prepared in a particular quantum state, and study their effect on quantum interference [9,10]. In this case it is shown that the quantum noise in the electromagnetic field destroys partly the electron interference fringes.…”
Section: Introductionmentioning
confidence: 99%