2006
DOI: 10.1088/0953-2048/20/2/s05
|View full text |Cite
|
Sign up to set email alerts
|

Effect of thermal fluctuations on Josephson vortex dynamics in intrinsic Josephson junctions

Abstract: We have made a numerical study of the effect of thermal fluctuations on Josephson vortex dynamics in a stack of intrinsic Josephson junctions. Our simulations successfully reproduced the experimental results such as the field dependence of the critical current, the noise-rounded current–voltage characteristics and a periodic oscillation of the Josephson vortex flow resistance. It was confirmed that the oscillation period of the Josephson vortex flow resistance is related to the modulation of the critical curre… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
5
0

Year Published

2007
2007
2014
2014

Publication Types

Select...
6
1

Relationship

0
7

Authors

Journals

citations
Cited by 8 publications
(5 citation statements)
references
References 22 publications
0
5
0
Order By: Relevance
“…Such behavior of the critical current has been recently reproduced by numerical simulations by Irie and Oya. 21 Experimentally, the crossover between Φ 0 /2-and Φ 0 -periodic oscillations has been observed in the fluxflow voltage by Kakeya et al 15 The crossover field can be arbitrarily defined as a field at which a kΦ 0 -peak in the product ΦJ c drops below the half of a (k + 1/2)Φ 0peak. At larger L the crossover takes place at larger field and larger Φ/Φ 0 but it always occurs at the same ratio h/L, h/L ∼ 1.6.…”
Section: Wide-stack/narrow-stack Crossovermentioning
confidence: 97%
See 1 more Smart Citation
“…Such behavior of the critical current has been recently reproduced by numerical simulations by Irie and Oya. 21 Experimentally, the crossover between Φ 0 /2-and Φ 0 -periodic oscillations has been observed in the fluxflow voltage by Kakeya et al 15 The crossover field can be arbitrarily defined as a field at which a kΦ 0 -peak in the product ΦJ c drops below the half of a (k + 1/2)Φ 0peak. At larger L the crossover takes place at larger field and larger Φ/Φ 0 but it always occurs at the same ratio h/L, h/L ∼ 1.6.…”
Section: Wide-stack/narrow-stack Crossovermentioning
confidence: 97%
“…15,16,17 The crossover in the voltage oscillations also has been studied numerically. 16,21 In the region L ∼ L B the lattice structure is determined by competition between two energies: the interaction with boundaries and the bulk shearing interaction between the Josephson-vortex planar arrays in neighboring layers. The interaction with the boundaries favors the aligned rectangular arrangement of the Josephson vortices while the local shearing interaction favors the triangular lattice.…”
Section: Introductionmentioning
confidence: 99%
“…70. Lattice structures also have been extensively explored numerically 46,48,71,72 and both approaches give identical results. In a small-size sample the lattice structure is determined by two competing interactions: the interaction with boundaries that favors an aligned rectangular configuration and the bulk shearing interaction between neighboring layers which favors a triangular configuration.…”
Section: Lattice Configurations and Magnetic Oscillations In Finite-s...mentioning
confidence: 99%
“…[20][21][22][23][24][25][26][27][28][29][30][31][32][33][34] It is sure that a pioneering work done by Sakai et al 20 is the starting point to understand the fluxon dynamics in BSCCO IJJs with a stacking structure. The is the phase difference of a SIS Josephson junction as a function of spatial variable x and real time t. It is also known that Eq.…”
Section: Introductionmentioning
confidence: 99%