2012
DOI: 10.1103/physreva.86.013814
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Josephson-junction-embedded transmission-line resonators: From Kerr medium to in-line transmon

Abstract: We provide a general method to find the Hamiltonian of a linear circuit in the presence of a nonlinearity. Focussing on the case of a Josephson junction embedded in a transmission-line resonator, we solve for the normal modes of the system by taking into account exactly the effect of the quadratic (i.e. inductive) part of the Josephson potential. The nonlinearity is then found to lead to self and cross-Kerr effects, as well as beam-splitter type interactions between modes. By adjusting the parameters of the ci… Show more

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Cited by 178 publications
(241 citation statements)
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“…The Josephson junction provides the nonlinearity through the term E J cos(2π/ 0 δφ) in the effective action. Here E J is the Josephson energy, 0 the flux quanta, and δφ the jump in the flux at both sides of the junction [33,34]. In Ref.…”
Section: Circuit-qed Implementationmentioning
confidence: 99%
“…The Josephson junction provides the nonlinearity through the term E J cos(2π/ 0 δφ) in the effective action. Here E J is the Josephson energy, 0 the flux quanta, and δφ the jump in the flux at both sides of the junction [33,34]. In Ref.…”
Section: Circuit-qed Implementationmentioning
confidence: 99%
“…As the leading neglected correction is of order Λ 2 /ω 0 , this approximation is valid in the regime |Λ| /ω 0 1 which is relevant for typical JPA frequencies and Kerr nonlinearities corresponding to |Λ| /ω 0 ∼ 10 −2 to 10 −6 [44]. We note that the Transmon qubit has the same circuit and Hamiltonian as a JPA but operates at larger Kerr nonlinearities [45].…”
Section: A Jpa Circuitmentioning
confidence: 98%
“…To keep the notation light, we neglect this simple renormalization of parameters in the present work. While the Kerr Hamiltonian was obtained from the lumped-element circuit, the same Hamiltonian with renormalized parameters would apply for a distributed nonlinear resonator in the single-mode approximation [9,44], or a lumped-element JPA with additional linear inductances [36]. However, it is worth noting that, in both cases, the additional inductances can reduce the validity of the quartic potential approximation.…”
Section: A Jpa Circuitmentioning
confidence: 99%
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“…The source of squeezing is a Josephson parametric amplifier pumped at twice the cavity frequency, which is described well by H 1 [33]. In the strong dispersive regime, the qubit is sufficiently far detuned from the cavity that, provided the number of photons in the cavity remains low, it is never significantly excited.…”
Section: Realization In Circuit Qedmentioning
confidence: 99%