2017
DOI: 10.1088/1367-2630/aa819d
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Nonequilibrium depinning transition of ac driven vortices with random pinning

Abstract: Keywords: vortex pinning, deformation and plasticity, dynamic critical phenomena ac ac,d, all t ( ) f ʼs collapse on a single line with a critical exponent of 1.4, which almost coincides with the value for the dc depinning transition. These results indicate that the critical behavior of the depinning transition is observed not only for the dc drive but also for the ac drive, further demonstrating the universality of the nonequilibrium depinning transition.

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Cited by 12 publications
(9 citation statements)
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References 48 publications
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“…Relaxation times required for the system to settle into the steady state exhibit a power-law divergence at the depinning current with critical exponents 1820 . More recently, using ac drive 21 , we have also observed the critical behavior of the depinning transition with the critical exponent close to that for the dc drive, which is the further demonstration of the universality of the nonequilibrium depinning transition 5 . In these experiments, however, the critical behavior has been observed only on the moving (fluctuating diffusing [active]) side of the transition.…”
Section: Introductionsupporting
confidence: 66%
“…Relaxation times required for the system to settle into the steady state exhibit a power-law divergence at the depinning current with critical exponents 1820 . More recently, using ac drive 21 , we have also observed the critical behavior of the depinning transition with the critical exponent close to that for the dc drive, which is the further demonstration of the universality of the nonequilibrium depinning transition 5 . In these experiments, however, the critical behavior has been observed only on the moving (fluctuating diffusing [active]) side of the transition.…”
Section: Introductionsupporting
confidence: 66%
“…The relaxation time for the system to settle into the moving steady state ( ) exhibits a power-law divergence at the depinning current with critical exponents = 1.4 ± 0.4 9 , 12 , 20 , within error bars, in agreement with the value expected for an absorbing phase transition in the two-dimensional (2D) directed-percolation (DP) universality class 36 38 . Using ac drive 39 , we have also observed the critical behavior of the depinning transition with the critical exponent close to that for the dc drive, further demonstrating the universality of the nonequilibrium depinning transition 5 .…”
Section: Introductionsupporting
confidence: 54%
“…In these experiments, however, the critical behavior of the depinning transition has been observed only on the moving (fluctuating diffusing [active]) side of the transition 9 , 12 , 20 , 39 , although that of RIT has been reported on both sides of the transition 20 , 24 , 26 . This is because it is difficult to obtain a reliable data of V ( t ) in the pinned (non-fluctuating quiescent [absorbing]) phase, where V ( t ) relaxes to = 0.…”
Section: Introductionmentioning
confidence: 99%
“…Driven 2D VLs can be used as simple models for a small portion of the 3D vortex systems studied experimentally, for which history effects in the response have been often observed [20] and signatures of criticality at the depinning transition were reported [3,23]. A prototype of such systems is the vortex matter in clean NbSe 2 single crystals in which the stable vortex phase at low temperatures and weak magnetic fields is an ordered Bragg glass (BG) without VL dislocations [24].…”
mentioning
confidence: 99%