2008
DOI: 10.1063/1.3012360
|View full text |Cite
|
Sign up to set email alerts
|

Fractional order Shapiro steps in superconducting nanowires

Abstract: We expose superconducting nanowires to microwave radiation in order to study phase lock-in effects in quasi-one-dimensional superconductors. For sufficiently high microwave powers a resistive branch with Shapiro steps appears in the voltage-current characteristics. At frequencies in the range of 0.9–4 GHz these steps are of integer order only. At higher frequencies steps of 1/2, 1/3, 1/4, and even 1/6 order appear. We numerically model this behavior using a multivalued current-phase relationship for nanowires.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

3
30
0

Year Published

2012
2012
2021
2021

Publication Types

Select...
6
3
1

Relationship

1
9

Authors

Journals

citations
Cited by 42 publications
(33 citation statements)
references
References 28 publications
(35 reference statements)
3
30
0
Order By: Relevance
“…These observations strongly indicate that the same physics for the transition out of the SCS to the JNS for P < P * and out of the SCS to the PSC for P > P * is involved. The Shapiro steps occur due to synchronization of the superconducting phase difference rotation with the applied high-frequency MW radiation and were discussed in detail in [17]. The steps appear at voltage values given by 2 eV = nh f , as expected, where e is the elementary charge, n is an integer number andh is the Plank constant.…”
Section: Fabrication and Measurementsmentioning
confidence: 56%
“…These observations strongly indicate that the same physics for the transition out of the SCS to the JNS for P < P * and out of the SCS to the PSC for P > P * is involved. The Shapiro steps occur due to synchronization of the superconducting phase difference rotation with the applied high-frequency MW radiation and were discussed in detail in [17]. The steps appear at voltage values given by 2 eV = nh f , as expected, where e is the elementary charge, n is an integer number andh is the Plank constant.…”
Section: Fabrication and Measurementsmentioning
confidence: 56%
“…The model also indicates non-monotonic temperature dependence of the width of the distribution of switching currents. Thus, these experiments with switching events as well as those with microwave radiation in unshunted wires suggest that the resistive state is the normal state of the wire maintained by Joule heating, i.e., the Joule heating normal state (JHNS) 10,11,26,60 . For unshunted wires, the retrapping process is non-stochastic since the retrapping occurs from the thermalized Joule heating state.…”
Section: A Unshunted Nanowiresmentioning
confidence: 99%
“…Due to the great significance of technical applications of phase locking effects, the amplitude and frequency dependence have particularly been a matter of many theoretical and experimental studies in Josephson-junction arrays (JJA), 6 charge density waves (CDW), 7 and superconducting nanowires. 8 In order to gain an insight into physics of these complex macroscopic many-body systems with competing interactions, attention has been always focused on simple many-body models. Among these models, the dissipative (overdamped) Frenkel-Kontorova (FK) model is one of the simplest but still complex a) Author to whom correspondence should be addressed.…”
Section: Introductionmentioning
confidence: 99%