2013
DOI: 10.1103/physrevb.88.104501
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Phase sticking in one-dimensional Josephson junction chains

Abstract: We studied current-voltage characteristics of long one dimensional Josephson junction chains with Josephson energy much larger than charging energy, EJ ≫ EC. In this regime, typical IV curves of the samples consist of a supercurrent branch at low bias voltages followed by a voltage-independent chain current branch, I Chain at high bias. Our experiments showed that I Chain is not only voltageindependent but it is also practically temperature-independent up to TC. We have successfully model the transport propert… Show more

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Cited by 17 publications
(21 citation statements)
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“…Furthermore, in the case of strong charge disorder, depinning effects are the dominant mechanism for the onset of transport above the threshold voltage 4 . In the conducting regime, where the Josephson energy dominates over the charging energy, the current-voltage curve shows a supercurrent-like behavior at low bias voltages and a constant current at higher voltages 5,6 . Another interesting effect is the persistent current that arises if a closed chain is pierced by a magnetic flux [7][8][9] .…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, in the case of strong charge disorder, depinning effects are the dominant mechanism for the onset of transport above the threshold voltage 4 . In the conducting regime, where the Josephson energy dominates over the charging energy, the current-voltage curve shows a supercurrent-like behavior at low bias voltages and a constant current at higher voltages 5,6 . Another interesting effect is the persistent current that arises if a closed chain is pierced by a magnetic flux [7][8][9] .…”
Section: Introductionmentioning
confidence: 99%
“…The series array can emulate an ideal superconducting nanowire when the array is long enough and uniform enough to hide its discrete nature, so that the probability per junction of QPS is relatively small and independent of position in the array. Classical simulations of phase slips in long arrays show that it is also necessary that the junction phase dynamics be overdamped in order for TAPS to occur uniformly along the array [16]. Underdamped dynamics results in persistent phase slips at random nucleation sites, as opposed to random TAPS occurring with equal probability along the array.…”
Section: Introductionmentioning
confidence: 99%
“…An effective speed of light depending on space and/or time can be generated in several 1 + 1 D superconducting circuit setups. In this work we consider a dc-SQUID array embedded in an open transmission line [12,[19][20][21]. The speed of propagation along the transmission line is given by…”
Section: Effective Speed Of Lightmentioning
confidence: 99%