2015
DOI: 10.1103/physrevb.91.014507
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Bloch band dynamics of a Josephson junction in an inductive environment

Abstract: We have measured the current-voltage characteristics of a Josephson junction with tunable Josephson energy E J embedded in an inductive environment provided by a chain of SQUIDs. Such an environment induces localization of the charge on the junction, which results in an enhancement of the zero-bias resistance of the circuit. We explain this result quantitatively in terms of the Bloch band dynamics of the localized charge. This dynamics is governed by charge diffusion in the lowest Bloch band of the Josephson j… Show more

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Cited by 36 publications
(38 citation statements)
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“…This is correct for relatively short chains, with N < 2C/C 0 . Yet for longer chains, these modes appear and their effect on the phase-slip amplitude is non-negligible 19,20 . Indeed, in the thermodynamic limit, it is the interplay between the modes and the phase-slips that leads to the superconductor-insulator transition.…”
Section: Introductionmentioning
confidence: 99%
“…This is correct for relatively short chains, with N < 2C/C 0 . Yet for longer chains, these modes appear and their effect on the phase-slip amplitude is non-negligible 19,20 . Indeed, in the thermodynamic limit, it is the interplay between the modes and the phase-slips that leads to the superconductor-insulator transition.…”
Section: Introductionmentioning
confidence: 99%
“…The results presented in this paper are relevant for recent experiments on Josephson junction chains [43] and nanowires [47,50]. In these works, typical phase-slip energies U 0 are in the range of 1-10 GHz, whereas the environmental inductances L are 50-500 nH.…”
Section: Discussionmentioning
confidence: 71%
“…The larger L, the smaller E L , and the larger the ratio U 0 /E L , thus favoring a well-defined charge state of the QPSJ. Recent experiments on nanowires [47,50] and chains of Josephson junctions [43] typically achieve U 0 /E L ratios that are of the order of 10 −2 -10 −1 . We will analyze the microwave response of a QPSJ in this regime in detail and study in particular the resolution and accuracy of the dual Shapiro steps.…”
Section: Introductionmentioning
confidence: 99%
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“…Typically, because both the fine structure constant and atomic dipoles are small, matter-light coupling is weak, allowing treatment by simple and controlled methodologies, such as the rotating wave approximation (RWA), Born-Markov schemes, and Fock space truncation [1]. However, recent artificial systems such as superconducting waveguides [2][3][4][5][6][7], especially the ones using Josephson junction elements to boost the circuit impedance [8][9][10][11][12], constitute metamaterials where charge density fluctuations mimic an optical-like medium in which the coupling to matter (namely superconducting qubits) can be ultra strong. In this situation, a plethora of interesting phenomena, such as wide-band frequency conversion [13], large nonlinearities [14], and non-trivial many-body vacua [13,15], have been theoretically predicted.…”
Section: Introductionmentioning
confidence: 99%