2017
DOI: 10.1016/j.physc.2016.08.001
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The dynamics of magnetic vortices in type II superconductors with pinning sites studied by the time dependent Ginzburg–Landau model

Abstract: We investigate the dynamics of magnetic vortices in type II superconductors with normal state pinning sites using the Ginzburg-Landau equations. Simulation results demonstrate hopping of vortices between pinning sites, influenced by external magnetic fields and external currents. The system is highly nonlinear and the vortices show complex nonlinear dynamical behaviour.

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Cited by 21 publications
(9 citation statements)
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“…On the one hand, fluxons are anchored by the normal cores of the CDs and this pinning potential prevents them for entering the superconducting material in between the CDs. Eventually, they can hop from one CD to a neighboring one [41]. On the other hand, interstitial vortices are pinned by intrinsic defects in the unirradiated parts of the sample.…”
Section: Discussionmentioning
confidence: 99%
“…On the one hand, fluxons are anchored by the normal cores of the CDs and this pinning potential prevents them for entering the superconducting material in between the CDs. Eventually, they can hop from one CD to a neighboring one [41]. On the other hand, interstitial vortices are pinned by intrinsic defects in the unirradiated parts of the sample.…”
Section: Discussionmentioning
confidence: 99%
“…Often real systems have rough surfaces and interior defects that don't match this geometry. There has been considerable effort to simulate vortex nucleation and subsequent dynamics for complicated domains within time-dependent Ginzburg-Landau (TDGL) theory [15][16][17][18][19][20][21][22][23][24]. This paper explores the dynamics of vortex nucleation and extends previous work by calculating H sh in geometries with inhomogeneities.…”
Section: Introductionmentioning
confidence: 91%
“…However, we relax this assumption in order to model spatial variations in T c by allowing α(r) to smoothly vary in space over a range of values. This has been done previously to model pinning sites by setting α(r) to zero at fixed points in the domain [16,[22][23][24]. We define α(r) = α 0 a(r) where α 0 is a reference value (to be subsumed by units), and a(r) is a dimensionless number characterizing the spatial material variation.…”
Section: A Problem Formulationmentioning
confidence: 99%
“…Within this approximation, we can neglect the magnetic field produced by the transport current itself. Therefore, it can be treated as a two-dimensional problem The formalism used to study the system considered in Figure 1(a-b) is given by the time-dependent Ginzburg-Landau (TDGL) equations [17][18][19][20][21][22].…”
Section: Theoretical Formalismmentioning
confidence: 99%